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Stereological formulas 1 AREA FRACTION FRACTIONATOR ............................................................................................................................................................................. 3 CAVALIERI ESTIMATOR ............................................................................................................................................................................................. 4 COMBINED POINT INTERCEPT.................................................................................................................................................................................. 6 CONNECTIVITY ASSAY .............................................................................................................................................................................................. 7 CYCLOIDS FOR LV ..................................................................................................................................................................................................... 8 CYCLOIDS FOR SV ................................................................................................................................................................................................... 10 DISCRETE VERTICAL ROTATOR ............................................................................................................................................................................... 12 FRACTIONATOR...................................................................................................................................................................................................... 13 ISOTROPIC FAKIR.................................................................................................................................................................................................... 17 ISOTROPIC VIRTUAL PLANES .................................................................................................................................................................................. 18 IUR PLANES OPTICAL FRACTIONATOR .................................................................................................................................................................... 21 L-CYCLOID OPTICAL FRACTIONATOR ...................................................................................................................................................................... 22 MERZ ..................................................................................................................................................................................................................... 23

ย ยท Stereological formulas . 25 . OPTICAL FRACTIONATOR . Estimate of total number of particles (N) โ„Ž. ๐‘๐‘= ๐‘„๐‘„ โˆ’. ๐‘ก๐‘ก. 1 ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ. 1 ๐‘Ž๐‘Ž๐‘Ž

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Page 1: ย ยท Stereological formulas . 25 . OPTICAL FRACTIONATOR . Estimate of total number of particles (N) โ„Ž. ๐‘๐‘= ๐‘„๐‘„ โˆ’. ๐‘ก๐‘ก. 1 ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ. 1 ๐‘Ž๐‘Ž๐‘Ž

Stereological formulas

1

AREA FRACTION FRACTIONATOR ............................................................................................................................................................................. 3

CAVALIERI ESTIMATOR ............................................................................................................................................................................................. 4

COMBINED POINT INTERCEPT .................................................................................................................................................................................. 6

CONNECTIVITY ASSAY .............................................................................................................................................................................................. 7

CYCLOIDS FOR LV ..................................................................................................................................................................................................... 8

CYCLOIDS FOR SV ................................................................................................................................................................................................... 10

DISCRETE VERTICAL ROTATOR ............................................................................................................................................................................... 12

FRACTIONATOR ...................................................................................................................................................................................................... 13

ISOTROPIC FAKIR .................................................................................................................................................................................................... 17

ISOTROPIC VIRTUAL PLANES .................................................................................................................................................................................. 18

IUR PLANES OPTICAL FRACTIONATOR .................................................................................................................................................................... 21

L-CYCLOID OPTICAL FRACTIONATOR ...................................................................................................................................................................... 22

MERZ ..................................................................................................................................................................................................................... 23

Page 2: ย ยท Stereological formulas . 25 . OPTICAL FRACTIONATOR . Estimate of total number of particles (N) โ„Ž. ๐‘๐‘= ๐‘„๐‘„ โˆ’. ๐‘ก๐‘ก. 1 ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ. 1 ๐‘Ž๐‘Ž๐‘Ž

Stereological formulas

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NUCLEATOR ........................................................................................................................................................................................................... 24

OPTICAL FRACTIONATOR ....................................................................................................................................................................................... 25

OPTICAL ROTATOR ................................................................................................................................................................................................. 29

PETRIMETRICS ........................................................................................................................................................................................................ 31

PHYSICAL FRACTIONATOR ...................................................................................................................................................................................... 32

PLANAR ROTATOR .................................................................................................................................................................................................. 33

POINT SAMPLED INTERCEPT .................................................................................................................................................................................. 35

SIZE DISTRIBUTION ................................................................................................................................................................................................. 36

SPACEBALLS ........................................................................................................................................................................................................... 38

SURFACE-WEIGHTED STAR VOLUME ...................................................................................................................................................................... 40

SURFACTOR ........................................................................................................................................................................................................... 41

SV-CYCLOID FRACTIONATOR .................................................................................................................................................................................. 42

VERTICAL SPATIAL GRID ......................................................................................................................................................................................... 43

