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A Mathematical Study of the Founder Principle of Evolutionary Genetics
Author(s): P. Holgate
Source: Journal of Applied Probability, Vol. 3, No. 1, (Jun., 1966), pp. 115-128
Published by: Applied Probability Trust
Stable URL: http://www.jstor.org/stable/3212041
Accessed: 09/06/2008 07:54
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J. Appl.Prob.3, 115-128(1966)Printed n Israel
J. Appl.Prob.3, 115-128(1966)Printed n Israel
J. Appl.Prob.3, 115-128(1966)Printed n Israel
J. Appl.Prob.3, 115-128(1966)Printed n Israel
J. Appl.Prob.3, 115-128(1966)Printed n Israel
J. Appl.Prob.3, 115-128(1966)Printed n Israel
A MATHEMATICAL STUDY OF THE FOUNDER PRINCIPLE
OF EVOLUTIONARY GENETICS
P. HOLGATE, The Nature Conservancy,London
Smmary
Some comparisons are made between various characteristicsof the geneticstructures of populations of the same size and age, which have (i) evolvedfrom a small founder population, and (ii) evolved from a population whichhas been of constant size throughout the period considered.
1. Introduction
Consider a gene having two alleles A and a. In the absence of selection, and if
there is no mutation, it is possible that one of these will become fixed in a popula-tion as a result of the random fluctuations in its frequency from generation to
generation. This is generally known as the Sewall Wright effect, and its possiblecontribution to evolution has been the subject of considerablediscussion. A sum-
mary of Wright's own views and a survey of his mathematical work on the subjectare given in Wright (1964).
Mathematical work on the tendency to homozygosity of a finite populationhas been surveyed by Moran (1962), and Kimura (1964). Roughly speaking, for
given initial gene frequencies, the probability that the populations will become
homozygous within a given number of generations may be appreciablefor small
populations, but becomes negligible as the population size increases.
Suppose however that a small founder population colonises an area, and inthe course of several generations multiplies to a much greater size. Fixation mayoccur at a given locus when the population is small, and the effect of populationgrowth will then lead to a homozygous population of such a size that fixationas a result of random fluctuation would be inconceivable in a population whichhad always had that same, large size. This phenomenon is known as the founder
principle, associated with Mayr (1942, 1963). Experimentalwork in relation to itis reportedby Dobzhansky and Pavlovsky (1957), and it has recentlybeen invokedin the controversy about the origins of geographical variations between snailcolonies in Southern England, (Goodhart 1962, 1963;Cain and Currey 1963a, b).
Despite its interest, little mathematicalwork has appearedon geneticfluctuations
Receivedin revisedform 6 May 1965.
115
A MATHEMATICAL STUDY OF THE FOUNDER PRINCIPLE
OF EVOLUTIONARY GENETICS
P. HOLGATE, The Nature Conservancy,London
Smmary
Some comparisons are made between various characteristicsof the geneticstructures of populations of the same size and age, which have (i) evolvedfrom a small founder population, and (ii) evolved from a population whichhas been of constant size throughout the period considered.
1. Introduction
Consider a gene having two alleles A and a. In the absence of selection, and if
there is no mutation, it is possible that one of these will become fixed in a popula-tion as a result of the random fluctuations in its frequency from generation to
generation. This is generally known as the Sewall Wright effect, and its possiblecontribution to evolution has been the subject of considerablediscussion. A sum-
mary of Wright's own views and a survey of his mathematical work on the subjectare given in Wright (1964).
Mathematical work on the tendency to homozygosity of a finite populationhas been surveyed by Moran (1962), and Kimura (1964). Roughly speaking, for
given initial gene frequencies, the probability that the populations will become
homozygous within a given number of generations may be appreciablefor small
populations, but becomes negligible as the population size increases.
Suppose however that a small founder population colonises an area, and inthe course of several generations multiplies to a much greater size. Fixation mayoccur at a given locus when the population is small, and the effect of populationgrowth will then lead to a homozygous population of such a size that fixationas a result of random fluctuation would be inconceivable in a population whichhad always had that same, large size. This phenomenon is known as the founder
principle, associated with Mayr (1942, 1963). Experimentalwork in relation to itis reportedby Dobzhansky and Pavlovsky (1957), and it has recentlybeen invokedin the controversy about the origins of geographical variations between snailcolonies in Southern England, (Goodhart 1962, 1963;Cain and Currey 1963a, b).
Despite its interest, little mathematicalwork has appearedon geneticfluctuations
Receivedin revisedform 6 May 1965.
115
A MATHEMATICAL STUDY OF THE FOUNDER PRINCIPLE
OF EVOLUTIONARY GENETICS
P. HOLGATE, The Nature Conservancy,London
Smmary
Some comparisons are made between various characteristicsof the geneticstructures of populations of the same size and age, which have (i) evolvedfrom a small founder population, and (ii) evolved from a population whichhas been of constant size throughout the period considered.
1. Introduction
Consider a gene having two alleles A and a. In the absence of selection, and if
there is no mutation, it is possible that one of these will become fixed in a popula-tion as a result of the random fluctuations in its frequency from generation to
generation. This is generally known as the Sewall Wright effect, and its possiblecontribution to evolution has been the subject of considerablediscussion. A sum-
mary of Wright's own views and a survey of his mathematical work on the subjectare given in Wright (1964).
Mathematical work on the tendency to homozygosity of a finite populationhas been surveyed by Moran (1962), and Kimura (1964). Roughly speaking, for
given initial gene frequencies, the probability that the populations will become
homozygous within a given number of generations may be appreciablefor small
populations, but becomes negligible as the population size increases.
Suppose however that a small founder population colonises an area, and inthe course of several generations multiplies to a much greater size. Fixation mayoccur at a given locus when the population is small, and the effect of populationgrowth will then lead to a homozygous population of such a size that fixationas a result of random fluctuation would be inconceivable in a population whichhad always had that same, large size. This phenomenon is known as the founder
principle, associated with Mayr (1942, 1963). Experimentalwork in relation to itis reportedby Dobzhansky and Pavlovsky (1957), and it has recentlybeen invokedin the controversy about the origins of geographical variations between snailcolonies in Southern England, (Goodhart 1962, 1963;Cain and Currey 1963a, b).
Despite its interest, little mathematicalwork has appearedon geneticfluctuations
Receivedin revisedform 6 May 1965.
115
A MATHEMATICAL STUDY OF THE FOUNDER PRINCIPLE
OF EVOLUTIONARY GENETICS
P. HOLGATE, The Nature Conservancy,London
Smmary
Some comparisons are made between various characteristicsof the geneticstructures of populations of the same size and age, which have (i) evolvedfrom a small founder population, and (ii) evolved from a population whichhas been of constant size throughout the period considered.
1. Introduction
Consider a gene having two alleles A and a. In the absence of selection, and if
there is no mutation, it is possible that one of these will become fixed in a popula-tion as a result of the random fluctuations in its frequency from generation to
generation. This is generally known as the Sewall Wright effect, and its possiblecontribution to evolution has been the subject of considerablediscussion. A sum-
mary of Wright's own views and a survey of his mathematical work on the subjectare given in Wright (1964).
Mathematical work on the tendency to homozygosity of a finite populationhas been surveyed by Moran (1962), and Kimura (1964). Roughly speaking, for
given initial gene frequencies, the probability that the populations will become
homozygous within a given number of generations may be appreciablefor small
populations, but becomes negligible as the population size increases.
Suppose however that a small founder population colonises an area, and inthe course of several generations multiplies to a much greater size. Fixation mayoccur at a given locus when the population is small, and the effect of populationgrowth will then lead to a homozygous population of such a size that fixationas a result of random fluctuation would be inconceivable in a population whichhad always had that same, large size. This phenomenon is known as the founder
principle, associated with Mayr (1942, 1963). Experimentalwork in relation to itis reportedby Dobzhansky and Pavlovsky (1957), and it has recentlybeen invokedin the controversy about the origins of geographical variations between snailcolonies in Southern England, (Goodhart 1962, 1963;Cain and Currey 1963a, b).
Despite its interest, little mathematicalwork has appearedon geneticfluctuations
Receivedin revisedform 6 May 1965.
115
A MATHEMATICAL STUDY OF THE FOUNDER PRINCIPLE
OF EVOLUTIONARY GENETICS
P. HOLGATE, The Nature Conservancy,London
Smmary
Some comparisons are made between various characteristicsof the geneticstructures of populations of the same size and age, which have (i) evolvedfrom a small founder population, and (ii) evolved from a population whichhas been of constant size throughout the period considered.
1. Introduction
Consider a gene having two alleles A and a. In the absence of selection, and if
there is no mutation, it is possible that one of these will become fixed in a popula-tion as a result of the random fluctuations in its frequency from generation to
generation. This is generally known as the Sewall Wright effect, and its possiblecontribution to evolution has been the subject of considerablediscussion. A sum-
mary of Wright's own views and a survey of his mathematical work on the subjectare given in Wright (1964).
Mathematical work on the tendency to homozygosity of a finite populationhas been surveyed by Moran (1962), and Kimura (1964). Roughly speaking, for
given initial gene frequencies, the probability that the populations will become
homozygous within a given number of generations may be appreciablefor small
populations, but becomes negligible as the population size increases.
Suppose however that a small founder population colonises an area, and inthe course of several generations multiplies to a much greater size. Fixation mayoccur at a given locus when the population is small, and the effect of populationgrowth will then lead to a homozygous population of such a size that fixationas a result of random fluctuation would be inconceivable in a population whichhad always had that same, large size. This phenomenon is known as the founder
principle, associated with Mayr (1942, 1963). Experimentalwork in relation to itis reportedby Dobzhansky and Pavlovsky (1957), and it has recentlybeen invokedin the controversy about the origins of geographical variations between snailcolonies in Southern England, (Goodhart 1962, 1963;Cain and Currey 1963a, b).
Despite its interest, little mathematicalwork has appearedon geneticfluctuations
Receivedin revisedform 6 May 1965.
115
A MATHEMATICAL STUDY OF THE FOUNDER PRINCIPLE
OF EVOLUTIONARY GENETICS
P. HOLGATE, The Nature Conservancy,London
Smmary
Some comparisons are made between various characteristicsof the geneticstructures of populations of the same size and age, which have (i) evolvedfrom a small founder population, and (ii) evolved from a population whichhas been of constant size throughout the period considered.
1. Introduction
Consider a gene having two alleles A and a. In the absence of selection, and if
there is no mutation, it is possible that one of these will become fixed in a popula-tion as a result of the random fluctuations in its frequency from generation to
generation. This is generally known as the Sewall Wright effect, and its possiblecontribution to evolution has been the subject of considerablediscussion. A sum-
mary of Wright's own views and a survey of his mathematical work on the subjectare given in Wright (1964).
Mathematical work on the tendency to homozygosity of a finite populationhas been surveyed by Moran (1962), and Kimura (1964). Roughly speaking, for
given initial gene frequencies, the probability that the populations will become
homozygous within a given number of generations may be appreciablefor small
populations, but becomes negligible as the population size increases.
Suppose however that a small founder population colonises an area, and inthe course of several generations multiplies to a much greater size. Fixation mayoccur at a given locus when the population is small, and the effect of populationgrowth will then lead to a homozygous population of such a size that fixationas a result of random fluctuation would be inconceivable in a population whichhad always had that same, large size. This phenomenon is known as the founder
principle, associated with Mayr (1942, 1963). Experimentalwork in relation to itis reportedby Dobzhansky and Pavlovsky (1957), and it has recentlybeen invokedin the controversy about the origins of geographical variations between snailcolonies in Southern England, (Goodhart 1962, 1963;Cain and Currey 1963a, b).
Despite its interest, little mathematicalwork has appearedon geneticfluctuations
Receivedin revisedform 6 May 1965.
115
8/8/2019 A Mathematical Study of the Founder Principle
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A mathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary enetics
this question for the growing population. If Zt is the number of heterozygotes
in Ft then{Zo
= 1, Z1, Z2, "*-} is a branching stochastic process of Galton-
Watson type. (For the theory of these processes see Bartlett (1960), Harris(1963)).
The probability generating function of the number of heterozygous offspring
of a heterozygote is
(1) f(s)=(2+f s).
Since the mean of the distribution given by (1) is 1, the ultimate elimination of
heterozygotes is certain. The p.g.f. of Zt is obtained by functional iteration which
may be carried out explicitly for small t. For instance, the probability that F3
will contain j heterozygotes is the coefficient of sJ in
(2) f3(s)= 2( 2(s+2 + 2 +2 '
This distribution is tabulated in the first column of Table I.
The elimination of heterozygotes in a population where each individual con-
tributed a single offspringto the next generation was discussed by Bartlett(1937).
Suppose, for comparison with the above case, that a population had been initiated
by 8 heterozygotes,and had undergone 3 generations of selfing,with each individ-
ual contributing a single offspring to the next generation. The probability that a
given line would remain heterozygous is 1/8, and the p.g.f of the number ofheterozygotes in F3 is therefore
(3) g3(s) = ( 1 + 7)8
This binomial distribution is tabulated in the second column of Table I.
TABLE
Distribution of number of heterozygotes
after three generations of selfing
ProbabilityGrowing Stationary
Population Population
0 .483459 .343609J
1 .217285 .392696
2 .176514 .196348
3 .077637 .056099
4 .032593 .010018
5 .009277 .001145
6 .002686 .000082
7 .000488 .0000038 .000061 .000000
this question for the growing population. If Zt is the number of heterozygotes
in Ft then{Zo
= 1, Z1, Z2, "*-} is a branching stochastic process of Galton-
Watson type. (For the theory of these processes see Bartlett (1960), Harris(1963)).
The probability generating function of the number of heterozygous offspring
of a heterozygote is
(1) f(s)=(2+f s).
Since the mean of the distribution given by (1) is 1, the ultimate elimination of
heterozygotes is certain. The p.g.f. of Zt is obtained by functional iteration which
may be carried out explicitly for small t. For instance, the probability that F3
will contain j heterozygotes is the coefficient of sJ in
(2) f3(s)= 2( 2(s+2 + 2 +2 '
This distribution is tabulated in the first column of Table I.
The elimination of heterozygotes in a population where each individual con-
tributed a single offspringto the next generation was discussed by Bartlett(1937).
Suppose, for comparison with the above case, that a population had been initiated
by 8 heterozygotes,and had undergone 3 generations of selfing,with each individ-
ual contributing a single offspring to the next generation. The probability that a
given line would remain heterozygous is 1/8, and the p.g.f of the number ofheterozygotes in F3 is therefore
(3) g3(s) = ( 1 + 7)8
This binomial distribution is tabulated in the second column of Table I.
TABLE
Distribution of number of heterozygotes
after three generations of selfing
ProbabilityGrowing Stationary
Population Population
0 .483459 .343609J
1 .217285 .392696
2 .176514 .196348
3 .077637 .056099
4 .032593 .010018
5 .009277 .001145
6 .002686 .000082
7 .000488 .0000038 .000061 .000000
this question for the growing population. If Zt is the number of heterozygotes
in Ft then{Zo
= 1, Z1, Z2, "*-} is a branching stochastic process of Galton-
Watson type. (For the theory of these processes see Bartlett (1960), Harris(1963)).
The probability generating function of the number of heterozygous offspring
of a heterozygote is
(1) f(s)=(2+f s).
Since the mean of the distribution given by (1) is 1, the ultimate elimination of
heterozygotes is certain. The p.g.f. of Zt is obtained by functional iteration which
may be carried out explicitly for small t. For instance, the probability that F3
will contain j heterozygotes is the coefficient of sJ in
(2) f3(s)= 2( 2(s+2 + 2 +2 '
This distribution is tabulated in the first column of Table I.
The elimination of heterozygotes in a population where each individual con-
tributed a single offspringto the next generation was discussed by Bartlett(1937).
Suppose, for comparison with the above case, that a population had been initiated
by 8 heterozygotes,and had undergone 3 generations of selfing,with each individ-
ual contributing a single offspring to the next generation. The probability that a
given line would remain heterozygous is 1/8, and the p.g.f of the number ofheterozygotes in F3 is therefore
(3) g3(s) = ( 1 + 7)8
This binomial distribution is tabulated in the second column of Table I.
TABLE
Distribution of number of heterozygotes
after three generations of selfing
ProbabilityGrowing Stationary
Population Population
0 .483459 .343609J
1 .217285 .392696
2 .176514 .196348
3 .077637 .056099
4 .032593 .010018
5 .009277 .001145
6 .002686 .000082
7 .000488 .0000038 .000061 .000000
this question for the growing population. If Zt is the number of heterozygotes
in Ft then{Zo
= 1, Z1, Z2, "*-} is a branching stochastic process of Galton-
Watson type. (For the theory of these processes see Bartlett (1960), Harris(1963)).
The probability generating function of the number of heterozygous offspring
of a heterozygote is
(1) f(s)=(2+f s).
Since the mean of the distribution given by (1) is 1, the ultimate elimination of
heterozygotes is certain. The p.g.f. of Zt is obtained by functional iteration which
may be carried out explicitly for small t. For instance, the probability that F3
will contain j heterozygotes is the coefficient of sJ in
(2) f3(s)= 2( 2(s+2 + 2 +2 '
This distribution is tabulated in the first column of Table I.
The elimination of heterozygotes in a population where each individual con-
tributed a single offspringto the next generation was discussed by Bartlett(1937).
Suppose, for comparison with the above case, that a population had been initiated
by 8 heterozygotes,and had undergone 3 generations of selfing,with each individ-
ual contributing a single offspring to the next generation. The probability that a
given line would remain heterozygous is 1/8, and the p.g.f of the number ofheterozygotes in F3 is therefore
(3) g3(s) = ( 1 + 7)8
This binomial distribution is tabulated in the second column of Table I.
