CHM102

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    CHEM106: Assessment 4Wave Functions and Probability

    Answer ey

    1! "e#ine t$e com%le& con'u(ate o# t$e #ollowin( #unctions!

    )$e com%le& con'u(ate #or a com%le& number * + a , ib is de#ined as *- + a − ib! .n

    (eneral/ to #ind t$e com%le& con'u(ate o# any #unction/ all we need to do is toreverse t$e si(n o# t$e ima(inary com%onent!

    A!   ibZ    += 3*

    !ix

    e xf    =)(*  

    C!   )2sin()(*  x xf    = / noticin( t$at #or a real #unction/ )()(

    * xf  xf    =

    ! W$at are t$e re2uirements #or an acce%table wave#unction3

    ince ΨΨ=Ψ  *2

     re%resents t$e %robability density #or #indin( t$e %article/ t$e

     wave#unctionΨ itsel# must meet t$e #ollowin( re2uirements: 51 #inite 5or2uadratically inte(rable7 5 sin(le valued7 and 58 continuous!

    8! W$ic$ o# t$e #ollowin( is an acce%table wave #unction over t$e indicated interval3

    A!∞≤≤  xwith

     x0

    1

     x

    1

     is not an acce%table wave#unction since it a%%roac$es in#inity as & + 0!

    !   2cos( x )   with   − ∞ ≤ x ≤ 0  2cos( x ) is an acce%table wave#unction since it meets all t$ree re2uirements listedin 2uestion in t$e s%eci#ied domain!

    C!   ∞≤≤∞−−  xwithe   x

     xe−

     is not an acce%table wave#unction since it a%%roac$es in#inity as∞−approaches x  !

    4! W$ic$ o# t$e #ollowin( #unctions are normali9able over t$e indicated intervals3ormali9e t$ose #unctions t$at can be normali9ed! 5Hint: .n normali9in(

     wave#unctions/ t$e inte(ration is over all s%ace in w$ic$ t$e wave #unction isde#ined!

    A!   π φ φ   φ 

    20)(   ≤≤=   −ief 

    )$e #unction is #inite everyw$ere/ and t$us normali9able!

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    ;iven

    π φ φ φ φ φ φ   π 

    π π 

    φ φ 

    π 

    2)()(  2

    0

    2

    0

    2

    0

    2

    0

    * ===== ∫ ∫ ∫   −+ ddeedf f  M    ii

    /

    t$e normali9ation constant is  M 

    1

    !

    )$us/ t$e normali9ed #unction is

    φ 

    π φ    i N    ef 

      −=2

    1)(

    !

    !  ∞≤≤∞−=   xwithe xf    x2)(

    )$e #unction xe xf    2)(   =

     is in#inite at ∞= x / and t$us not normali9able!

    C! L xwith x

     L xf    ≤≤=   0)

    2sin()(  π 

    )$e #unction is #inite everyw$ere/ and t$us normali9able!

    ;iven

     xd x L

     xd x L

     x L

     xd xf  xf  M 

     L L L

    ∫ ∫ ∫    ===0

    2

    00

    * )2(sin)

    2sin()

    2sin()()(

      π π π 

    /

    loo< u% t$e inte(ration table/ and #ind t$at

    )2sin(4

    1

    2

    1)(sin

    2  x x xd x   α α 

    α    −=∫ !

    )$us/ 2)]0sin()

    4[sin(

    82)

    4sin(

    82

    10

     L L

     L

     L L x

     L

     L x M 

      L=−−=−=

      π 

    π 

    π 

    π  !

    )$e normali9ation constant is

     M 

    1

    !

    )$us/ t$e normali9ed #unction is)

    2sin(

    2)(   x

     L L xf  N 

    π =

    !

    =! Consider t$e #ollowin( normali9ed wave#unction)

    2

    3cos(

    1)(   x

     L L x

      π ψ    =

    / #or a

    one>dimensional system con#ined in t$e re(ion  L x L   ≤≤− !

    A. Calculate t$e %robability t$at t$e %article will be #ound in t$e re(ion between & + 0

    and & + ?@!

     xd x L L

     xd x x P L L

    ∫ ∫    = ==2/

    0

    22/

    0

    *)

    2

    3(cos

    1)()(

      π ψ ψ 

    ?oo< u% t$e inte(ration table/ and #ind t$at

    )2sin(4

    1

    2

    1)(cos

    2  x x xd x   α α 

    α    +=∫ !

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