WEIBEL................................................................................................................................................................................................................... 44

Page 3: ย ยท Stereological formulas . 25 . OPTICAL FRACTIONATOR . Estimate of total number of particles (N) โ„Ž. ๐‘๐‘= ๐‘„๐‘„ โˆ’. ๐‘ก๐‘ก. 1 ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ. 1 ๐‘Ž๐‘Ž๐‘Ž

Stereological formulas

3

AREA FRACTION FRACTIONATOR

Estimated volume fraction (๐‘‰๐‘‰๐‘ฃ๐‘ฃ๏ฟฝ )

๐‘‰๐‘‰๐‘ฃ๐‘ฃ๏ฟฝ (๐‘Œ๐‘Œ, ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ) =โˆ‘ ๐‘ƒ๐‘ƒ(๐‘Œ๐‘Œ)๐‘–๐‘–๐‘š๐‘š๐‘–๐‘–=1

โˆ‘ ๐‘ƒ๐‘ƒ(๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ)๐‘–๐‘–๐‘š๐‘š๐‘–๐‘–=1

P(ref) Points hitting reference volume

Y Sub-region P(Y) Points hitting sub-region

Estimated area (๏ฟฝฬ‚๏ฟฝ๐ด)

๏ฟฝฬ‚๏ฟฝ๐ด =1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.๐‘Ž๐‘Ž(๐‘๐‘).๐‘ƒ๐‘ƒ(๐‘Œ๐‘Œ๐‘–๐‘–)

asf Area sampling fraction a(p) Area associated with a point

R e f e r e n c e s Howard, C. V., & Reed, M. G. (1998). Unbiased Stereology, Three-Dimensional Measurement in Microscopy (pp. 170โ€“172). Milton Park, England: BIOS Scientific Publishers.

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Stereological formulas

4

CAVALIERI ESTIMATOR

Area associated with a point (Ap)

๐ด๐ด๐‘๐‘ = ๐‘”๐‘”2 g2 Grid area

Volume associated with a point (VP)

๐‘‰๐‘‰๐‘๐‘ = ๐‘”๐‘”2๐‘š๐‘š๐‘ก๐‘กฬ…

m Section evaluation interval ๐‘ก๐‘กฬ… Mean section cut thickness

Estimated volume (๐‘ฝ๐‘ฝ๏ฟฝ) ๐‘‰๐‘‰๏ฟฝ = ๐ด๐ด๐‘๐‘๐‘š๐‘šโ€ฒ๐‘ก๐‘กฬ… ๏ฟฝ๏ฟฝ๐‘ƒ๐‘ƒ๐‘–๐‘–

๐‘›๐‘›

๐‘–๐‘–=1

๏ฟฝ Ap Area associated with a point mโ€™ Section evaluation interval ๐‘ก๐‘กฬ… Mean section cut thickness Pi Points counted on grid

Estimated volume

corrected for over-projection ([v])

[๐‘ฃ๐‘ฃ] = ๐‘ก๐‘ก.๏ฟฝ๐‘˜๐‘˜.๏ฟฝ๐‘Ž๐‘Žโ€ฒ๐‘—๐‘—

๐‘”๐‘”

๐‘—๐‘—=1

โˆ’ ๐‘š๐‘š๐‘Ž๐‘Ž๐‘š๐‘š(๐‘Ž๐‘Žโ€ฒ)๏ฟฝ t Section cut thickness k Correction factor g Grid size aโ€™ Projected area

Coefficient of error

(CE)

๐ถ๐ถ๐ถ๐ถ =โˆš๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿโˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

TotalVar Total variance of the estimated volume n Number of sections Pi Points counted on grid

๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ = ๐‘Ž๐‘Ž2 + ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘†

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Stereological formulas

5

Cavalieri Estimator (2)

Variance of systematic

random sampling (VARSRS)

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2) โˆ’ 4๐ต๐ต + ๐ถ๐ถ

12,๐‘š๐‘š = 0

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2) โˆ’ 4๐ต๐ต + ๐ถ๐ถ

240,๐‘š๐‘š = 1

m Smoothness class of sampled function s2 Variance due to noise ๐ด๐ด = โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–2๐‘›๐‘›