TABLE
Distribution of number of heterozygotes
after three generations of selfing
ProbabilityGrowing Stationary
Population Population
0 .483459 .343609J
1 .217285 .392696
2 .176514 .196348
3 .077637 .056099
4 .032593 .010018
5 .009277 .001145
6 .002686 .000082
7 .000488 .0000038 .000061 .000000
this question for the growing population. If Zt is the number of heterozygotes
in Ft then{Zo
= 1, Z1, Z2, "*-} is a branching stochastic process of Galton-
Watson type. (For the theory of these processes see Bartlett (1960), Harris(1963)).
The probability generating function of the number of heterozygous offspring
of a heterozygote is
(1) f(s)=(2+f s).
Since the mean of the distribution given by (1) is 1, the ultimate elimination of
heterozygotes is certain. The p.g.f. of Zt is obtained by functional iteration which
may be carried out explicitly for small t. For instance, the probability that F3
will contain j heterozygotes is the coefficient of sJ in
(2) f3(s)= 2( 2(s+2 + 2 +2 '
This distribution is tabulated in the first column of Table I.
The elimination of heterozygotes in a population where each individual con-
tributed a single offspringto the next generation was discussed by Bartlett(1937).
Suppose, for comparison with the above case, that a population had been initiated
by 8 heterozygotes,and had undergone 3 generations of selfing,with each individ-
ual contributing a single offspring to the next generation. The probability that a
given line would remain heterozygous is 1/8, and the p.g.f of the number ofheterozygotes in F3 is therefore
(3) g3(s) = ( 1 + 7)8
This binomial distribution is tabulated in the second column of Table I.
TABLE
Distribution of number of heterozygotes
after three generations of selfing
ProbabilityGrowing Stationary
Population Population
0 .483459 .343609J
1 .217285 .392696
2 .176514 .196348
3 .077637 .056099
4 .032593 .010018
5 .009277 .001145
6 .002686 .000082
7 .000488 .0000038 .000061 .000000
this question for the growing population. If Zt is the number of heterozygotes
in Ft then{Zo
= 1, Z1, Z2, "*-} is a branching stochastic process of Galton-
Watson type. (For the theory of these processes see Bartlett (1960), Harris(1963)).
The probability generating function of the number of heterozygous offspring
of a heterozygote is
(1) f(s)=(2+f s).
Since the mean of the distribution given by (1) is 1, the ultimate elimination of
heterozygotes is certain. The p.g.f. of Zt is obtained by functional iteration which
may be carried out explicitly for small t. For instance, the probability that F3
will contain j heterozygotes is the coefficient of sJ in
(2) f3(s)= 2( 2(s+2 + 2 +2 '
This distribution is tabulated in the first column of Table I.
The elimination of heterozygotes in a population where each individual con-
tributed a single offspringto the next generation was discussed by Bartlett(1937).
Suppose, for comparison with the above case, that a population had been initiated
by 8 heterozygotes,and had undergone 3 generations of selfing,with each individ-
ual contributing a single offspring to the next generation. The probability that a
given line would remain heterozygous is 1/8, and the p.g.f of the number ofheterozygotes in F3 is therefore
(3) g3(s) = ( 1 + 7)8
This binomial distribution is tabulated in the second column of Table I.
TABLE
Distribution of number of heterozygotes
after three generations of selfing
ProbabilityGrowing Stationary
Population Population
0 .483459 .343609J
1 .217285 .392696
2 .176514 .196348
3 .077637 .056099
4 .032593 .010018
5 .009277 .001145
6 .002686 .000082
7 .000488 .0000038 .000061 .000000
1171717171717
8/8/2019 A Mathematical Study of the Founder Principle
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Despitethe smallnumberof generations,TableI illustrateshefactthat boththe
probabilityof completeelimination of heterozygotes,and the probability hattheir numberwill be large,aregreateror thegrowing population.The variancesare1.5 for the growingpopulationand0.875 for the stationary ne.
Thevarianceof Z, forgeneral maybe obtainedby letting -2 inFormula7a)in Bartlett 1937),or by substitutingor a2 inFormula 5.3)inHarris 1963,p. 6),eitherof which ead to:
(4) Zt 1, varZ,= t.
The probabilityhat therewould be no heterozygotes fter t generationss given
by the asymptotic ormulaof Kolmogorov 1938)as
(5) Pr(Z, =0) 1- 2 I 4- 1tf(1) t
In fact, the p.g.f. (1) and result 5)arementionedby Kolmogorovas an exampleat the end of Section4 of his paper,where heyarise n the solutionof adifferent
problemn populationgenetics. t maybe notedthat t has to be quite arge or(5)to give good numericalresults.For t = 40 when (5) gives 0.9, the correct alueobtainedbyiterations 0.9142.However hederivation ivenbyHarris1963,p. 20
ff.)suggests /(4+ t) as a betterapproximation, ndfor t = 40 it gives0.9091.For
comparisonconsider an Ft which had arisenfrom an Fo of 2t heterozygotes,evolving throught t generationsof selfingatconstant population size, and letZt be the numberof heterozygotesn Ft in this population. It shouldbe bornein mind that the sequence{Z'},althougha stochasticprocess n themathematical
sense,does not represent he evolutionof a definitepopulation.)By reasoningsimilar to that given in the case t = 3, the distributionof Zt is binomial withn = 2t, p = (1/2)t, and hence
(6) Z;=l1, varZt'=(1- ())
(7) Pr(Zf=0)== (1-( ) e- =0.367879.
Comparison f thevariances iven n (4)and(6), and theprobabilitieshat hetero-
zygoteswill be absent,given in (5) and (7), togetherwith the numericalresultsof TableI, illustrate he fact that selfingpopulationswhichhavereacheda largesize by repeateddoubling will be more variable in respectto proportionsof
heterozygotes, nd in particularwill be morelikelyto containnone, thanthose
Despitethe smallnumberof generations,TableI illustrateshefactthat boththe
probabilityof completeelimination of heterozygotes,and the probability hattheir numberwill be large,aregreateror thegrowing population.The variancesare1.5 for the growingpopulationand0.875 for the stationary ne.
Thevarianceof Z, forgeneral maybe obtainedby letting -2 inFormula7a)in Bartlett 1937),or by substitutingor a2 inFormula 5.3)inHarris 1963,p. 6),eitherof which ead to:
(4) Zt 1, varZ,= t.
The probabilityhat therewould be no heterozygotes fter t generationss given
by the asymptotic ormulaof Kolmogorov 1938)as
(5) Pr(Z, =0) 1- 2 I 4- 1tf(1) t
In fact, the p.g.f. (1) and result 5)arementionedby Kolmogorovas an exampleat the end of Section4 of his paper,where heyarise n the solutionof adifferent
problemn populationgenetics. t maybe notedthat t has to be quite arge or(5)to give good numericalresults.For t = 40 when (5) gives 0.9, the correct alueobtainedbyiterations 0.9142.However hederivation ivenbyHarris1963,p. 20
ff.)suggests /(4+ t) as a betterapproximation, ndfor t = 40 it gives0.9091.For
comparisonconsider an Ft which had arisenfrom an Fo of 2t heterozygotes,evolving throught t generationsof selfingatconstant population size, and letZt be the numberof heterozygotesn Ft in this population. It shouldbe bornein mind that the sequence{Z'},althougha stochasticprocess n themathematical
sense,does not represent he evolutionof a definitepopulation.)By reasoningsimilar to that given in the case t = 3, the distributionof Zt is binomial withn = 2t, p = (1/2)t, and hence
(6) Z;=l1, varZt'=(1- ())
(7) Pr(Zf=0)== (1-( ) e- =0.367879.
Comparison f thevariances iven n (4)and(6), and theprobabilitieshat hetero-
zygoteswill be absent,given in (5) and (7), togetherwith the numericalresultsof TableI, illustrate he fact that selfingpopulationswhichhavereacheda largesize by repeateddoubling will be more variable in respectto proportionsof
heterozygotes, nd in particularwill be morelikelyto containnone, thanthose
Despitethe smallnumberof generations,TableI illustrateshefactthat boththe
probabilityof completeelimination of heterozygotes,and the probability hattheir numberwill be large,aregreateror thegrowing population.The variancesare1.5 for the growingpopulationand0.875 for the stationary ne.
Thevarianceof Z, forgeneral maybe obtainedby letting -2 inFormula7a)in Bartlett 1937),or by substitutingor a2 inFormula 5.3)inHarris 1963,p. 6),eitherof which ead to:
(4) Zt 1, varZ,= t.
The probabilityhat therewould be no heterozygotes fter t generationss given
by the asymptotic ormulaof Kolmogorov 1938)as
(5) Pr(Z, =0) 1- 2 I 4- 1tf(1) t
In fact, the p.g.f. (1) and result 5)arementionedby Kolmogorovas an exampleat the end of Section4 of his paper,where heyarise n the solutionof adifferent
problemn populationgenetics. t maybe notedthat t has to be quite arge or(5)to give good numericalresults.For t = 40 when (5) gives 0.9, the correct alueobtainedbyiterations 0.9142.However hederivation ivenbyHarris1963,p. 20
ff.)suggests /(4+ t) as a betterapproximation, ndfor t = 40 it gives0.9091.For
comparisonconsider an Ft which had arisenfrom an Fo of 2t heterozygotes,evolving throught t generationsof selfingatconstant population size, and letZt be the numberof heterozygotesn Ft in this population. It shouldbe bornein mind that the sequence{Z'},althougha stochasticprocess n themathematical
sense,does not represent he evolutionof a definitepopulation.)By reasoningsimilar to that given in the case t = 3, the distributionof Zt is binomial withn = 2t, p = (1/2)t, and hence
(6) Z;=l1, varZt'=(1- ())
(7) Pr(Zf=0)== (1-( ) e- =0.367879.
Comparison f thevariances iven n (4)and(6), and theprobabilitieshat hetero-
zygoteswill be absent,given in (5) and (7), togetherwith the numericalresultsof TableI, illustrate he fact that selfingpopulationswhichhavereacheda largesize by repeateddoubling will be more variable in respectto proportionsof
heterozygotes, nd in particularwill be morelikelyto containnone, thanthose
Despitethe smallnumberof generations,TableI illustrateshefactthat boththe
probabilityof completeelimination of heterozygotes,and the probability hattheir numberwill be large,aregreateror thegrowing population.The variancesare1.5 for the growingpopulationand0.875 for the stationary ne.
Thevarianceof Z, forgeneral maybe obtainedby letting -2 inFormula7a)in Bartlett 1937),or by substitutingor a2 inFormula 5.3)inHarris 1963,p. 6),eitherof which ead to:
(4) Zt 1, varZ,= t.
The probabilityhat therewould be no heterozygotes fter t generationss given
by the asymptotic ormulaof Kolmogorov 1938)as
(5) Pr(Z, =0) 1- 2 I 4- 1tf(1) t
In fact, the p.g.f. (1) and result 5)arementionedby Kolmogorovas an exampleat the end of Section4 of his paper,where heyarise n the solutionof adifferent
problemn populationgenetics. t maybe notedthat t has to be quite arge or(5)to give good numericalresults.For t = 40 when (5) gives 0.9, the correct alueobtainedbyiterations 0.9142.However hederivation ivenbyHarris1963,p. 20
ff.)suggests /(4+ t) as a betterapproximation, ndfor t = 40 it gives0.9091.For
comparisonconsider an Ft which had arisenfrom an Fo of 2t heterozygotes,evolving throught t generationsof selfingatconstant population size, and letZt be the numberof heterozygotesn Ft in this population. It shouldbe bornein mind that the sequence{Z'},althougha stochasticprocess n themathematical
sense,does not represent he evolutionof a definitepopulation.)By reasoningsimilar to that given in the case t = 3, the distributionof Zt is binomial withn = 2t, p = (1/2)t, and hence
(6) Z;=l1, varZt'=(1- ())
(7) Pr(Zf=0)== (1-( ) e- =0.367879.
Comparison f thevariances iven n (4)and(6), and theprobabilitieshat hetero-
zygoteswill be absent,given in (5) and (7), togetherwith the numericalresultsof TableI, illustrate he fact that selfingpopulationswhichhavereacheda largesize by repeateddoubling will be more variable in respectto proportionsof
heterozygotes, nd in particularwill be morelikelyto containnone, thanthose
Despitethe smallnumberof generations,TableI illustrateshefactthat boththe
probabilityof completeelimination of heterozygotes,and the probability hattheir numberwill be large,aregreateror thegrowing population.The variancesare1.5 for the growingpopulationand0.875 for the stationary ne.
Thevarianceof Z, forgeneral maybe obtainedby letting -2 inFormula7a)in Bartlett 1937),or by substitutingor a2 inFormula 5.3)inHarris 1963,p. 6),eitherof which ead to:
(4) Zt 1, varZ,= t.
The probabilityhat therewould be no heterozygotes fter t generationss given
by the asymptotic ormulaof Kolmogorov 1938)as
(5) Pr(Z, =0) 1- 2 I 4- 1tf(1) t
In fact, the p.g.f. (1) and result 5)arementionedby Kolmogorovas an exampleat the end of Section4 of his paper,where heyarise n the solutionof adifferent
problemn populationgenetics. t maybe notedthat t has to be quite arge or(5)to give good numericalresults.For t = 40 when (5) gives 0.9, the correct alueobtainedbyiterations 0.9142.However hederivation ivenbyHarris1963,p. 20
ff.)suggests /(4+ t) as a betterapproximation, ndfor t = 40 it gives0.9091.For
comparisonconsider an Ft which had arisenfrom an Fo of 2t heterozygotes,evolving throught t generationsof selfingatconstant population size, and letZt be the numberof heterozygotesn Ft in this population. It shouldbe bornein mind that the sequence{Z'},althougha stochasticprocess n themathematical
sense,does not represent he evolutionof a definitepopulation.)By reasoningsimilar to that given in the case t = 3, the distributionof Zt is binomial withn = 2t, p = (1/2)t, and hence
(6) Z;=l1, varZt'=(1- ())
(7) Pr(Zf=0)== (1-( ) e- =0.367879.
Comparison f thevariances iven n (4)and(6), and theprobabilitieshat hetero-
zygoteswill be absent,given in (5) and (7), togetherwith the numericalresultsof TableI, illustrate he fact that selfingpopulationswhichhavereacheda largesize by repeateddoubling will be more variable in respectto proportionsof
heterozygotes, nd in particularwill be morelikelyto containnone, thanthose
Despitethe smallnumberof generations,TableI illustrateshefactthat boththe
probabilityof completeelimination of heterozygotes,and the probability hattheir numberwill be large,aregreateror thegrowing population.The variancesare1.5 for the growingpopulationand0.875 for the stationary ne.
Thevarianceof Z, forgeneral maybe obtainedby letting -2 inFormula7a)in Bartlett 1937),or by substitutingor a2 inFormula 5.3)inHarris 1963,p. 6),eitherof which ead to:
(4) Zt 1, varZ,= t.
The probabilityhat therewould be no heterozygotes fter t generationss given
by the asymptotic ormulaof Kolmogorov 1938)as
(5) Pr(Z, =0) 1- 2 I 4- 1tf(1) t
In fact, the p.g.f. (1) and result 5)arementionedby Kolmogorovas an exampleat the end of Section4 of his paper,where heyarise n the solutionof adifferent
problemn populationgenetics. t maybe notedthat t has to be quite arge or(5)to give good numericalresults.For t = 40 when (5) gives 0.9, the correct alueobtainedbyiterations 0.9142.However hederivation ivenbyHarris1963,p. 20
ff.)suggests /(4+ t) as a betterapproximation, ndfor t = 40 it gives0.9091.For
comparisonconsider an Ft which had arisenfrom an Fo of 2t heterozygotes,evolving throught t generationsof selfingatconstant population size, and letZt be the numberof heterozygotesn Ft in this population. It shouldbe bornein mind that the sequence{Z'},althougha stochasticprocess n themathematical
sense,does not represent he evolutionof a definitepopulation.)By reasoningsimilar to that given in the case t = 3, the distributionof Zt is binomial withn = 2t, p = (1/2)t, and hence
(6) Z;=l1, varZt'=(1- ())
(7) Pr(Zf=0)== (1-( ) e- =0.367879.
Comparison f thevariances iven n (4)and(6), and theprobabilitieshat hetero-
zygoteswill be absent,given in (5) and (7), togetherwith the numericalresultsof TableI, illustrate he fact that selfingpopulationswhichhavereacheda largesize by repeateddoubling will be more variable in respectto proportionsof
heterozygotes, nd in particularwill be morelikelyto containnone, thanthose
1181818181818 P. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE
8/8/2019 A Mathematical Study of the Founder Principle
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A mathematicaltudyof the ounderrinciple f evolutionaryeneticsmathematicaltudyof the ounderrinciple f evolutionaryeneticsmathematicaltudyof the ounderrinciple f evolutionaryeneticsmathematicaltudyof the ounderrinciple f evolutionaryeneticsmathematicaltudyof the ounderrinciple f evolutionaryeneticsmathematicaltudyof the ounderrinciple f evolutionaryenetics
of the same size and age that have always been that size. The stochastic process
describing the number of individuals in Ft which are homozygous for a given
allele, say A, is not a branching process, nor even a Markov process. However,
the probability P, that Ft will consist entirely of AA's, has a simple recurrence
relation. The probabilities that the offspring of a heterozygote are (AA,AA),
(AA,Aa) or (Aa,Aa) are 1/16,1/4,1/4 respectively. It is then required that the
offspring should consist entirely of AA's after (t- 1) generations, which leads to
11 1 2Pt = + Pt-1 + Pt2-1
from which P3 = 0.083840. Since the Pt are obviously increasing, lim0 Pt = P,
the probability that the population ultimately consists entirely of AA's satisfies
11 1 1 2P=- +-p +P2
16 4 4
of which the relevant root is P = 1 1/2 - V2 = 0.085786. For the comparable
stationary population the chance that all its members are AA is given by
(1/4 + 1/2 *1/4 + 1/2 *1/2 *1/4)8 = 0.001342.
In the doubling population the elimination of heterozygotes occurs with
probability one. When it has occurred the population which will then consist
entirely of AA's and aa's will continue to increase, but with the numbersof these
types, and hence of the two alleles, in a constant proportion. The remainderof this section is devoted to obtaining some propertiesof Y,the randomproportion
of AA's when the heterozygotes have been eliminated. Clearly, Y can take only
those values whose expression as a binary fraction can be written in terminating
form, and every such value in the interval [0,1] is taken with positive probability.
It is therefore an example of a random variable whose distributionfunction has
jumps at a set of points everywheredense (in [0,1]), although this peculiarity is a
mathematicalconsequence of insisting on the population doubling exactly at each
generation. If Ytis the proportion of the limiting population belonging to lines
which became AA at exactly the tth generation, then Y = t 1 Yt. t is interesting
to note that the stochastic process
2Yt, j=1,2,-.,t= I
is such that almost every realisation is monotonically increasing, the form of the
'remainder' term in the submartingale decomposition theorem (Loeve, 1963,
p. 389). Some properties of Y may be obtained by enumerating the possible
structures of F1, and equating the unconditional expectations of certain variables,
to the appropriate expectations obtained after conditioning by the outcome of F1.
The possible F1 's are listed in column 2 of TableII,preceded by their probabilities.
of the same size and age that have always been that size. The stochastic process
describing the number of individuals in Ft which are homozygous for a given
allele, say A, is not a branching process, nor even a Markov process. However,
the probability P, that Ft will consist entirely of AA's, has a simple recurrence
relation. The probabilities that the offspring of a heterozygote are (AA,AA),
(AA,Aa) or (Aa,Aa) are 1/16,1/4,1/4 respectively. It is then required that the
offspring should consist entirely of AA's after (t- 1) generations, which leads to
11 1 2Pt = + Pt-1 + Pt2-1
from which P3 = 0.083840. Since the Pt are obviously increasing, lim0 Pt = P,
the probability that the population ultimately consists entirely of AA's satisfies
11 1 1 2P=- +-p +P2
16 4 4
of which the relevant root is P = 1 1/2 - V2 = 0.085786. For the comparable
stationary population the chance that all its members are AA is given by
(1/4 + 1/2 *1/4 + 1/2 *1/2 *1/4)8 = 0.001342.
In the doubling population the elimination of heterozygotes occurs with
probability one. When it has occurred the population which will then consist
entirely of AA's and aa's will continue to increase, but with the numbersof these
types, and hence of the two alleles, in a constant proportion. The remainderof this section is devoted to obtaining some propertiesof Y,the randomproportion
of AA's when the heterozygotes have been eliminated. Clearly, Y can take only
those values whose expression as a binary fraction can be written in terminating
form, and every such value in the interval [0,1] is taken with positive probability.
It is therefore an example of a random variable whose distributionfunction has
jumps at a set of points everywheredense (in [0,1]), although this peculiarity is a
mathematicalconsequence of insisting on the population doubling exactly at each
generation. If Ytis the proportion of the limiting population belonging to lines
which became AA at exactly the tth generation, then Y = t 1 Yt. t is interesting
to note that the stochastic process
2Yt, j=1,2,-.,t= I
is such that almost every realisation is monotonically increasing, the form of the
'remainder' term in the submartingale decomposition theorem (Loeve, 1963,
p. 389). Some properties of Y may be obtained by enumerating the possible
structures of F1, and equating the unconditional expectations of certain variables,
to the appropriate expectations obtained after conditioning by the outcome of F1.
The possible F1 's are listed in column 2 of TableII,preceded by their probabilities.
of the same size and age that have always been that size. The stochastic process
describing the number of individuals in Ft which are homozygous for a given
allele, say A, is not a branching process, nor even a Markov process. However,
the probability P, that Ft will consist entirely of AA's, has a simple recurrence
relation. The probabilities that the offspring of a heterozygote are (AA,AA),
(AA,Aa) or (Aa,Aa) are 1/16,1/4,1/4 respectively. It is then required that the
offspring should consist entirely of AA's after (t- 1) generations, which leads to
11 1 2Pt = + Pt-1 + Pt2-1
from which P3 = 0.083840. Since the Pt are obviously increasing, lim0 Pt = P,
the probability that the population ultimately consists entirely of AA's satisfies
11 1 1 2P=- +-p +P2
16 4 4
of which the relevant root is P = 1 1/2 - V2 = 0.085786. For the comparable
stationary population the chance that all its members are AA is given by
(1/4 + 1/2 *1/4 + 1/2 *1/2 *1/4)8 = 0.001342.
In the doubling population the elimination of heterozygotes occurs with
probability one. When it has occurred the population which will then consist
entirely of AA's and aa's will continue to increase, but with the numbersof these
types, and hence of the two alleles, in a constant proportion. The remainderof this section is devoted to obtaining some propertiesof Y,the randomproportion
of AA's when the heterozygotes have been eliminated. Clearly, Y can take only
those values whose expression as a binary fraction can be written in terminating
form, and every such value in the interval [0,1] is taken with positive probability.
It is therefore an example of a random variable whose distributionfunction has
jumps at a set of points everywheredense (in [0,1]), although this peculiarity is a
mathematicalconsequence of insisting on the population doubling exactly at each
generation. If Ytis the proportion of the limiting population belonging to lines
which became AA at exactly the tth generation, then Y = t 1 Yt. t is interesting
to note that the stochastic process
2Yt, j=1,2,-.,t= I
is such that almost every realisation is monotonically increasing, the form of the
'remainder' term in the submartingale decomposition theorem (Loeve, 1963,
p. 389). Some properties of Y may be obtained by enumerating the possible
structures of F1, and equating the unconditional expectations of certain variables,
to the appropriate expectations obtained after conditioning by the outcome of F1.
The possible F1 's are listed in column 2 of TableII,preceded by their probabilities.
of the same size and age that have always been that size. The stochastic process
describing the number of individuals in Ft which are homozygous for a given
allele, say A, is not a branching process, nor even a Markov process. However,
the probability P, that Ft will consist entirely of AA's, has a simple recurrence
relation. The probabilities that the offspring of a heterozygote are (AA,AA),
(AA,Aa) or (Aa,Aa) are 1/16,1/4,1/4 respectively. It is then required that the
offspring should consist entirely of AA's after (t- 1) generations, which leads to
11 1 2Pt = + Pt-1 + Pt2-1
from which P3 = 0.083840. Since the Pt are obviously increasing, lim0 Pt = P,
the probability that the population ultimately consists entirely of AA's satisfies
11 1 1 2P=- +-p +P2
16 4 4
of which the relevant root is P = 1 1/2 - V2 = 0.085786. For the comparable
stationary population the chance that all its members are AA is given by
(1/4 + 1/2 *1/4 + 1/2 *1/2 *1/4)8 = 0.001342.
In the doubling population the elimination of heterozygotes occurs with
probability one. When it has occurred the population which will then consist
entirely of AA's and aa's will continue to increase, but with the numbersof these
types, and hence of the two alleles, in a constant proportion. The remainderof this section is devoted to obtaining some propertiesof Y,the randomproportion
of AA's when the heterozygotes have been eliminated. Clearly, Y can take only
those values whose expression as a binary fraction can be written in terminating
form, and every such value in the interval [0,1] is taken with positive probability.
It is therefore an example of a random variable whose distributionfunction has
jumps at a set of points everywheredense (in [0,1]), although this peculiarity is a
mathematicalconsequence of insisting on the population doubling exactly at each
generation. If Ytis the proportion of the limiting population belonging to lines
which became AA at exactly the tth generation, then Y = t 1 Yt. t is interesting
to note that the stochastic process
2Yt, j=1,2,-.,t= I
is such that almost every realisation is monotonically increasing, the form of the
'remainder' term in the submartingale decomposition theorem (Loeve, 1963,
p. 389). Some properties of Y may be obtained by enumerating the possible
structures of F1, and equating the unconditional expectations of certain variables,
to the appropriate expectations obtained after conditioning by the outcome of F1.
The possible F1 's are listed in column 2 of TableII,preceded by their probabilities.
of the same size and age that have always been that size. The stochastic process
describing the number of individuals in Ft which are homozygous for a given
allele, say A, is not a branching process, nor even a Markov process. However,
the probability P, that Ft will consist entirely of AA's, has a simple recurrence
relation. The probabilities that the offspring of a heterozygote are (AA,AA),
(AA,Aa) or (Aa,Aa) are 1/16,1/4,1/4 respectively. It is then required that the
offspring should consist entirely of AA's after (t- 1) generations, which leads to
11 1 2Pt = + Pt-1 + Pt2-1
from which P3 = 0.083840. Since the Pt are obviously increasing, lim0 Pt = P,
the probability that the population ultimately consists entirely of AA's satisfies
11 1 1 2P=- +-p +P2
16 4 4
of which the relevant root is P = 1 1/2 - V2 = 0.085786. For the comparable
stationary population the chance that all its members are AA is given by
(1/4 + 1/2 *1/4 + 1/2 *1/2 *1/4)8 = 0.001342.
In the doubling population the elimination of heterozygotes occurs with
probability one. When it has occurred the population which will then consist
entirely of AA's and aa's will continue to increase, but with the numbersof these
types, and hence of the two alleles, in a constant proportion. The remainderof this section is devoted to obtaining some propertiesof Y,the randomproportion
of AA's when the heterozygotes have been eliminated. Clearly, Y can take only
those values whose expression as a binary fraction can be written in terminating
form, and every such value in the interval [0,1] is taken with positive probability.
It is therefore an example of a random variable whose distributionfunction has
jumps at a set of points everywheredense (in [0,1]), although this peculiarity is a
mathematicalconsequence of insisting on the population doubling exactly at each
generation. If Ytis the proportion of the limiting population belonging to lines
which became AA at exactly the tth generation, then Y = t 1 Yt. t is interesting
to note that the stochastic process
2Yt, j=1,2,-.,t= I
is such that almost every realisation is monotonically increasing, the form of the
'remainder' term in the submartingale decomposition theorem (Loeve, 1963,
p. 389). Some properties of Y may be obtained by enumerating the possible
structures of F1, and equating the unconditional expectations of certain variables,
to the appropriate expectations obtained after conditioning by the outcome of F1.
The possible F1 's are listed in column 2 of TableII,preceded by their probabilities.
of the same size and age that have always been that size. The stochastic process
describing the number of individuals in Ft which are homozygous for a given
allele, say A, is not a branching process, nor even a Markov process. However,
the probability P, that Ft will consist entirely of AA's, has a simple recurrence
relation. The probabilities that the offspring of a heterozygote are (AA,AA),
(AA,Aa) or (Aa,Aa) are 1/16,1/4,1/4 respectively. It is then required that the
offspring should consist entirely of AA's after (t- 1) generations, which leads to
11 1 2Pt = + Pt-1 + Pt2-1
from which P3 = 0.083840. Since the Pt are obviously increasing, lim0 Pt = P,
the probability that the population ultimately consists entirely of AA's satisfies
11 1 1 2P=- +-p +P2
16 4 4
of which the relevant root is P = 1 1/2 - V2 = 0.085786. For the comparable
stationary population the chance that all its members are AA is given by
(1/4 + 1/2 *1/4 + 1/2 *1/2 *1/4)8 = 0.001342.
In the doubling population the elimination of heterozygotes occurs with
probability one. When it has occurred the population which will then consist
entirely of AA's and aa's will continue to increase, but with the numbersof these
types, and hence of the two alleles, in a constant proportion. The remainderof this section is devoted to obtaining some propertiesof Y,the randomproportion
of AA's when the heterozygotes have been eliminated. Clearly, Y can take only
those values whose expression as a binary fraction can be written in terminating
form, and every such value in the interval [0,1] is taken with positive probability.
It is therefore an example of a random variable whose distributionfunction has
jumps at a set of points everywheredense (in [0,1]), although this peculiarity is a
mathematicalconsequence of insisting on the population doubling exactly at each
generation. If Ytis the proportion of the limiting population belonging to lines
which became AA at exactly the tth generation, then Y = t 1 Yt. t is interesting
to note that the stochastic process
2Yt, j=1,2,-.,t= I
is such that almost every realisation is monotonically increasing, the form of the
'remainder' term in the submartingale decomposition theorem (Loeve, 1963,
p. 389). Some properties of Y may be obtained by enumerating the possible
structures of F1, and equating the unconditional expectations of certain variables,
to the appropriate expectations obtained after conditioning by the outcome of F1.
The possible F1 's are listed in column 2 of TableII,preceded by their probabilities.
1191919191919
8/8/2019 A Mathematical Study of the Founder Principle
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Column 3 givesthe conditionalexpectationof Y,columns4 and 5 give the con-
ditionalvarianceof Y and the probability hat Y = 0, wherev and P denote he
unconditionalvalues of these quantities.Column6 gives the conditional xpec-tation of ez, wherem(z) is the unconditionalvalue.
TABLE I
Probabilitiesof possibleF1's,and values of various haracteristicsf populationstructure onditionalon these,for the growing,selfingpopulation
Pr. F,1 S{Y\F1} var{Yr|FI Pr{Y=OIF,} ?{ez\F,}
1AA,AA 1 0 0 ez16
- AA,Aa 4 ^ 0 e '2m( z)
AA,aa1
0 0 ezI
Aa,Aa 2 \2
(z
aa,aa 0 0 1 116
AA
Column 3 givesthe conditionalexpectationof Y,columns4 and 5 give the con-
ditionalvarianceof Y and the probability hat Y = 0, wherev and P denote he
unconditionalvalues of these quantities.Column6 gives the conditional xpec-tation of ez, wherem(z) is the unconditionalvalue.
TABLE I
Probabilitiesof possibleF1's,and values of various haracteristicsf populationstructure onditionalon these,for the growing,selfingpopulation
Pr. F,1 S{Y\F1} var{Yr|FI Pr{Y=OIF,} ?{ez\F,}
1AA,AA 1 0 0 ez16
- AA,Aa 4 ^ 0 e '2m( z)
AA,aa1
0 0 ezI
Aa,Aa 2 \2
(z
aa,aa 0 0 1 116
AA
Column 3 givesthe conditionalexpectationof Y,columns4 and 5 give the con-
ditionalvarianceof Y and the probability hat Y = 0, wherev and P denote he
unconditionalvalues of these quantities.Column6 gives the conditional xpec-tation of ez, wherem(z) is the unconditionalvalue.
TABLE I
Probabilitiesof possibleF1's,and values of various haracteristicsf populationstructure onditionalon these,for the growing,selfingpopulation
Pr. F,1 S{Y\F1} var{Yr|FI Pr{Y=OIF,} ?{ez\F,}
1AA,AA 1 0 0 ez16
- AA,Aa 4 ^ 0 e '2m( z)
AA,aa1
0 0 ezI
Aa,Aa 2 \2
(z
aa,aa 0 0 1 116
AA
Column 3 givesthe conditionalexpectationof Y,columns4 and 5 give the con-
ditionalvarianceof Y and the probability hat Y = 0, wherev and P denote he
unconditionalvalues of these quantities.Column6 gives the conditional xpec-tation of ez, wherem(z) is the unconditionalvalue.
TABLE I
Probabilitiesof possibleF1's,and values of various haracteristicsf populationstructure onditionalon these,for the growing,selfingpopulation
Pr. F,1 S{Y\F1} var{Yr|FI Pr{Y=OIF,} ?{ez\F,}
1AA,AA 1 0 0 ez16
- AA,Aa 4 ^ 0 e '2m( z)
AA,aa1
0 0 ezI
Aa,Aa 2 \2
(z
aa,aa 0 0 1 116
AA
Column 3 givesthe conditionalexpectationof Y,columns4 and 5 give the con-
ditionalvarianceof Y and the probability hat Y = 0, wherev and P denote he
unconditionalvalues of these quantities.Column6 gives the conditional xpec-tation of ez, wherem(z) is the unconditionalvalue.
TABLE I
Probabilitiesof possibleF1's,and values of various haracteristicsf populationstructure onditionalon these,for the growing,selfingpopulation
Pr. F,1 S{Y\F1} var{Yr|FI Pr{Y=OIF,} ?{ez\F,}
1AA,AA 1 0 0 ez16
- AA,Aa 4 ^ 0 e '2m( z)
AA,aa1
0 0 ezI
Aa,Aa 2 \2
(z
aa,aa 0 0 1 116
AA
Column 3 givesthe conditionalexpectationof Y,columns4 and 5 give the con-
ditionalvarianceof Y and the probability hat Y = 0, wherev and P denote he
unconditionalvalues of these quantities.Column6 gives the conditional xpec-tation of ez, wherem(z) is the unconditionalvalue.