๐‘–๐‘–=1 , ๐ต๐ต = โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘ƒ๐‘ƒ๐‘–๐‘–+1๐‘›๐‘›โˆ’1๐‘–๐‘–=1 , ๐ถ๐ถ = โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘ƒ๐‘ƒ๐‘–๐‘–+2๐‘›๐‘›โˆ’2

๐‘–๐‘–=1

With:

n : number of sections

๐‘Ž๐‘Ž2 = 0.0724 ๏ฟฝ ๐‘๐‘โˆš๐‘Ž๐‘Ž๏ฟฝ๏ฟฝ๐‘›๐‘›โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›

๐‘–๐‘–=1 ๐‘๐‘โˆš๐‘Ž๐‘Ž

Shape factor

R e f e r e n c e s Garcรญa-Fiรฑana, M., Cruz-Orive, L.M., Mackay, C.E., Pakkenberg, B. & Roberts, N. (2003). Comparison of MR imaging against physical sectioning to estimate the volume of human cerebral compartments. Neuroimage, 18 (2), 505โ€“516. Gundersen, H. J. G., & Jensen, E.B. (1987). The efficiency of systematic sampling in stereology and its prediction. Journal of Microscopy, 147 (3), 229โ€“263. Howard, C. V., & Reed, M.G. (2005). Unbiased Stereology, Three-Dimensional Measurement in Microscopy (Chapter 3). New York: Garland Science/BIOS Scientific Publishers.

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Stereological formulas

6

COMBINED POINT INTERCEPT

Profile area (a) ๐‘Ž๐‘Ž = ๐‘Ž๐‘Ž(๐‘๐‘).๏ฟฝ๐‘ƒ๐‘ƒ a(p) Area associated with a point โˆ‘๐‘ƒ๐‘ƒ Number of points

Profile boundary (b) ๐‘๐‘ =

๐œ‹๐œ‹2๐‘‘๐‘‘.๏ฟฝ๐ผ๐ผ d Distance between points

โˆ‘๐ผ๐ผ Number of intersections

This method is based on the principles described in the following:

Howard, C.V., Reed, M.G. (2010). Unbiased Stereology (Second Edition). QTP Publications: Coleraine, UK. See equations 2.5 and 3.2

Miles, R.E., Davy, P. (1976). Precise and general conditions for the validity of a comprehensive set of stereological fundamental formulae. Journal of Microscopy, 107 (3), 211โ€“226.

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Stereological formulas

7

CONNECTIVITY ASSAY

Euler number (X3) ๐‘‹๐‘‹3 = ๐ผ๐ผ + ๐ป๐ป โˆ’ ๐ต๐ต I Total island markers ๐ป๐ป Total hole markers ๐ต๐ต Total bridge markers

Number of alveoli (Nalv) ๐‘๐‘๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘ฃ๐‘ฃ = โˆ’๐‘‹๐‘‹3 X3 Euler number

Sum counting frame volumes (V)

๐‘‰๐‘‰ = โ„Ž.๐‘›๐‘›.๐‘Ž๐‘Ž h Disector height n Number of disectors a Area counting frame

Numerical density of alveoli (Nv)

๐‘๐‘๐‘ฃ๐‘ฃ =๐‘๐‘๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘ฃ๐‘ฃ๐‘‰๐‘‰

Nalv Number of alveoli V Sum counting frame volumes

R e f e r e n c e s Ochs, M., Nyengaard, J.R., Jung, A., Knudsen, L., Voigt, M., Wahlers, T., Richter, J., & Gundersen, H.J.G. (2004). The number of alveoli in the human lung. American journal of respiratory and critical care medicine, 169 (1), 120โ€“124.