TABLE I
Probabilitiesof possibleF1's,and values of various haracteristicsf populationstructure onditionalon these,for the growing,selfingpopulation
Pr. F,1 S{Y\F1} var{Yr|FI Pr{Y=OIF,} ?{ez\F,}
1AA,AA 1 0 0 ez16
- AA,Aa 4 ^ 0 e '2m( z)
AA,aa1
0 0 ezI
Aa,Aa 2 \2
(z
aa,aa 0 0 1 116
AA
For instance to obtain v we have on writingdown the two expressionsor the
secondmomentaboutzero:
-v+4T6H+4+4v+8(1+1 4 + )14(16+4)whichgivesv = 1/12. For the probabilityof the eliminationof A,
1 1 1p 2P=- +-P + -p2
whichwas derivedaboveby a more or lessequivalentmethod.An identityor the
moment generating unction written down from the last column simplifieso
4m(z)= {(l+ez/2)+m( z)}2
Clearly,Yis distributedymmetricallybout1/2.If (z)is the momentgenerating
For instance to obtain v we have on writingdown the two expressionsor the
secondmomentaboutzero:
-v+4T6H+4+4v+8(1+1 4 + )14(16+4)whichgivesv = 1/12. For the probabilityof the eliminationof A,
1 1 1p 2P=- +-P + -p2
whichwas derivedaboveby a more or lessequivalentmethod.An identityor the
moment generating unction written down from the last column simplifieso
4m(z)= {(l+ez/2)+m( z)}2
Clearly,Yis distributedymmetricallybout1/2.If (z)is the momentgenerating
For instance to obtain v we have on writingdown the two expressionsor the
secondmomentaboutzero:
-v+4T6H+4+4v+8(1+1 4 + )14(16+4)whichgivesv = 1/12. For the probabilityof the eliminationof A,
1 1 1p 2P=- +-P + -p2
whichwas derivedaboveby a more or lessequivalentmethod.An identityor the
moment generating unction written down from the last column simplifieso
4m(z)= {(l+ez/2)+m( z)}2
Clearly,Yis distributedymmetricallybout1/2.If (z)is the momentgenerating
For instance to obtain v we have on writingdown the two expressionsor the
secondmomentaboutzero:
-v+4T6H+4+4v+8(1+1 4 + )14(16+4)whichgivesv = 1/12. For the probabilityof the eliminationof A,
1 1 1p 2P=- +-P + -p2
whichwas derivedaboveby a more or lessequivalentmethod.An identityor the
moment generating unction written down from the last column simplifieso
4m(z)= {(l+ez/2)+m( z)}2
Clearly,Yis distributedymmetricallybout1/2.If (z)is the momentgenerating
For instance to obtain v we have on writingdown the two expressionsor the
secondmomentaboutzero:
-v+4T6H+4+4v+8(1+1 4 + )14(16+4)whichgivesv = 1/12. For the probabilityof the eliminationof A,
1 1 1p 2P=- +-P + -p2
whichwas derivedaboveby a more or lessequivalentmethod.An identityor the
moment generating unction written down from the last column simplifieso
4m(z)= {(l+ez/2)+m( z)}2
Clearly,Yis distributedymmetricallybout1/2.If (z)is the momentgenerating
For instance to obtain v we have on writingdown the two expressionsor the
secondmomentaboutzero:
-v+4T6H+4+4v+8(1+1 4 + )14(16+4)whichgivesv = 1/12. For the probabilityof the eliminationof A,
1 1 1p 2P=- +-P + -p2
whichwas derivedaboveby a more or lessequivalentmethod.An identityor the
moment generating unction written down from the last column simplifieso
4m(z)= {(l+ez/2)+m( z)}2
Clearly,Yis distributedymmetricallybout1/2.If (z)is the momentgenerating
1202020202020 P. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE
8/8/2019 A Mathematical Study of the Founder Principle
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A mathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary eneticsmathematical tudyof thefounderprincipleof evolutionary enetics
function of Y - 1/2, then on writing m(z) = e'Z2 /(z), and then replacing z by
2z for convenience,+(z)
is found to satisfy the functional relation
(9) 4+(z)= cosh z + (z) .
Since Y is bounded, all its moments exist, and expansion of the m.g.f. in (9)
provides a recurrencerelation for the even ordercentralmoments. The first few are
1 11 121 61663#2 2= , P4 =
720 6 = 36288' P8 79315200'
of which the first value confirms the solution of (8). Since the probabilities of
the end points are known exactly, the moments of the distribution conditionalon fixation not occurring can be calculated from the formula
(10) 12k -2P 2k-2P )
from which we obtain
12 = 0.048816, /14= 0.005498, 16 = 0.000789, % = 0.000129.
The coefficient of kurtosis of the conditional distribution is f2 = 2.3071.
3. RandommatingNotation used in this section is not everywherecomparable with that of the last.
Since a random mating population cannot be initiated by a single individual,
in order to make the situations in this section and the last as similar as possible,
I have assumed that the population begins with an F1 consisting of 2 animals,
each of whose 4 genes are A or a with probability 1/2. This means that if the
mathematical definition were extrapolated backwards, independently of its
interpretation, we could imagine an Fo consisting of a single heterozygote. As in
studies of random mating populations of constant size, only the number of genes
in each generation is considered, and they are supposed to be determined inde-
pendently, being A or a with probabilities equal to the proportions in the previousgeneration. Moran (1962, pp. 12-20) has discussed the implications for the form
of the offspring distribution of the constant population model and analogous
considerations apply here. Let Zt be the number of A genes in F,. The distribution
of Zt conditional on Z- = z,_ is binomial with n =2'+ p = (1/2)tzti.
The distribution may be computed explicitly for small t, and for t = 3 it is given
in the first column of Table III. For a comparable population of constant size,
suppose that Fo had consisted of 8 heterozygotes, which had then evolved through
3 generations of random mating. The distribution of Z3, the number of A's in
F3 is given by post-multiplying the 1 x 17 row vector with 1 in its ninth column
and zeros elsewhere, three times by the matrix (ail) with elements
function of Y - 1/2, then on writing m(z) = e'Z2 /(z), and then replacing z by
2z for convenience,+(z)
is found to satisfy the functional relation
(9) 4+(z)= cosh z + (z) .
Since Y is bounded, all its moments exist, and expansion of the m.g.f. in (9)
provides a recurrencerelation for the even ordercentralmoments. The first few are
1 11 121 61663#2 2= , P4 =
720 6 = 36288' P8 79315200'
of which the first value confirms the solution of (8). Since the probabilities of
the end points are known exactly, the moments of the distribution conditionalon fixation not occurring can be calculated from the formula
(10) 12k -2P 2k-2P )
from which we obtain
12 = 0.048816, /14= 0.005498, 16 = 0.000789, % = 0.000129.
The coefficient of kurtosis of the conditional distribution is f2 = 2.3071.
3. RandommatingNotation used in this section is not everywherecomparable with that of the last.
Since a random mating population cannot be initiated by a single individual,
in order to make the situations in this section and the last as similar as possible,
I have assumed that the population begins with an F1 consisting of 2 animals,
each of whose 4 genes are A or a with probability 1/2. This means that if the
mathematical definition were extrapolated backwards, independently of its
interpretation, we could imagine an Fo consisting of a single heterozygote. As in
studies of random mating populations of constant size, only the number of genes
in each generation is considered, and they are supposed to be determined inde-
pendently, being A or a with probabilities equal to the proportions in the previousgeneration. Moran (1962, pp. 12-20) has discussed the implications for the form
of the offspring distribution of the constant population model and analogous
considerations apply here. Let Zt be the number of A genes in F,. The distribution
of Zt conditional on Z- = z,_ is binomial with n =2'+ p = (1/2)tzti.
The distribution may be computed explicitly for small t, and for t = 3 it is given
in the first column of Table III. For a comparable population of constant size,
suppose that Fo had consisted of 8 heterozygotes, which had then evolved through
3 generations of random mating. The distribution of Z3, the number of A's in
F3 is given by post-multiplying the 1 x 17 row vector with 1 in its ninth column
and zeros elsewhere, three times by the matrix (ail) with elements
function of Y - 1/2, then on writing m(z) = e'Z2 /(z), and then replacing z by
2z for convenience,+(z)
is found to satisfy the functional relation
(9) 4+(z)= cosh z + (z) .
Since Y is bounded, all its moments exist, and expansion of the m.g.f. in (9)
provides a recurrencerelation for the even ordercentralmoments. The first few are
1 11 121 61663#2 2= , P4 =
720 6 = 36288' P8 79315200'
of which the first value confirms the solution of (8). Since the probabilities of
the end points are known exactly, the moments of the distribution conditionalon fixation not occurring can be calculated from the formula
(10) 12k -2P 2k-2P )
from which we obtain
12 = 0.048816, /14= 0.005498, 16 = 0.000789, % = 0.000129.
The coefficient of kurtosis of the conditional distribution is f2 = 2.3071.
3. RandommatingNotation used in this section is not everywherecomparable with that of the last.
Since a random mating population cannot be initiated by a single individual,
in order to make the situations in this section and the last as similar as possible,
I have assumed that the population begins with an F1 consisting of 2 animals,
each of whose 4 genes are A or a with probability 1/2. This means that if the
mathematical definition were extrapolated backwards, independently of its
interpretation, we could imagine an Fo consisting of a single heterozygote. As in
studies of random mating populations of constant size, only the number of genes
in each generation is considered, and they are supposed to be determined inde-
pendently, being A or a with probabilities equal to the proportions in the previousgeneration. Moran (1962, pp. 12-20) has discussed the implications for the form
of the offspring distribution of the constant population model and analogous
considerations apply here. Let Zt be the number of A genes in F,. The distribution
of Zt conditional on Z- = z,_ is binomial with n =2'+ p = (1/2)tzti.
The distribution may be computed explicitly for small t, and for t = 3 it is given
in the first column of Table III. For a comparable population of constant size,
suppose that Fo had consisted of 8 heterozygotes, which had then evolved through
3 generations of random mating. The distribution of Z3, the number of A's in
F3 is given by post-multiplying the 1 x 17 row vector with 1 in its ninth column
and zeros elsewhere, three times by the matrix (ail) with elements
function of Y - 1/2, then on writing m(z) = e'Z2 /(z), and then replacing z by
2z for convenience,+(z)
is found to satisfy the functional relation
(9) 4+(z)= cosh z + (z) .
Since Y is bounded, all its moments exist, and expansion of the m.g.f. in (9)
provides a recurrencerelation for the even ordercentralmoments. The first few are
1 11 121 61663#2 2= , P4 =
720 6 = 36288' P8 79315200'
of which the first value confirms the solution of (8). Since the probabilities of
the end points are known exactly, the moments of the distribution conditionalon fixation not occurring can be calculated from the formula
(10) 12k -2P 2k-2P )
from which we obtain
12 = 0.048816, /14= 0.005498, 16 = 0.000789, % = 0.000129.
The coefficient of kurtosis of the conditional distribution is f2 = 2.3071.
3. RandommatingNotation used in this section is not everywherecomparable with that of the last.
Since a random mating population cannot be initiated by a single individual,
in order to make the situations in this section and the last as similar as possible,
I have assumed that the population begins with an F1 consisting of 2 animals,
each of whose 4 genes are A or a with probability 1/2. This means that if the
mathematical definition were extrapolated backwards, independently of its
interpretation, we could imagine an Fo consisting of a single heterozygote. As in
studies of random mating populations of constant size, only the number of genes
in each generation is considered, and they are supposed to be determined inde-
pendently, being A or a with probabilities equal to the proportions in the previousgeneration. Moran (1962, pp. 12-20) has discussed the implications for the form
of the offspring distribution of the constant population model and analogous
considerations apply here. Let Zt be the number of A genes in F,. The distribution
of Zt conditional on Z- = z,_ is binomial with n =2'+ p = (1/2)tzti.
The distribution may be computed explicitly for small t, and for t = 3 it is given
in the first column of Table III. For a comparable population of constant size,
suppose that Fo had consisted of 8 heterozygotes, which had then evolved through
3 generations of random mating. The distribution of Z3, the number of A's in
F3 is given by post-multiplying the 1 x 17 row vector with 1 in its ninth column
and zeros elsewhere, three times by the matrix (ail) with elements
function of Y - 1/2, then on writing m(z) = e'Z2 /(z), and then replacing z by
2z for convenience,+(z)
is found to satisfy the functional relation
(9) 4+(z)= cosh z + (z) .
Since Y is bounded, all its moments exist, and expansion of the m.g.f. in (9)
provides a recurrencerelation for the even ordercentralmoments. The first few are
1 11 121 61663#2 2= , P4 =
720 6 = 36288' P8 79315200'
of which the first value confirms the solution of (8). Since the probabilities of
the end points are known exactly, the moments of the distribution conditionalon fixation not occurring can be calculated from the formula
(10) 12k -2P 2k-2P )
from which we obtain
12 = 0.048816, /14= 0.005498, 16 = 0.000789, % = 0.000129.
The coefficient of kurtosis of the conditional distribution is f2 = 2.3071.
3. RandommatingNotation used in this section is not everywherecomparable with that of the last.
Since a random mating population cannot be initiated by a single individual,
in order to make the situations in this section and the last as similar as possible,
I have assumed that the population begins with an F1 consisting of 2 animals,
each of whose 4 genes are A or a with probability 1/2. This means that if the
mathematical definition were extrapolated backwards, independently of its
interpretation, we could imagine an Fo consisting of a single heterozygote. As in
studies of random mating populations of constant size, only the number of genes
in each generation is considered, and they are supposed to be determined inde-
pendently, being A or a with probabilities equal to the proportions in the previousgeneration. Moran (1962, pp. 12-20) has discussed the implications for the form
of the offspring distribution of the constant population model and analogous
considerations apply here. Let Zt be the number of A genes in F,. The distribution
of Zt conditional on Z- = z,_ is binomial with n =2'+ p = (1/2)tzti.
The distribution may be computed explicitly for small t, and for t = 3 it is given
in the first column of Table III. For a comparable population of constant size,
suppose that Fo had consisted of 8 heterozygotes, which had then evolved through
3 generations of random mating. The distribution of Z3, the number of A's in
F3 is given by post-multiplying the 1 x 17 row vector with 1 in its ninth column
and zeros elsewhere, three times by the matrix (ail) with elements
function of Y - 1/2, then on writing m(z) = e'Z2 /(z), and then replacing z by
2z for convenience,+(z)
is found to satisfy the functional relation
(9) 4+(z)= cosh z + (z) .
Since Y is bounded, all its moments exist, and expansion of the m.g.f. in (9)
provides a recurrencerelation for the even ordercentralmoments. The first few are
1 11 121 61663#2 2= , P4 =
720 6 = 36288' P8 79315200'
of which the first value confirms the solution of (8). Since the probabilities of
the end points are known exactly, the moments of the distribution conditionalon fixation not occurring can be calculated from the formula
(10) 12k -2P 2k-2P )
from which we obtain
12 = 0.048816, /14= 0.005498, 16 = 0.000789, % = 0.000129.
The coefficient of kurtosis of the conditional distribution is f2 = 2.3071.
3. RandommatingNotation used in this section is not everywherecomparable with that of the last.
Since a random mating population cannot be initiated by a single individual,
in order to make the situations in this section and the last as similar as possible,
I have assumed that the population begins with an F1 consisting of 2 animals,
each of whose 4 genes are A or a with probability 1/2. This means that if the
mathematical definition were extrapolated backwards, independently of its
interpretation, we could imagine an Fo consisting of a single heterozygote. As in
studies of random mating populations of constant size, only the number of genes
in each generation is considered, and they are supposed to be determined inde-
pendently, being A or a with probabilities equal to the proportions in the previousgeneration. Moran (1962, pp. 12-20) has discussed the implications for the form
of the offspring distribution of the constant population model and analogous
considerations apply here. Let Zt be the number of A genes in F,. The distribution
of Zt conditional on Z- = z,_ is binomial with n =2'+ p = (1/2)tzti.
The distribution may be computed explicitly for small t, and for t = 3 it is given
in the first column of Table III. For a comparable population of constant size,
suppose that Fo had consisted of 8 heterozygotes, which had then evolved through
3 generations of random mating. The distribution of Z3, the number of A's in
F3 is given by post-multiplying the 1 x 17 row vector with 1 in its ninth column
and zeros elsewhere, three times by the matrix (ail) with elements
1212121212121
8/8/2019 A Mathematical Study of the Founder Principle
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al= 16- i1
iJ{ HJ)
( )6 16)
(Feller, 1951).The resulting distribution is given in the second column of Table III.
In this case the probability of elimination of A can be seen to be greater for the
growing population. The variances of the proportion of A genes are 0.0962 and
0.0440 for the growing and stationary populations respectively.
TABLE II
Distribution of number of A's after three generations of random mating
(The distribution is symmetric about 8.)
Probability
Growing Stationaryj Population Population
0 .0996 .0068
1 .0284 .0155
2 .0423 .0290
3 .0505 .0457
4 .0562 .0639
5 .0607 .0816
6 .0738 .0964
7 .0655 .1062
8 .0661 .1096
Now consider the sequence of random variables Y = Z/2t+1, the proportions
of A genes in successive generations.
It will be shown that Yt ends to a limit Y as t -+ oo, and some of the propertiesof Y obtained.
A recurrencerelation can be derived for the second moments of the Zt about
the origin as follows: let P(z,t) = Pr(Zt = z),
2t"I
He(t)
= 2x2P(x,
t)
=t
x 2y(2X
=O 0
= ]P(y,t - 1) X2y
y=0
2= P(yt - 1) 2y 1 +(2 -I1) - -
H;( -)+( 2-^l )82( -)
al= 16- i1
iJ{ HJ)
( )6 16)
(Feller, 1951).The resulting distribution is given in the second column of Table III.
In this case the probability of elimination of A can be seen to be greater for the
growing population. The variances of the proportion of A genes are 0.0962 and
0.0440 for the growing and stationary populations respectively.
TABLE II
Distribution of number of A's after three generations of random mating
(The distribution is symmetric about 8.)
Probability
Growing Stationaryj Population Population
0 .0996 .0068
1 .0284 .0155
2 .0423 .0290
3 .0505 .0457
4 .0562 .0639
5 .0607 .0816
6 .0738 .0964
7 .0655 .1062
8 .0661 .1096
Now consider the sequence of random variables Y = Z/2t+1, the proportions
of A genes in successive generations.
It will be shown that Yt ends to a limit Y as t -+ oo, and some of the propertiesof Y obtained.
A recurrencerelation can be derived for the second moments of the Zt about
the origin as follows: let P(z,t) = Pr(Zt = z),
2t"I
He(t)
= 2x2P(x,
t)
=t
x 2y(2X
=O 0
= ]P(y,t - 1) X2y
y=0
2= P(yt - 1) 2y 1 +(2 -I1) - -
H;( -)+( 2-^l )82( -)
al= 16- i1
iJ{ HJ)
( )6 16)
(Feller, 1951).The resulting distribution is given in the second column of Table III.
In this case the probability of elimination of A can be seen to be greater for the
growing population. The variances of the proportion of A genes are 0.0962 and
0.0440 for the growing and stationary populations respectively.
TABLE II
Distribution of number of A's after three generations of random mating
(The distribution is symmetric about 8.)
Probability
Growing Stationaryj Population Population
0 .0996 .0068
1 .0284 .0155
2 .0423 .0290
3 .0505 .0457
4 .0562 .0639
5 .0607 .0816
6 .0738 .0964
7 .0655 .1062
8 .0661 .1096
Now consider the sequence of random variables Y = Z/2t+1, the proportions
of A genes in successive generations.
It will be shown that Yt ends to a limit Y as t -+ oo, and some of the propertiesof Y obtained.
A recurrencerelation can be derived for the second moments of the Zt about
the origin as follows: let P(z,t) = Pr(Zt = z),
2t"I
He(t)
= 2x2P(x,
t)
=t
x 2y(2X
=O 0
= ]P(y,t - 1) X2y
y=0
2= P(yt - 1) 2y 1 +(2 -I1) - -
H;( -)+( 2-^l )82( -)
al= 16- i1
iJ{ HJ)
( )6 16)
(Feller, 1951).The resulting distribution is given in the second column of Table III.
In this case the probability of elimination of A can be seen to be greater for the
growing population. The variances of the proportion of A genes are 0.0962 and
0.0440 for the growing and stationary populations respectively.
TABLE II
Distribution of number of A's after three generations of random mating
(The distribution is symmetric about 8.)
Probability
Growing Stationaryj Population Population
0 .0996 .0068
1 .0284 .0155
2 .0423 .0290
3 .0505 .0457
4 .0562 .0639
5 .0607 .0816
6 .0738 .0964
7 .0655 .1062
8 .0661 .1096
Now consider the sequence of random variables Y = Z/2t+1, the proportions
of A genes in successive generations.
It will be shown that Yt ends to a limit Y as t -+ oo, and some of the propertiesof Y obtained.
A recurrencerelation can be derived for the second moments of the Zt about
the origin as follows: let P(z,t) = Pr(Zt = z),
2t"I
He(t)
= 2x2P(x,
t)
=t
x 2y(2X
=O 0
= ]P(y,t - 1) X2y
y=0
2= P(yt - 1) 2y 1 +(2 -I1) - -
H;( -)+( 2-^l )82( -)
al= 16- i1
iJ{ HJ)
( )6 16)
(Feller, 1951).The resulting distribution is given in the second column of Table III.
In this case the probability of elimination of A can be seen to be greater for the
growing population. The variances of the proportion of A genes are 0.0962 and
0.0440 for the growing and stationary populations respectively.
TABLE II
Distribution of number of A's after three generations of random mating
(The distribution is symmetric about 8.)
Probability
Growing Stationaryj Population Population
0 .0996 .0068
1 .0284 .0155
2 .0423 .0290
3 .0505 .0457
4 .0562 .0639
5 .0607 .0816
6 .0738 .0964
7 .0655 .1062
8 .0661 .1096
Now consider the sequence of random variables Y = Z/2t+1, the proportions
of A genes in successive generations.
It will be shown that Yt ends to a limit Y as t -+ oo, and some of the propertiesof Y obtained.
A recurrencerelation can be derived for the second moments of the Zt about
the origin as follows: let P(z,t) = Pr(Zt = z),
2t"I
He(t)
= 2x2P(x,
t)
=t
x 2y(2X
=O 0
= ]P(y,t - 1) X2y
y=0
2= P(yt - 1) 2y 1 +(2 -I1) - -
H;( -)+( 2-^l )82( -)
al= 16- i1
iJ{ HJ)
( )6 16)
(Feller, 1951).The resulting distribution is given in the second column of Table III.
In this case the probability of elimination of A can be seen to be greater for the
growing population. The variances of the proportion of A genes are 0.0962 and
0.0440 for the growing and stationary populations respectively.
TABLE II
Distribution of number of A's after three generations of random mating
(The distribution is symmetric about 8.)
Probability
Growing Stationaryj Population Population
0 .0996 .0068
1 .0284 .0155
2 .0423 .0290
3 .0505 .0457
4 .0562 .0639
5 .0607 .0816
6 .0738 .0964
7 .0655 .1062
8 .0661 .1096
Now consider the sequence of random variables Y = Z/2t+1, the proportions
of A genes in successive generations.
It will be shown that Yt ends to a limit Y as t -+ oo, and some of the propertiesof Y obtained.
A recurrencerelation can be derived for the second moments of the Zt about
the origin as follows: let P(z,t) = Pr(Zt = z),
2t"I
He(t)
= 2x2P(x,
t)
=t
x 2y(2X
=O 0
= ]P(y,t - 1) X2y
y=0
2= P(yt - 1) 2y 1 +(2 -I1) - -
H;( -)+( 2-^l )82( -)
1222222222222 P. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE
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A mathematicaltudyof thefounderprincipleof evolutionary eneticsmathematicaltudyof thefounderprincipleof evolutionary eneticsmathematicaltudyof thefounderprincipleof evolutionary eneticsmathematicaltudyof thefounderprincipleof evolutionary eneticsmathematicaltudyof thefounderprincipleof evolutionary eneticsmathematicaltudyof thefounderprincipleof evolutionary enetics
The step from the thirdto the fourth line follows from the fact that the secondsummation s the second moment about zero of a binomialdistributionwithn = 2+, p = y/2t. On writing 4 = u2
+ ,u2 a recurrence elationfor the var-iancesof Z, is obtained
82(t) = (4-
1 2(t-1) + 2t-.
If v2(t) = #2(t)/4t+l denotesthe variances f the Yt heysatisfy herecurrenceela-tion
(11) v2(t)= v2(t- 1) +V-4T ~- v2(t 1) )
Since the variancesof all distributions n [0,1] areboundedaboveby 1/4, (11shows that the sequence tends monotonically, as t -> ooto a limit
_
1/4.On writing 11)in the form
I I 1( V2(t)) ()(--2(t-))
an explicitsolution can be obtained or any t,
(--.(,): (1_4) (,-)..( __ ) -(4 0(0)).
More lengthyalgebra eads to the followingrecurrencerelation for the fourthmomentsv4(t)
{IV 1 I 2t3 1 t
V4(t) =4(t() )
d 2 )( , - , ) { ~ ) ) _ ( T ) .
With nitial valuesv2(0) = v4(0)=0, computationusing(11) and(12) leadsto thelimits
(13) v2 = 0.105606, V4= 0.020182.
Foreveryk,
V2k(t)= Yt- )
-tPr (Yt1 = q)
t
2 Yt-=
>_ Pr(y,t = ) (?-
= V20(t-1),
The step from the thirdto the fourth line follows from the fact that the secondsummation s the second moment about zero of a binomialdistributionwithn = 2+, p = y/2t. On writing 4 = u2
+ ,u2 a recurrence elationfor the var-iancesof Z, is obtained
82(t) = (4-
1 2(t-1) + 2t-.
If v2(t) = #2(t)/4t+l denotesthe variances f the Yt heysatisfy herecurrenceela-tion
(11) v2(t)= v2(t- 1) +V-4T ~- v2(t 1) )
Since the variancesof all distributions n [0,1] areboundedaboveby 1/4, (11shows that the sequence tends monotonically, as t -> ooto a limit
_
1/4.On writing 11)in the form
I I 1( V2(t)) ()(--2(t-))
an explicitsolution can be obtained or any t,
(--.(,): (1_4) (,-)..( __ ) -(4 0(0)).
More lengthyalgebra eads to the followingrecurrencerelation for the fourthmomentsv4(t)
{IV 1 I 2t3 1 t
V4(t) =4(t() )
d 2 )( , - , ) { ~ ) ) _ ( T ) .
With nitial valuesv2(0) = v4(0)=0, computationusing(11) and(12) leadsto thelimits
(13) v2 = 0.105606, V4= 0.020182.
Foreveryk,
V2k(t)= Yt- )
-tPr (Yt1 = q)
t
2 Yt-=
>_ Pr(y,t = ) (?-
= V20(t-1),
The step from the thirdto the fourth line follows from the fact that the secondsummation s the second moment about zero of a binomialdistributionwithn = 2+, p = y/2t. On writing 4 = u2
+ ,u2 a recurrence elationfor the var-iancesof Z, is obtained
82(t) = (4-
1 2(t-1) + 2t-.
If v2(t) = #2(t)/4t+l denotesthe variances f the Yt heysatisfy herecurrenceela-tion
(11) v2(t)= v2(t- 1) +V-4T ~- v2(t 1) )
Since the variancesof all distributions n [0,1] areboundedaboveby 1/4, (11shows that the sequence tends monotonically, as t -> ooto a limit
_
1/4.On writing 11)in the form
I I 1( V2(t)) ()(--2(t-))
an explicitsolution can be obtained or any t,
(--.(,): (1_4) (,-)..( __ ) -(4 0(0)).
More lengthyalgebra eads to the followingrecurrencerelation for the fourthmomentsv4(t)
{IV 1 I 2t3 1 t
V4(t) =4(t() )
d 2 )( , - , ) { ~ ) ) _ ( T ) .
With nitial valuesv2(0) = v4(0)=0, computationusing(11) and(12) leadsto thelimits
(13) v2 = 0.105606, V4= 0.020182.
Foreveryk,
V2k(t)= Yt- )
-tPr (Yt1 = q)
t
2 Yt-=
>_ Pr(y,t = ) (?-
= V20(t-1),
The step from the thirdto the fourth line follows from the fact that the secondsummation s the second moment about zero of a binomialdistributionwithn = 2+, p = y/2t. On writing 4 = u2
+ ,u2 a recurrence elationfor the var-iancesof Z, is obtained
82(t) = (4-
1 2(t-1) + 2t-.
If v2(t) = #2(t)/4t+l denotesthe variances f the Yt heysatisfy herecurrenceela-tion
(11) v2(t)= v2(t- 1) +V-4T ~- v2(t 1) )
Since the variancesof all distributions n [0,1] areboundedaboveby 1/4, (11shows that the sequence tends monotonically, as t -> ooto a limit
_
1/4.On writing 11)in the form
I I 1( V2(t)) ()(--2(t-))
an explicitsolution can be obtained or any t,
(--.(,): (1_4) (,-)..( __ ) -(4 0(0)).
More lengthyalgebra eads to the followingrecurrencerelation for the fourthmomentsv4(t)
{IV 1 I 2t3 1 t
V4(t) =4(t() )
d 2 )( , - , ) { ~ ) ) _ ( T ) .
With nitial valuesv2(0) = v4(0)=0, computationusing(11) and(12) leadsto thelimits
(13) v2 = 0.105606, V4= 0.020182.
Foreveryk,
V2k(t)= Yt- )
-tPr (Yt1 = q)
t
2 Yt-=
>_ Pr(y,t = ) (?-
= V20(t-1),
The step from the thirdto the fourth line follows from the fact that the secondsummation s the second moment about zero of a binomialdistributionwithn = 2+, p = y/2t. On writing 4 = u2
+ ,u2 a recurrence elationfor the var-iancesof Z, is obtained
82(t) = (4-
1 2(t-1) + 2t-.
If v2(t) = #2(t)/4t+l denotesthe variances f the Yt heysatisfy herecurrenceela-tion
(11) v2(t)= v2(t- 1) +V-4T ~- v2(t 1) )
Since the variancesof all distributions n [0,1] areboundedaboveby 1/4, (11shows that the sequence tends monotonically, as t -> ooto a limit
_
1/4.On writing 11)in the form
I I 1( V2(t)) ()(--2(t-))
an explicitsolution can be obtained or any t,
(--.(,): (1_4) (,-)..( __ ) -(4 0(0)).
More lengthyalgebra eads to the followingrecurrencerelation for the fourthmomentsv4(t)
{IV 1 I 2t3 1 t
V4(t) =4(t() )
d 2 )( , - , ) { ~ ) ) _ ( T ) .
With nitial valuesv2(0) = v4(0)=0, computationusing(11) and(12) leadsto thelimits
(13) v2 = 0.105606, V4= 0.020182.
Foreveryk,
V2k(t)= Yt- )
-tPr (Yt1 = q)
t
2 Yt-=
>_ Pr(y,t = ) (?-
= V20(t-1),
The step from the thirdto the fourth line follows from the fact that the secondsummation s the second moment about zero of a binomialdistributionwithn = 2+, p = y/2t. On writing 4 = u2
+ ,u2 a recurrence elationfor the var-iancesof Z, is obtained
82(t) = (4-
1 2(t-1) + 2t-.
If v2(t) = #2(t)/4t+l denotesthe variances f the Yt heysatisfy herecurrenceela-tion
(11) v2(t)= v2(t- 1) +V-4T ~- v2(t 1) )
Since the variancesof all distributions n [0,1] areboundedaboveby 1/4, (11shows that the sequence tends monotonically, as t -> ooto a limit
_
1/4.On writing 11)in the form
I I 1( V2(t)) ()(--2(t-))
an explicitsolution can be obtained or any t,
(--.(,): (1_4) (,-)..( __ ) -(4 0(0)).
More lengthyalgebra eads to the followingrecurrencerelation for the fourthmomentsv4(t)
{IV 1 I 2t3 1 t
V4(t) =4(t() )
d 2 )( , - , ) { ~ ) ) _ ( T ) .
With nitial valuesv2(0) = v4(0)=0, computationusing(11) and(12) leadsto thelimits
(13) v2 = 0.105606, V4= 0.020182.
Foreveryk,
V2k(t)= Yt- )
-tPr (Yt1 = q)
t
2 Yt-=
>_ Pr(y,t = ) (?-
= V20(t-1),
1232323232323
8/8/2019 A Mathematical Study of the Founder Principle
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on applyingJensen'stheoremto the convexfunction {(Yt- )2k Yt-1=t }, andthen usingthe symmetry f Yt-1about ?. Hencethe sequencev2k(t) is increasingandit is bounded aboveby(1/2)2k.Hence he momentsequences f the Yt end to
a limiting sequenceand since this must be the moment sequenceof a boundedrandomvariable, t definesit uniquely,and the convergenceof the sequence
{Yt} follows from the secondlimit theoremof the probabilitycalculus.(Seee.g. Rao and Kendall(1950)).Alternatively,{&Yt Yt_-I Yt-} = Yt-1 and so
{Yt}is a martingale,and the fact that its random variables are bounded is
easily enough seen to ensureconvergence y themartingale onvergenceheorem
(Doob, 1953,Chapter7).
In thisparagraph nd the next I obtainupperand lowerbounds ortheproba-
bilityof ultimatehomozygosity, howing n particular hat it is less thanone. Inthe presentproblem,actual computation or the early generations ollowedbynumerical extrapolationenables the exact value to be calculatedaccurately,but the methods of obtaining he bounds are of interest,andmaybe of valuein
parallelstudies, since it is clearlyimportantto know whetherthe probabilityof absorptionis boundedaway from one. The coefficientof kurtosis of Y is
P2 = 1.809738.Henceusingthe generalisation f Tchebychef'snequalityquoted
e.g. by Cram6r1946, p. 256)
Pr ( |ry - 1.5385997)
(P2 1)/{(1.5385992 - 1)2 + P2 1}
= 0.3022.
The probability hat a givenallele,say A, will be fixedis less than half this, i.e.0.1511.
Let yt be the probability hat the populationbecomeshomozygousat exactlythe tth generationconditionalon it beingheterozygousat the (t - 1)th,y, the
probabilitythat it becomeshomozygous at or before the tth generation,and
y = lim, . Vt hat it ultimatelybecomeshomozygous.The chance that fixationwill occur preciselyat time t can be shown to be greatestwhen Ft-_ contains
only one representative f one of the alleles,and least whentheyarepresentn
equalnumbers.Hence
1 )t 2t ( )t 2t+1
^(~~~~~-a'^
) ) " -
on applyingJensen'stheoremto the convexfunction {(Yt- )2k Yt-1=t }, andthen usingthe symmetry f Yt-1about ?. Hencethe sequencev2k(t) is increasingandit is bounded aboveby(1/2)2k.Hence he momentsequences f the Yt end to
a limiting sequenceand since this must be the moment sequenceof a boundedrandomvariable, t definesit uniquely,and the convergenceof the sequence
{Yt} follows from the secondlimit theoremof the probabilitycalculus.(Seee.g. Rao and Kendall(1950)).Alternatively,{&Yt Yt_-I Yt-} = Yt-1 and so
{Yt}is a martingale,and the fact that its random variables are bounded is
easily enough seen to ensureconvergence y themartingale onvergenceheorem
(Doob, 1953,Chapter7).
In thisparagraph nd the next I obtainupperand lowerbounds ortheproba-
bilityof ultimatehomozygosity, howing n particular hat it is less thanone. Inthe presentproblem,actual computation or the early generations ollowedbynumerical extrapolationenables the exact value to be calculatedaccurately,but the methods of obtaining he bounds are of interest,andmaybe of valuein
parallelstudies, since it is clearlyimportantto know whetherthe probabilityof absorptionis boundedaway from one. The coefficientof kurtosis of Y is
P2 = 1.809738.Henceusingthe generalisation f Tchebychef'snequalityquoted
e.g. by Cram6r1946, p. 256)
Pr ( |ry - 1.5385997)
(P2 1)/{(1.5385992 - 1)2 + P2 1}
= 0.3022.
The probability hat a givenallele,say A, will be fixedis less than half this, i.e.0.1511.
Let yt be the probability hat the populationbecomeshomozygousat exactlythe tth generationconditionalon it beingheterozygousat the (t - 1)th,y, the
probabilitythat it becomeshomozygous at or before the tth generation,and
y = lim, . Vt hat it ultimatelybecomeshomozygous.The chance that fixationwill occur preciselyat time t can be shown to be greatestwhen Ft-_ contains
only one representative f one of the alleles,and least whentheyarepresentn
equalnumbers.Hence
1 )t 2t ( )t 2t+1
^(~~~~~-a'^
) ) " -
on applyingJensen'stheoremto the convexfunction {(Yt- )2k Yt-1=t }, andthen usingthe symmetry f Yt-1about ?. Hencethe sequencev2k(t) is increasingandit is bounded aboveby(1/2)2k.Hence he momentsequences f the Yt end to
a limiting sequenceand since this must be the moment sequenceof a boundedrandomvariable, t definesit uniquely,and the convergenceof the sequence
{Yt} follows from the secondlimit theoremof the probabilitycalculus.(Seee.g. Rao and Kendall(1950)).Alternatively,{&Yt Yt_-I Yt-} = Yt-1 and so
{Yt}is a martingale,and the fact that its random variables are bounded is
easily enough seen to ensureconvergence y themartingale onvergenceheorem
(Doob, 1953,Chapter7).
In thisparagraph nd the next I obtainupperand lowerbounds ortheproba-
bilityof ultimatehomozygosity, howing n particular hat it is less thanone. Inthe presentproblem,actual computation or the early generations ollowedbynumerical extrapolationenables the exact value to be calculatedaccurately,but the methods of obtaining he bounds are of interest,andmaybe of valuein
parallelstudies, since it is clearlyimportantto know whetherthe probabilityof absorptionis boundedaway from one. The coefficientof kurtosis of Y is
P2 = 1.809738.Henceusingthe generalisation f Tchebychef'snequalityquoted
e.g. by Cram6r1946, p. 256)
Pr ( |ry - 1.5385997)
(P2 1)/{(1.5385992 - 1)2 + P2 1}
= 0.3022.
The probability hat a givenallele,say A, will be fixedis less than half this, i.e.0.1511.
Let yt be the probability hat the populationbecomeshomozygousat exactlythe tth generationconditionalon it beingheterozygousat the (t - 1)th,y, the
probabilitythat it becomeshomozygous at or before the tth generation,and
y = lim, . Vt hat it ultimatelybecomeshomozygous.The chance that fixationwill occur preciselyat time t can be shown to be greatestwhen Ft-_ contains
only one representative f one of the alleles,and least whentheyarepresentn
equalnumbers.Hence
1 )t 2t ( )t 2t+1
^(~~~~~-a'^
) ) " -
on applyingJensen'stheoremto the convexfunction {(Yt- )2k Yt-1=t }, andthen usingthe symmetry f Yt-1about ?. Hencethe sequencev2k(t) is increasingandit is bounded aboveby(1/2)2k.Hence he momentsequences f the Yt end to
a limiting sequenceand since this must be the moment sequenceof a boundedrandomvariable, t definesit uniquely,and the convergenceof the sequence
{Yt} follows from the secondlimit theoremof the probabilitycalculus.(Seee.g. Rao and Kendall(1950)).Alternatively,{&Yt Yt_-I Yt-} = Yt-1 and so
{Yt}is a martingale,and the fact that its random variables are bounded is
easily enough seen to ensureconvergence y themartingale onvergenceheorem
(Doob, 1953,Chapter7).
In thisparagraph nd the next I obtainupperand lowerbounds ortheproba-
bilityof ultimatehomozygosity, howing n particular hat it is less thanone. Inthe presentproblem,actual computation or the early generations ollowedbynumerical extrapolationenables the exact value to be calculatedaccurately,but the methods of obtaining he bounds are of interest,andmaybe of valuein
parallelstudies, since it is clearlyimportantto know whetherthe probabilityof absorptionis boundedaway from one. The coefficientof kurtosis of Y is
P2 = 1.809738.Henceusingthe generalisation f Tchebychef'snequalityquoted
e.g. by Cram6r1946, p. 256)
Pr ( |ry - 1.5385997)
(P2 1)/{(1.5385992 - 1)2 + P2 1}
= 0.3022.
The probability hat a givenallele,say A, will be fixedis less than half this, i.e.0.1511.
Let yt be the probability hat the populationbecomeshomozygousat exactlythe tth generationconditionalon it beingheterozygousat the (t - 1)th,y, the
probabilitythat it becomeshomozygous at or before the tth generation,and
y = lim, . Vt hat it ultimatelybecomeshomozygous.The chance that fixationwill occur preciselyat time t can be shown to be greatestwhen Ft-_ contains
only one representative f one of the alleles,and least whentheyarepresentn
equalnumbers.Hence
1 )t 2t ( )t 2t+1
^(~~~~~-a'^
) ) " -
on applyingJensen'stheoremto the convexfunction {(Yt- )2k Yt-1=t }, andthen usingthe symmetry f Yt-1about ?. Hencethe sequencev2k(t) is increasingandit is bounded aboveby(1/2)2k.Hence he momentsequences f the Yt end to
a limiting sequenceand since this must be the moment sequenceof a boundedrandomvariable, t definesit uniquely,and the convergenceof the sequence
{Yt} follows from the secondlimit theoremof the probabilitycalculus.(Seee.g. Rao and Kendall(1950)).Alternatively,{&Yt Yt_-I Yt-} = Yt-1 and so
{Yt}is a martingale,and the fact that its random variables are bounded is
easily enough seen to ensureconvergence y themartingale onvergenceheorem
(Doob, 1953,Chapter7).
In thisparagraph nd the next I obtainupperand lowerbounds ortheproba-
bilityof ultimatehomozygosity, howing n particular hat it is less thanone. Inthe presentproblem,actual computation or the early generations ollowedbynumerical extrapolationenables the exact value to be calculatedaccurately,but the methods of obtaining he bounds are of interest,andmaybe of valuein
parallelstudies, since it is clearlyimportantto know whetherthe probabilityof absorptionis boundedaway from one. The coefficientof kurtosis of Y is
P2 = 1.809738.Henceusingthe generalisation f Tchebychef'snequalityquoted
e.g. by Cram6r1946, p. 256)
Pr ( |ry - 1.5385997)
(P2 1)/{(1.5385992 - 1)2 + P2 1}
= 0.3022.
The probability hat a givenallele,say A, will be fixedis less than half this, i.e.0.1511.
Let yt be the probability hat the populationbecomeshomozygousat exactlythe tth generationconditionalon it beingheterozygousat the (t - 1)th,y, the
probabilitythat it becomeshomozygous at or before the tth generation,and
y = lim, . Vt hat it ultimatelybecomeshomozygous.The chance that fixationwill occur preciselyat time t can be shown to be greatestwhen Ft-_ contains
only one representative f one of the alleles,and least whentheyarepresentn
equalnumbers.Hence
1 )t 2t ( )t 2t+1
^(~~~~~-a'^
) ) " -
on applyingJensen'stheoremto the convexfunction {(Yt- )2k Yt-1=t }, andthen usingthe symmetry f Yt-1about ?. Hencethe sequencev2k(t) is increasingandit is bounded aboveby(1/2)2k.Hence he momentsequences f the Yt end to
a limiting sequenceand since this must be the moment sequenceof a boundedrandomvariable, t definesit uniquely,and the convergenceof the sequence
{Yt} follows from the secondlimit theoremof the probabilitycalculus.(Seee.g. Rao and Kendall(1950)).Alternatively,{&Yt Yt_-I Yt-} = Yt-1 and so
{Yt}is a martingale,and the fact that its random variables are bounded is
easily enough seen to ensureconvergence y themartingale onvergenceheorem
(Doob, 1953,Chapter7).
In thisparagraph nd the next I obtainupperand lowerbounds ortheproba-
bilityof ultimatehomozygosity, howing n particular hat it is less thanone. Inthe presentproblem,actual computation or the early generations ollowedbynumerical extrapolationenables the exact value to be calculatedaccurately,but the methods of obtaining he bounds are of interest,andmaybe of valuein
parallelstudies, since it is clearlyimportantto know whetherthe probabilityof absorptionis boundedaway from one. The coefficientof kurtosis of Y is
P2 = 1.809738.Henceusingthe generalisation f Tchebychef'snequalityquoted
e.g. by Cram6r1946, p. 256)
Pr ( |ry - 1.5385997)
(P2 1)/{(1.5385992 - 1)2 + P2 1}
= 0.3022.
The probability hat a givenallele,say A, will be fixedis less than half this, i.e.0.1511.
Let yt be the probability hat the populationbecomeshomozygousat exactlythe tth generationconditionalon it beingheterozygousat the (t - 1)th,y, the
probabilitythat it becomeshomozygous at or before the tth generation,and
y = lim, . Vt hat it ultimatelybecomeshomozygous.The chance that fixationwill occur preciselyat time t can be shown to be greatestwhen Ft-_ contains
only one representative f one of the alleles,and least whentheyarepresentn
equalnumbers.Hence
1 )t 2t ( )t 2t+1
^(~~~~~-a'^
) ) " -
1242424242424 P. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE
8/8/2019 A Mathematical Study of the Founder Principle
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A mathematicaltudy of thefounderprincipleof evolutionary eneticsmathematicaltudy of thefounderprincipleof evolutionary eneticsmathematicaltudy of thefounderprincipleof evolutionary eneticsmathematicaltudy of thefounderprincipleof evolutionary eneticsmathematicaltudy of thefounderprincipleof evolutionary eneticsmathematicaltudy of thefounderprincipleof evolutionary enetics
Suppose hat for some k, yk is known, then
Y = Yk+ (1 - yk)Yk+ + (1 - Y)(l - Yk+I)7k+2 +
[1 (1 )k+i 1 \ ( k+
>= +-) +(l-
-e-)
(14) ( 1 k+2
Y-k + (Y) [ ) 1 1([2eI)}] -
By computation, heprobabilitieshat a givenallele,sayA will be fixedbythe kth
generation avebeenobtainedupto k = 5, and aregiven n TableIV.
TABLE V
Probabilitiesof the fixationof A aftert generationsof randommating,for the
growingpopulation
k 1 2 3 4 5
i Yk .062500 .088997 .099550 .103808 .105536
Takingk = 5 in (14)leads to
1y > 0.105598,
which n thepresentcaseis only slightly arger hanI 75. Using the 62 technique
(Aitken,1926) a numericalapproximation o ly may be obtainedfrom the
termsgiven
in Table IV.Applying
the method toI72,
i73 andI74 gives
Iy = 0.10669, and applying it to I73, I74 and Iy5 gives Iy = 0.10672, which
is thereforeprobablycorrectto 5 decimalplaces.Acceptingthis the moments
of Y conditionalon absorptionnot havingtakenplace may be calculated rom
(10)and(13),
t2 = 0.06643, r/4= 0.00982, P2 = 2.23.
For a populationof 2t individualswhichhas evolved through t generationsof
randommating at constant size, the probabilityof fixation is approximately
1-(1-(1/2)t+1)' (Moran, 1962, Chapter 4), and this approaches zero very
quicklyas t increases.
Suppose hat for some k, yk is known, then
Y = Yk+ (1 - yk)Yk+ + (1 - Y)(l - Yk+I)7k+2 +
[1 (1 )k+i 1 \ ( k+
>= +-) +(l-
-e-)
(14) ( 1 k+2
Y-k + (Y) [ ) 1 1([2eI)}] -
By computation, heprobabilitieshat a givenallele,sayA will be fixedbythe kth
generation avebeenobtainedupto k = 5, and aregiven n TableIV.
TABLE V
Probabilitiesof the fixationof A aftert generationsof randommating,for the
growingpopulation
k 1 2 3 4 5
i Yk .062500 .088997 .099550 .103808 .105536
Takingk = 5 in (14)leads to
1y > 0.105598,
which n thepresentcaseis only slightly arger hanI 75. Using the 62 technique
(Aitken,1926) a numericalapproximation o ly may be obtainedfrom the
termsgiven
in Table IV.Applying
the method toI72,
i73 andI74 gives
Iy = 0.10669, and applying it to I73, I74 and Iy5 gives Iy = 0.10672, which
is thereforeprobablycorrectto 5 decimalplaces.Acceptingthis the moments
of Y conditionalon absorptionnot havingtakenplace may be calculated rom
(10)and(13),
t2 = 0.06643, r/4= 0.00982, P2 = 2.23.
For a populationof 2t individualswhichhas evolved through t generationsof
randommating at constant size, the probabilityof fixation is approximately
1-(1-(1/2)t+1)' (Moran, 1962, Chapter 4), and this approaches zero very
quicklyas t increases.
Suppose hat for some k, yk is known, then
Y = Yk+ (1 - yk)Yk+ + (1 - Y)(l - Yk+I)7k+2 +
[1 (1 )k+i 1 \ ( k+
>= +-) +(l-
-e-)
(14) ( 1 k+2
Y-k + (Y) [ ) 1 1([2eI)}] -
By computation, heprobabilitieshat a givenallele,sayA will be fixedbythe kth
generation avebeenobtainedupto k = 5, and aregiven n TableIV.
TABLE V
Probabilitiesof the fixationof A aftert generationsof randommating,for the
growingpopulation
k 1 2 3 4 5
i Yk .062500 .088997 .099550 .103808 .105536
Takingk = 5 in (14)leads to
1y > 0.105598,
which n thepresentcaseis only slightly arger hanI 75. Using the 62 technique
(Aitken,1926) a numericalapproximation o ly may be obtainedfrom the
termsgiven
in Table IV.Applying
the method toI72,
i73 andI74 gives
Iy = 0.10669, and applying it to I73, I74 and Iy5 gives Iy = 0.10672, which
is thereforeprobablycorrectto 5 decimalplaces.Acceptingthis the moments
of Y conditionalon absorptionnot havingtakenplace may be calculated rom
(10)and(13),
t2 = 0.06643, r/4= 0.00982, P2 = 2.23.
For a populationof 2t individualswhichhas evolved through t generationsof
randommating at constant size, the probabilityof fixation is approximately
1-(1-(1/2)t+1)' (Moran, 1962, Chapter 4), and this approaches zero very
quicklyas t increases.
Suppose hat for some k, yk is known, then
Y = Yk+ (1 - yk)Yk+ + (1 - Y)(l - Yk+I)7k+2 +
[1 (1 )k+i 1 \ ( k+
>= +-) +(l-
-e-)
(14) ( 1 k+2
Y-k + (Y) [ ) 1 1([2eI)}] -
By computation, heprobabilitieshat a givenallele,sayA will be fixedbythe kth
generation avebeenobtainedupto k = 5, and aregiven n TableIV.
TABLE V
Probabilitiesof the fixationof A aftert generationsof randommating,for the
growingpopulation
k 1 2 3 4 5
i Yk .062500 .088997 .099550 .103808 .105536
Takingk = 5 in (14)leads to
1y > 0.105598,
which n thepresentcaseis only slightly arger hanI 75. Using the 62 technique
(Aitken,1926) a numericalapproximation o ly may be obtainedfrom the
termsgiven
in Table IV.Applying
the method toI72,
i73 andI74 gives
Iy = 0.10669, and applying it to I73, I74 and Iy5 gives Iy = 0.10672, which
is thereforeprobablycorrectto 5 decimalplaces.Acceptingthis the moments
of Y conditionalon absorptionnot havingtakenplace may be calculated rom
(10)and(13),
t2 = 0.06643, r/4= 0.00982, P2 = 2.23.
For a populationof 2t individualswhichhas evolved through t generationsof
randommating at constant size, the probabilityof fixation is approximately
1-(1-(1/2)t+1)' (Moran, 1962, Chapter 4), and this approaches zero very
quicklyas t increases.
Suppose hat for some k, yk is known, then
Y = Yk+ (1 - yk)Yk+ + (1 - Y)(l - Yk+I)7k+2 +
[1 (1 )k+i 1 \ ( k+
>= +-) +(l-
-e-)
(14) ( 1 k+2
Y-k + (Y) [ ) 1 1([2eI)}] -
By computation, heprobabilitieshat a givenallele,sayA will be fixedbythe kth
generation avebeenobtainedupto k = 5, and aregiven n TableIV.
TABLE V
Probabilitiesof the fixationof A aftert generationsof randommating,for the
growingpopulation
k 1 2 3 4 5
i Yk .062500 .088997 .099550 .103808 .105536
Takingk = 5 in (14)leads to
1y > 0.105598,
which n thepresentcaseis only slightly arger hanI 75. Using the 62 technique
(Aitken,1926) a numericalapproximation o ly may be obtainedfrom the
termsgiven
in Table IV.Applying
the method toI72,
i73 andI74 gives
Iy = 0.10669, and applying it to I73, I74 and Iy5 gives Iy = 0.10672, which
is thereforeprobablycorrectto 5 decimalplaces.Acceptingthis the moments
of Y conditionalon absorptionnot havingtakenplace may be calculated rom
(10)and(13),
t2 = 0.06643, r/4= 0.00982, P2 = 2.23.
For a populationof 2t individualswhichhas evolved through t generationsof
randommating at constant size, the probabilityof fixation is approximately
1-(1-(1/2)t+1)' (Moran, 1962, Chapter 4), and this approaches zero very
quicklyas t increases.
Suppose hat for some k, yk is known, then
Y = Yk+ (1 - yk)Yk+ + (1 - Y)(l - Yk+I)7k+2 +
[1 (1 )k+i 1 \ ( k+
>= +-) +(l-
-e-)
(14) ( 1 k+2
Y-k + (Y) [ ) 1 1([2eI)}] -
By computation, heprobabilitieshat a givenallele,sayA will be fixedbythe kth
generation avebeenobtainedupto k = 5, and aregiven n TableIV.
TABLE V
Probabilitiesof the fixationof A aftert generationsof randommating,for the
growingpopulation
k 1 2 3 4 5
i Yk .062500 .088997 .099550 .103808 .105536
Takingk = 5 in (14)leads to
1y > 0.105598,
which n thepresentcaseis only slightly arger hanI 75. Using the 62 technique
(Aitken,1926) a numericalapproximation o ly may be obtainedfrom the
termsgiven
in Table IV.Applying
the method toI72,
i73 andI74 gives
Iy = 0.10669, and applying it to I73, I74 and Iy5 gives Iy = 0.10672, which
is thereforeprobablycorrectto 5 decimalplaces.Acceptingthis the moments
of Y conditionalon absorptionnot havingtakenplace may be calculated rom
(10)and(13),
t2 = 0.06643, r/4= 0.00982, P2 = 2.23.
For a populationof 2t individualswhichhas evolved through t generationsof
randommating at constant size, the probabilityof fixation is approximately
1-(1-(1/2)t+1)' (Moran, 1962, Chapter 4), and this approaches zero very
quicklyas t increases.
1252525252525
8/8/2019 A Mathematical Study of the Founder Principle
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4. A fullystochasticmodel
A simplefully stochasticmodelis obtainedby lettingthe numberof offspringof each individual be, not a constant,but a Poisson variable.Bartlett(1937,Formula 7b))obtained he variances f thenumbersof heterozygotesn successive
generations,(without conditioningon the population as a whole remaining
non-extinct).For the case where i) the Poissonmean s unityand hencethe mean
populationsize is constant, ii)the numberof generations ufficientlyargefor the
probability hat the heterozygousoffspringof a given individualwill not have
been eliminatedto be given by the asympoticformuladerivede.g. by Harris
(1963, p. 18),Formula9.5), and (iii) the founderpopulationso large that the
chanceof completeextinction s negligible,Bartlettalso showedhow the proba-
bility that the population should consist entirelyof homozygotes could becalculated.
In the remainder f this sectionI present ome numerical aluesrelating o the
resultsof threegenerationsof mating,for a population nitiatedby a singlein-
dividualandhavinga mean rate of increaseof 2, and for a population nitiated
by 8 individuals,and havinga mean rate of increaseof unity.If the numberof
offspringof each individuals a Poisson variablewith mean2, andthe offspringof a heterozygote re AA, Aa, aa withprobabilities1/4, 1/2, 1/4. Thetrivariate
stochasticprocessgiving he numbers f the three ypes n successive enerationss
a multi-type Galton-Watson process (Harris, 1963, Ch. 2) with generatingfunctions
f '(S, S2,S3)= exp2(sl - 1)
f2(sl,s2,s3) = exp2 s + + 3-
f3 (s1, s2,s3) = exp2s3- 1).
Takingthe generatingunctionfor Fo as s2, that for Ft may be obtainedbymultivariateunctional teration.Fromit, the probabilitieshatvariouscombina-
tions of classes will have no representativesmay be computed.The probabilityof completeextinction urns out to be 0.192975.Onmultiplyingup theremaining
probabilities,he probability hat a population,giventhat it is still in existence
after threegenerations,consists entirelyof AA's, or entirelyof homozygotes,
may be calculated.The comparable tationarypopulation s obtainedby takingthe mean numberof offspringas one instead of two, and startingwith eight
heterozygotes.n this case the chance of total extinction n F3 is much smaller,0.023558.In Table V a numberof probabilities elating o the F3's of various
models consideredare collectedtogether.
4. A fullystochasticmodel
A simplefully stochasticmodelis obtainedby lettingthe numberof offspringof each individual be, not a constant,but a Poisson variable.Bartlett(1937,Formula 7b))obtained he variances f thenumbersof heterozygotesn successive
generations,(without conditioningon the population as a whole remaining
non-extinct).For the case where i) the Poissonmean s unityand hencethe mean
populationsize is constant, ii)the numberof generations ufficientlyargefor the
probability hat the heterozygousoffspringof a given individualwill not have
been eliminatedto be given by the asympoticformuladerivede.g. by Harris
(1963, p. 18),Formula9.5), and (iii) the founderpopulationso large that the
chanceof completeextinction s negligible,Bartlettalso showedhow the proba-
bility that the population should consist entirelyof homozygotes could becalculated.
In the remainder f this sectionI present ome numerical aluesrelating o the
resultsof threegenerationsof mating,for a population nitiatedby a singlein-
dividualandhavinga mean rate of increaseof 2, and for a population nitiated
by 8 individuals,and havinga mean rate of increaseof unity.If the numberof
offspringof each individuals a Poisson variablewith mean2, andthe offspringof a heterozygote re AA, Aa, aa withprobabilities1/4, 1/2, 1/4. Thetrivariate
stochasticprocessgiving he numbers f the three ypes n successive enerationss
a multi-type Galton-Watson process (Harris, 1963, Ch. 2) with generatingfunctions
f '(S, S2,S3)= exp2(sl - 1)
f2(sl,s2,s3) = exp2 s + + 3-
f3 (s1, s2,s3) = exp2s3- 1).
Takingthe generatingunctionfor Fo as s2, that for Ft may be obtainedbymultivariateunctional teration.Fromit, the probabilitieshatvariouscombina-
tions of classes will have no representativesmay be computed.The probabilityof completeextinction urns out to be 0.192975.Onmultiplyingup theremaining
probabilities,he probability hat a population,giventhat it is still in existence
after threegenerations,consists entirelyof AA's, or entirelyof homozygotes,
may be calculated.The comparable tationarypopulation s obtainedby takingthe mean numberof offspringas one instead of two, and startingwith eight
heterozygotes.n this case the chance of total extinction n F3 is much smaller,0.023558.In Table V a numberof probabilities elating o the F3's of various
models consideredare collectedtogether.
4. A fullystochasticmodel
A simplefully stochasticmodelis obtainedby lettingthe numberof offspringof each individual be, not a constant,but a Poisson variable.Bartlett(1937,Formula 7b))obtained he variances f thenumbersof heterozygotesn successive
generations,(without conditioningon the population as a whole remaining
non-extinct).For the case where i) the Poissonmean s unityand hencethe mean
populationsize is constant, ii)the numberof generations ufficientlyargefor the
probability hat the heterozygousoffspringof a given individualwill not have
been eliminatedto be given by the asympoticformuladerivede.g. by Harris
(1963, p. 18),Formula9.5), and (iii) the founderpopulationso large that the
chanceof completeextinction s negligible,Bartlettalso showedhow the proba-
bility that the population should consist entirelyof homozygotes could becalculated.
In the remainder f this sectionI present ome numerical aluesrelating o the
resultsof threegenerationsof mating,for a population nitiatedby a singlein-
dividualandhavinga mean rate of increaseof 2, and for a population nitiated
by 8 individuals,and havinga mean rate of increaseof unity.If the numberof
offspringof each individuals a Poisson variablewith mean2, andthe offspringof a heterozygote re AA, Aa, aa withprobabilities1/4, 1/2, 1/4. Thetrivariate
stochasticprocessgiving he numbers f the three ypes n successive enerationss
a multi-type Galton-Watson process (Harris, 1963, Ch. 2) with generatingfunctions
f '(S, S2,S3)= exp2(sl - 1)
f2(sl,s2,s3) = exp2 s + + 3-
f3 (s1, s2,s3) = exp2s3- 1).
Takingthe generatingunctionfor Fo as s2, that for Ft may be obtainedbymultivariateunctional teration.Fromit, the probabilitieshatvariouscombina-
tions of classes will have no representativesmay be computed.The probabilityof completeextinction urns out to be 0.192975.Onmultiplyingup theremaining
probabilities,he probability hat a population,giventhat it is still in existence
after threegenerations,consists entirelyof AA's, or entirelyof homozygotes,
may be calculated.The comparable tationarypopulation s obtainedby takingthe mean numberof offspringas one instead of two, and startingwith eight
heterozygotes.n this case the chance of total extinction n F3 is much smaller,0.023558.In Table V a numberof probabilities elating o the F3's of various
models consideredare collectedtogether.
4. A fullystochasticmodel
A simplefully stochasticmodelis obtainedby lettingthe numberof offspringof each individual be, not a constant,but a Poisson variable.Bartlett(1937,Formula 7b))obtained he variances f thenumbersof heterozygotesn successive
generations,(without conditioningon the population as a whole remaining
non-extinct).For the case where i) the Poissonmean s unityand hencethe mean
populationsize is constant, ii)the numberof generations ufficientlyargefor the
probability hat the heterozygousoffspringof a given individualwill not have
been eliminatedto be given by the asympoticformuladerivede.g. by Harris
(1963, p. 18),Formula9.5), and (iii) the founderpopulationso large that the
chanceof completeextinction s negligible,Bartlettalso showedhow the proba-
bility that the population should consist entirelyof homozygotes could becalculated.
In the remainder f this sectionI present ome numerical aluesrelating o the
resultsof threegenerationsof mating,for a population nitiatedby a singlein-
dividualandhavinga mean rate of increaseof 2, and for a population nitiated
by 8 individuals,and havinga mean rate of increaseof unity.If the numberof
offspringof each individuals a Poisson variablewith mean2, andthe offspringof a heterozygote re AA, Aa, aa withprobabilities1/4, 1/2, 1/4. Thetrivariate
stochasticprocessgiving he numbers f the three ypes n successive enerationss
a multi-type Galton-Watson process (Harris, 1963, Ch. 2) with generatingfunctions
f '(S, S2,S3)= exp2(sl - 1)
f2(sl,s2,s3) = exp2 s + + 3-
f3 (s1, s2,s3) = exp2s3- 1).
Takingthe generatingunctionfor Fo as s2, that for Ft may be obtainedbymultivariateunctional teration.Fromit, the probabilitieshatvariouscombina-
tions of classes will have no representativesmay be computed.The probabilityof completeextinction urns out to be 0.192975.Onmultiplyingup theremaining
probabilities,he probability hat a population,giventhat it is still in existence
after threegenerations,consists entirelyof AA's, or entirelyof homozygotes,
may be calculated.The comparable tationarypopulation s obtainedby takingthe mean numberof offspringas one instead of two, and startingwith eight
heterozygotes.n this case the chance of total extinction n F3 is much smaller,0.023558.In Table V a numberof probabilities elating o the F3's of various
models consideredare collectedtogether.
4. A fullystochasticmodel
A simplefully stochasticmodelis obtainedby lettingthe numberof offspringof each individual be, not a constant,but a Poisson variable.Bartlett(1937,Formula 7b))obtained he variances f thenumbersof heterozygotesn successive
generations,(without conditioningon the population as a whole remaining
non-extinct).For the case where i) the Poissonmean s unityand hencethe mean
populationsize is constant, ii)the numberof generations ufficientlyargefor the
probability hat the heterozygousoffspringof a given individualwill not have
been eliminatedto be given by the asympoticformuladerivede.g. by Harris
(1963, p. 18),Formula9.5), and (iii) the founderpopulationso large that the
chanceof completeextinction s negligible,Bartlettalso showedhow the proba-
bility that the population should consist entirelyof homozygotes could becalculated.
In the remainder f this sectionI present ome numerical aluesrelating o the
resultsof threegenerationsof mating,for a population nitiatedby a singlein-
dividualandhavinga mean rate of increaseof 2, and for a population nitiated
by 8 individuals,and havinga mean rate of increaseof unity.If the numberof
offspringof each individuals a Poisson variablewith mean2, andthe offspringof a heterozygote re AA, Aa, aa withprobabilities1/4, 1/2, 1/4. Thetrivariate
stochasticprocessgiving he numbers f the three ypes n successive enerationss
a multi-type Galton-Watson process (Harris, 1963, Ch. 2) with generatingfunctions
f '(S, S2,S3)= exp2(sl - 1)
f2(sl,s2,s3) = exp2 s + + 3-
f3 (s1, s2,s3) = exp2s3- 1).
Takingthe generatingunctionfor Fo as s2, that for Ft may be obtainedbymultivariateunctional teration.Fromit, the probabilitieshatvariouscombina-
tions of classes will have no representativesmay be computed.The probabilityof completeextinction urns out to be 0.192975.Onmultiplyingup theremaining
probabilities,he probability hat a population,giventhat it is still in existence
after threegenerations,consists entirelyof AA's, or entirelyof homozygotes,
may be calculated.The comparable tationarypopulation s obtainedby takingthe mean numberof offspringas one instead of two, and startingwith eight
heterozygotes.n this case the chance of total extinction n F3 is much smaller,0.023558.In Table V a numberof probabilities elating o the F3's of various
models consideredare collectedtogether.
4. A fullystochasticmodel
A simplefully stochasticmodelis obtainedby lettingthe numberof offspringof each individual be, not a constant,but a Poisson variable.Bartlett(1937,Formula 7b))obtained he variances f thenumbersof heterozygotesn successive
generations,(without conditioningon the population as a whole remaining
non-extinct).For the case where i) the Poissonmean s unityand hencethe mean
populationsize is constant, ii)the numberof generations ufficientlyargefor the
probability hat the heterozygousoffspringof a given individualwill not have
been eliminatedto be given by the asympoticformuladerivede.g. by Harris
(1963, p. 18),Formula9.5), and (iii) the founderpopulationso large that the
chanceof completeextinction s negligible,Bartlettalso showedhow the proba-
bility that the population should consist entirelyof homozygotes could becalculated.
In the remainder f this sectionI present ome numerical aluesrelating o the
resultsof threegenerationsof mating,for a population nitiatedby a singlein-
dividualandhavinga mean rate of increaseof 2, and for a population nitiated
by 8 individuals,and havinga mean rate of increaseof unity.If the numberof
offspringof each individuals a Poisson variablewith mean2, andthe offspringof a heterozygote re AA, Aa, aa withprobabilities1/4, 1/2, 1/4. Thetrivariate
stochasticprocessgiving he numbers f the three ypes n successive enerationss
a multi-type Galton-Watson process (Harris, 1963, Ch. 2) with generatingfunctions
f '(S, S2,S3)= exp2(sl - 1)
f2(sl,s2,s3) = exp2 s + + 3-
f3 (s1, s2,s3) = exp2s3- 1).
Takingthe generatingunctionfor Fo as s2, that for Ft may be obtainedbymultivariateunctional teration.Fromit, the probabilitieshatvariouscombina-
tions of classes will have no representativesmay be computed.The probabilityof completeextinction urns out to be 0.192975.Onmultiplyingup theremaining
probabilities,he probability hat a population,giventhat it is still in existence
after threegenerations,consists entirelyof AA's, or entirelyof homozygotes,
may be calculated.The comparable tationarypopulation s obtainedby takingthe mean numberof offspringas one instead of two, and startingwith eight
heterozygotes.n this case the chance of total extinction n F3 is much smaller,0.023558.In Table V a numberof probabilities elating o the F3's of various
models consideredare collectedtogether.
1262626262626 P. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE. HOLGATE
8/8/2019 A Mathematical Study of the Founder Principle
http://slidepdf.com/reader/full/a-mathematical-study-of-the-founder-principle 14/15
A mathematicaltudyof thefounderprincipleof evolutionary enetics 127
Acknowledgements
I am grateful o Mr. J. G. Skellam or severalhelpfulsuggestionsmadein thecourse of this work,andto Mr. K. Lakhaniand Mr. D. Spalding or assistancein computation.
TABLEV
Some fixationand eliminationprobabilitiesor variousmodelsconsidered.Forstochasticgrowth models probabilitiesare conditionalon completeextinction
not havingoccurred.
ProbabilityhatF3 consistsentirelyof:(i) AA's (ii) homozygotes
Growingpopulation
Deterministiceproduction 0.0838 0.4835
Stochastic eproduction 0.1580 0.4555
Stationary opulation
Deterministiceproduction 0.0013 0.3436Stochastic eproduction 0.0645 0.3222
A mathematicaltudyof thefounderprincipleof evolutionary enetics 127
Acknowledgements
I am grateful o Mr. J. G. Skellam or severalhelpfulsuggestionsmadein thecourse of this work,andto Mr. K. Lakhaniand Mr. D. Spalding or assistancein computation.
TABLEV
Some fixationand eliminationprobabilitiesor variousmodelsconsidered.Forstochasticgrowth models probabilitiesare conditionalon completeextinction
not havingoccurred.
ProbabilityhatF3 consistsentirelyof:(i) AA's (ii) homozygotes
Growingpopulation
Deterministiceproduction 0.0838 0.4835
Stochastic eproduction 0.1580 0.4555
Stationary opulation
Deterministiceproduction 0.0013 0.3436Stochastic eproduction 0.0645 0.3222
A mathematicaltudyof thefounderprincipleof evolutionary enetics 127
Acknowledgements
I am grateful o Mr. J. G. Skellam or severalhelpfulsuggestionsmadein thecourse of this work,andto Mr. K. Lakhaniand Mr. D. Spalding or assistancein computation.
TABLEV
Some fixationand eliminationprobabilitiesor variousmodelsconsidered.Forstochasticgrowth models probabilitiesare conditionalon completeextinction
not havingoccurred.
ProbabilityhatF3 consistsentirelyof:(i) AA's (ii) homozygotes
Growingpopulation
Deterministiceproduction 0.0838 0.4835
Stochastic eproduction 0.1580 0.4555
Stationary opulation
Deterministiceproduction 0.0013 0.3436Stochastic eproduction 0.0645 0.3222
A mathematicaltudyof thefounderprincipleof evolutionary enetics 127
Acknowledgements
I am grateful o Mr. J. G. Skellam or severalhelpfulsuggestionsmadein thecourse of this work,andto Mr. K. Lakhaniand Mr. D. Spalding or assistancein computation.
TABLEV
Some fixationand eliminationprobabilitiesor variousmodelsconsidered.Forstochasticgrowth models probabilitiesare conditionalon completeextinction
not havingoccurred.
ProbabilityhatF3 consistsentirelyof:(i) AA's (ii) homozygotes
Growingpopulation
Deterministiceproduction 0.0838 0.4835
Stochastic eproduction 0.1580 0.4555
Stationary opulation
Deterministiceproduction 0.0013 0.3436Stochastic eproduction 0.0645 0.3222
A mathematicaltudyof thefounderprincipleof evolutionary enetics 127
Acknowledgements
I am grateful o Mr. J. G. Skellam or severalhelpfulsuggestionsmadein thecourse of this work,andto Mr. K. Lakhaniand Mr. D. Spalding or assistancein computation.
TABLEV
Some fixationand eliminationprobabilitiesor variousmodelsconsidered.Forstochasticgrowth models probabilitiesare conditionalon completeextinction
not havingoccurred.
ProbabilityhatF3 consistsentirelyof:(i) AA's (ii) homozygotes
Growingpopulation
Deterministiceproduction 0.0838 0.4835
Stochastic eproduction 0.1580 0.4555
Stationary opulation
Deterministiceproduction 0.0013 0.3436Stochastic eproduction 0.0645 0.3222
A mathematicaltudyof thefounderprincipleof evolutionary enetics 127
Acknowledgements
I am grateful o Mr. J. G. Skellam or severalhelpfulsuggestionsmadein thecourse of this work,andto Mr. K. Lakhaniand Mr. D. Spalding or assistancein computation.
TABLEV
Some fixationand eliminationprobabilitiesor variousmodelsconsidered.Forstochasticgrowth models probabilitiesare conditionalon completeextinction
not havingoccurred.
ProbabilityhatF3 consistsentirelyof:(i) AA's (ii) homozygotes
Growingpopulation
Deterministiceproduction 0.0838 0.4835
Stochastic eproduction 0.1580 0.4555
Stationary opulation
Deterministiceproduction 0.0013 0.3436Stochastic eproduction 0.0645 0.3222
References
AITKEN, . C. (1926) On Bernoulli's numerical solution of algebraic equations.Proc.Roy. Soc. Edinburgh 6, 289-305.
BARTLETT,. S. (1937) Deviations from expectedfrequency n the theory of inbreedingJ. Genet. 35, 83-87.
(1960) Stochastic Population Models in Biology and Epidemiology.Methuen,London.
CAIN,A. J. ANDCURREY,J. D. (1963a) Area effects in Cepaea. Philos. Trans. Roy. Soc. B.246, 1-81.
(1936b) The causes of area effects. Heredity 18, 466-471.
CRAMER,. (1946) MathematicalMethodsof Statistics. PrincetonUniv. Press.
DOBZHANSKY, . AND PAVLOVSKY, . (1957) An experimental study of the interactionbetweengenetic drift and natural selection. Evolution11, 311-319.
DOOB, . L. (1953) StochasticProcesses. Wiley, New York.
FELLER,. (1951) Diffusion processes in genetics. Proc. Second BerkeleySymposiumonMathematicalStatistics andProbability,227-246.
GOODHART,. B. (1962) Variationin a colony of the snail CepaeaNemoralis (L.) J.Anim.Ecol. 31, 207-237.
(1963) "Area effects"and non-adaptivevariationbetweenpopulationsof Cepaea
(mollusca). Heredity 18, 459-465.HARRIS, . (1963) BranchingProcesses. Springer,Berlin.
References
AITKEN, . C. (1926) On Bernoulli's numerical solution of algebraic equations.Proc.Roy. Soc. Edinburgh 6, 289-305.
BARTLETT,. S. (1937) Deviations from expectedfrequency n the theory of inbreedingJ. Genet. 35, 83-87.
(1960) Stochastic Population Models in Biology and Epidemiology.Methuen,London.
CAIN,A. J. ANDCURREY,J. D. (1963a) Area effects in Cepaea. Philos. Trans. Roy. Soc. B.246, 1-81.
(1936b) The causes of area effects. Heredity 18, 466-471.
CRAMER,. (1946) MathematicalMethodsof Statistics. PrincetonUniv. Press.
DOBZHANSKY, . AND PAVLOVSKY, . (1957) An experimental study of the interactionbetweengenetic drift and natural selection. Evolution11, 311-319.
DOOB, . L. (1953) StochasticProcesses. Wiley, New York.
FELLER,. (1951) Diffusion processes in genetics. Proc. Second BerkeleySymposiumonMathematicalStatistics andProbability,227-246.
GOODHART,. B. (1962) Variationin a colony of the snail CepaeaNemoralis (L.) J.Anim.Ecol. 31, 207-237.
(1963) "Area effects"and non-adaptivevariationbetweenpopulationsof Cepaea
(mollusca). Heredity 18, 459-465.HARRIS, . (1963) BranchingProcesses. Springer,Berlin.
References
AITKEN, . C. (1926) On Bernoulli's numerical solution of algebraic equations.Proc.Roy. Soc. Edinburgh 6, 289-305.
BARTLETT,. S. (1937) Deviations from expectedfrequency n the theory of inbreedingJ. Genet. 35, 83-87.
(1960) Stochastic Population Models in Biology and Epidemiology.Methuen,London.
CAIN,A. J. ANDCURREY,J. D. (1963a) Area effects in Cepaea. Philos. Trans. Roy. Soc. B.246, 1-81.
(1936b) The causes of area effects. Heredity 18, 466-471.
CRAMER,. (1946) MathematicalMethodsof Statistics. PrincetonUniv. Press.
DOBZHANSKY, . AND PAVLOVSKY, . (1957) An experimental study of the interactionbetweengenetic drift and natural selection. Evolution11, 311-319.
DOOB, . L. (1953) StochasticProcesses. Wiley, New York.
FELLER,. (1951) Diffusion processes in genetics. Proc. Second BerkeleySymposiumonMathematicalStatistics andProbability,227-246.
GOODHART,. B. (1962) Variationin a colony of the snail CepaeaNemoralis (L.) J.Anim.Ecol. 31, 207-237.
(1963) "Area effects"and non-adaptivevariationbetweenpopulationsof Cepaea
(mollusca). Heredity 18, 459-465.HARRIS, . (1963) BranchingProcesses. Springer,Berlin.
References
AITKEN, . C. (1926) On Bernoulli's numerical solution of algebraic equations.Proc.Roy. Soc. Edinburgh 6, 289-305.
BARTLETT,. S. (1937) Deviations from expectedfrequency n the theory of inbreedingJ. Genet. 35, 83-87.
(1960) Stochastic Population Models in Biology and Epidemiology.Methuen,London.
CAIN,A. J. ANDCURREY,J. D. (1963a) Area effects in Cepaea. Philos. Trans. Roy. Soc. B.246, 1-81.
(1936b) The causes of area effects. Heredity 18, 466-471.
CRAMER,. (1946) MathematicalMethodsof Statistics. PrincetonUniv. Press.
DOBZHANSKY, . AND PAVLOVSKY, . (1957) An experimental study of the interactionbetweengenetic drift and natural selection. Evolution11, 311-319.
DOOB, . L. (1953) StochasticProcesses. Wiley, New York.
FELLER,. (1951) Diffusion processes in genetics. Proc. Second BerkeleySymposiumonMathematicalStatistics andProbability,227-246.
GOODHART,. B. (1962) Variationin a colony of the snail CepaeaNemoralis (L.) J.Anim.Ecol. 31, 207-237.
(1963) "Area effects"and non-adaptivevariationbetweenpopulationsof Cepaea
(mollusca). Heredity 18, 459-465.HARRIS, . (1963) BranchingProcesses. Springer,Berlin.
References
AITKEN, . C. (1926) On Bernoulli's numerical solution of algebraic equations.Proc.Roy. Soc. Edinburgh 6, 289-305.
BARTLETT,. S. (1937) Deviations from expectedfrequency n the theory of inbreedingJ. Genet. 35, 83-87.
(1960) Stochastic Population Models in Biology and Epidemiology.Methuen,London.
CAIN,A. J. ANDCURREY,J. D. (1963a) Area effects in Cepaea. Philos. Trans. Roy. Soc. B.246, 1-81.
(1936b) The causes of area effects. Heredity 18, 466-471.
CRAMER,. (1946) MathematicalMethodsof Statistics. PrincetonUniv. Press.
DOBZHANSKY, . AND PAVLOVSKY, . (1957) An experimental study of the interactionbetweengenetic drift and natural selection. Evolution11, 311-319.
DOOB, . L. (1953) StochasticProcesses. Wiley, New York.
FELLER,. (1951) Diffusion processes in genetics. Proc. Second BerkeleySymposiumonMathematicalStatistics andProbability,227-246.
GOODHART,. B. (1962) Variationin a colony of the snail CepaeaNemoralis (L.) J.Anim.Ecol. 31, 207-237.
(1963) "Area effects"and non-adaptivevariationbetweenpopulationsof Cepaea
(mollusca). Heredity 18, 459-465.HARRIS, . (1963) BranchingProcesses. Springer,Berlin.
References
AITKEN, . C. (1926) On Bernoulli's numerical solution of algebraic equations.Proc.Roy. Soc. Edinburgh 6, 289-305.
BARTLETT,. S. (1937) Deviations from expectedfrequency n the theory of inbreedingJ. Genet. 35, 83-87.
(1960) Stochastic Population Models in Biology and Epidemiology.Methuen,London.
CAIN,A. J. ANDCURREY,J. D. (1963a) Area effects in Cepaea. Philos. Trans. Roy. Soc. B.246, 1-81.
(1936b) The causes of area effects. Heredity 18, 466-471.
CRAMER,. (1946) MathematicalMethodsof Statistics. PrincetonUniv. Press.
DOBZHANSKY, . AND PAVLOVSKY, . (1957) An experimental study of the interactionbetweengenetic drift and natural selection. Evolution11, 311-319.
DOOB, . L. (1953) StochasticProcesses. Wiley, New York.
FELLER,. (1951) Diffusion processes in genetics. Proc. Second BerkeleySymposiumonMathematicalStatistics andProbability,227-246.
GOODHART,. B. (1962) Variationin a colony of the snail CepaeaNemoralis (L.) J.Anim.Ecol. 31, 207-237.
(1963) "Area effects"and non-adaptivevariationbetweenpopulationsof Cepaea
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KIMURA, . (1964)Diffusionmodelsin populationgenetics.J. Appl.Prob.1177-232.
KOLMOGOROV,. (1938), Zur Losung einer biologischenAufgabe. Izvestianaukno-issedo-
vatel'skogo Instituta Matematiki i Mechanikipri TomskomGosudarstvennomUniversitete2,1-6 (German),7-12 (Russian).
Li, C. C. (1955)PopulationGenetics.Chicago Univ. Press.
LOgVE,M. (1963) ProbabilityTheory.3rd Ed. Van Nostrand, New York.
MAYR, . (1942), Systematicsandthe Originof Species.ColumbiaUniv. Press.
(1963) AnimalSpeciesandEvolution.Harvardand Oxford Univ. Presses.
MODE,C. J. (1964) Some branching processes and their application to population
genetics(Abstract).Biometrics20, 663.
MORAN,. A. P. (1962) Statistical Processesof EvolutionaryTheory.OxfordUniv. Press.
RAO,K. R. ANDKENDALL,. G. (1950) On the generalisedsecond limit theoremin the
calculus of probabilities. Biometrika37, 224-230.
WRIGHT,S.1964) Stochasticprocessesin evolution. In StochasticModels nMedicineand
Biology,ed. J.
Gurland,Wisconsin Univ. Press.
128 P. HOLGATE
KIMURA, . (1964)Diffusionmodelsin populationgenetics.J. Appl.Prob.1177-232.
KOLMOGOROV,. (1938), Zur Losung einer biologischenAufgabe. Izvestianaukno-issedo-
vatel'skogo Instituta Matematiki i Mechanikipri TomskomGosudarstvennomUniversitete2,1-6 (German),7-12 (Russian).
Li, C. C. (1955)PopulationGenetics.Chicago Univ. Press.
LOgVE,M. (1963) ProbabilityTheory.3rd Ed. Van Nostrand, New York.
MAYR, . (1942), Systematicsandthe Originof Species.ColumbiaUniv. Press.
(1963) AnimalSpeciesandEvolution.Harvardand Oxford Univ. Presses.
MODE,C. J. (1964) Some branching processes and their application to population
genetics(Abstract).Biometrics20, 663.
MORAN,. A. P. (1962) Statistical Processesof EvolutionaryTheory.OxfordUniv. Press.
RAO,K. R. ANDKENDALL,. G. (1950) On the generalisedsecond limit theoremin the
calculus of probabilities. Biometrika37, 224-230.
WRIGHT,S.1964) Stochasticprocessesin evolution. In StochasticModels nMedicineand
Biology,ed. J.
Gurland,Wisconsin Univ. Press.
128 P. HOLGATE
KIMURA, . (1964)Diffusionmodelsin populationgenetics.J. Appl.Prob.1177-232.
KOLMOGOROV,. (1938), Zur Losung einer biologischenAufgabe. Izvestianaukno-issedo-
vatel'skogo Instituta Matematiki i Mechanikipri TomskomGosudarstvennomUniversitete2,1-6 (German),7-12 (Russian).
Li, C. C. (1955)PopulationGenetics.Chicago Univ. Press.
LOgVE,M. (1963) ProbabilityTheory.3rd Ed. Van Nostrand, New York.
MAYR, . (1942), Systematicsandthe Originof Species.ColumbiaUniv. Press.
(1963) AnimalSpeciesandEvolution.Harvardand Oxford Univ. Presses.
MODE,C. J. (1964) Some branching processes and their application to population
genetics(Abstract).Biometrics20, 663.
MORAN,. A. P. (1962) Statistical Processesof EvolutionaryTheory.OxfordUniv. Press.
RAO,K. R. ANDKENDALL,. G. (1950) On the generalisedsecond limit theoremin the
calculus of probabilities. Biometrika37, 224-230.
WRIGHT,S.1964) Stochasticprocessesin evolution. In StochasticModels nMedicineand
Biology,ed. J.
Gurland,Wisconsin Univ. Press.
128 P. HOLGATE
KIMURA, . (1964)Diffusionmodelsin populationgenetics.J. Appl.Prob.1177-232.
KOLMOGOROV,. (1938), Zur Losung einer biologischenAufgabe. Izvestianaukno-issedo-
vatel'skogo Instituta Matematiki i Mechanikipri TomskomGosudarstvennomUniversitete2,1-6 (German),7-12 (Russian).
Li, C. C. (1955)PopulationGenetics.Chicago Univ. Press.
LOgVE,M. (1963) ProbabilityTheory.3rd Ed. Van Nostrand, New York.
MAYR, . (1942), Systematicsandthe Originof Species.ColumbiaUniv. Press.
(1963) AnimalSpeciesandEvolution.Harvardand Oxford Univ. Presses.
MODE,C. J. (1964) Some branching processes and their application to population
genetics(Abstract).Biometrics20, 663.
MORAN,. A. P. (1962) Statistical Processesof EvolutionaryTheory.OxfordUniv. Press.
RAO,K. R. ANDKENDALL,. G. (1950) On the generalisedsecond limit theoremin the
calculus of probabilities. Biometrika37, 224-230.
WRIGHT,S.1964) Stochasticprocessesin evolution. In StochasticModels nMedicineand
Biology,ed. J.
Gurland,Wisconsin Univ. Press.
128 P. HOLGATE
KIMURA, . (1964)Diffusionmodelsin populationgenetics.J. Appl.Prob.1177-232.
KOLMOGOROV,. (1938), Zur Losung einer biologischenAufgabe. Izvestianaukno-issedo-
vatel'skogo Instituta Matematiki i Mechanikipri TomskomGosudarstvennomUniversitete2,1-6 (German),7-12 (Russian).
Li, C. C. (1955)PopulationGenetics.Chicago Univ. Press.
LOgVE,M. (1963) ProbabilityTheory.3rd Ed. Van Nostrand, New York.
MAYR, . (1942), Systematicsandthe Originof Species.ColumbiaUniv. Press.
(1963) AnimalSpeciesandEvolution.Harvardand Oxford Univ. Presses.
MODE,C. J. (1964) Some branching processes and their application to population
genetics(Abstract).Biometrics20, 663.
MORAN,. A. P. (1962) Statistical Processesof EvolutionaryTheory.OxfordUniv. Press.
RAO,K. R. ANDKENDALL,. G. (1950) On the generalisedsecond limit theoremin the
calculus of probabilities. Biometrika37, 224-230.
WRIGHT,S.1964) Stochasticprocessesin evolution. In StochasticModels nMedicineand
Biology,ed. J.
Gurland,Wisconsin Univ. Press.
128 P. HOLGATE
KIMURA, . (1964)Diffusionmodelsin populationgenetics.J. Appl.Prob.1177-232.
KOLMOGOROV,. (1938), Zur Losung einer biologischenAufgabe. Izvestianaukno-issedo-
vatel'skogo Instituta Matematiki i Mechanikipri TomskomGosudarstvennomUniversitete2,1-6 (German),7-12 (Russian).
Li, C. C. (1955)PopulationGenetics.Chicago Univ. Press.
LOgVE,M. (1963) ProbabilityTheory.3rd Ed. Van Nostrand, New York.
MAYR, . (1942), Systematicsandthe Originof Species.ColumbiaUniv. Press.
(1963) AnimalSpeciesandEvolution.Harvardand Oxford Univ. Presses.
MODE,C. J. (1964) Some branching processes and their application to population
genetics(Abstract).Biometrics20, 663.
MORAN,. A. P. (1962) Statistical Processesof EvolutionaryTheory.OxfordUniv. Press.
RAO,K. R. ANDKENDALL,. G. (1950) On the generalisedsecond limit theoremin the
calculus of probabilities. Biometrika37, 224-230.
WRIGHT,S.1964) Stochasticprocessesin evolution. In StochasticModels nMedicineand
Biology,ed. J.
Gurland,Wisconsin Univ. Press.