Page 8: ย ยท Stereological formulas . 25 . OPTICAL FRACTIONATOR . Estimate of total number of particles (N) โ„Ž. ๐‘๐‘= ๐‘„๐‘„ โˆ’. ๐‘ก๐‘ก. 1 ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ. 1 ๐‘Ž๐‘Ž๐‘Ž

Stereological formulas

8

CYCLOIDS FOR LV

Area associated with a point (Ap)

๐ด๐ด๐‘๐‘ = ๐‘”๐‘”2 g2 Grid area

Volume associated with a

point (Vp) ๐‘‰๐‘‰๐‘๐‘ = ๐‘”๐‘”2๐‘š๐‘š๐‘ก๐‘กฬ… g2 Grid area

m Section evaluation interval ๐‘ก๐‘กฬ… Mean section cut thickness

Length per unit volume (Lv) ๐ฟ๐ฟ๐‘‰๐‘‰ = 2

๏ฟฝ๐ผ๐ผ๏ฟฝฬ…๏ฟฝ๐ฟ๐ถ๐ถ๏ฟฝ๐‘๐‘๐‘๐‘๐‘—๐‘—โˆ†

๐ฟ๐ฟ๐‘‰๐‘‰ =2โˆ†

.๏ฟฝ๐ผ๐ผ๏ฟฝฬ…๏ฟฝ๐‘๐‘๐‘๐‘๐‘๐‘๐‘๏ฟฝ๐‘๐‘๐‘๐‘๐‘—๐‘—

๐‘ƒ๐‘ƒ๏ฟฝ. ๏ฟฝ๐‘‡๐‘‡๐‘๐‘๏ฟฝ=

2โˆ†๏ฟฝ๐‘๐‘๐‘๐‘๏ฟฝโˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

๏ฟฝILฬ…C๏ฟฝprj Number of counting frames โˆ† Section cut thickness Ii Intercepts Pi Test points ๏ฟฝICฬ…cyc๏ฟฝ

prj Average number of intersections of

projected images pl Test points per unit length of cycloid

Estimated volume (๐‘‰๐‘‰๏ฟฝ) ๐‘‰๐‘‰๏ฟฝ = ๐‘š๐‘šโˆ†๏ฟฝ

๐‘Ž๐‘Ž๐‘๐‘๏ฟฝ๏ฟฝ๐‘ƒ๐‘ƒ๐‘–๐‘–

๐‘›๐‘›

๐‘–๐‘–=1

m Sampling fractions โˆ† Section cut thickness a Area p Number of test points Pi Test points

Estimated length (๐ฟ๐ฟ๏ฟฝ) ๐ฟ๐ฟ๏ฟฝ = 2 ๏ฟฝ

๐‘Ž๐‘Ž๐‘‡๐‘‡๏ฟฝ๐‘š๐‘š๏ฟฝ๐ผ๐ผ๐‘–๐‘–

๐‘›๐‘›

๐‘–๐‘–=1

a Area l Line length m Sampling fractions Ii Intercepts

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Stereological formulas

9

Cycloids for Lv (2)

Coefficient of error for line length ๐ถ๐ถ๐ถ๐ถ๏ฟฝ๐ฟ๐ฟ๏ฟฝ|๐ฟ๐ฟ๏ฟฝ =

๏ฟฝ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘†โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

VARSRS Variance of systematic random sampling L๏ฟฝ|L Estimated length per length Ii Intercepts

Variance of systematic

random sampling (VARSRS) ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =

3๐‘”๐‘”0 โˆ’ 4๐‘”๐‘”1 + ๐‘”๐‘”212

๐‘”๐‘”๐‘˜๐‘˜ = ๏ฟฝ ๐ฟ๐ฟ๐‘–๐‘–๐ฟ๐ฟ๐‘–๐‘–+๐‘˜๐‘˜๐‘›๐‘›โˆ’๐‘˜๐‘˜

๐‘–๐‘–=1

g Grid size Li Line length at section i

Coefficient of error for length

density ๐ถ๐ถ๐ถ๐ถ(๐ฟ๐ฟ๐‘‰๐‘‰) = ๏ฟฝ

๐‘›๐‘›๐‘›๐‘› โˆ’ 1๏ฟฝ

โˆ‘ ๐ผ๐ผ๐‘–๐‘–2๐‘›๐‘›๐‘–๐‘–=1

โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1 โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›

๐‘–๐‘–=1+

โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–2๐‘›๐‘›๐‘–๐‘–=1

โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1 โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›

๐‘–๐‘–=1โˆ’ 2

โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1 โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›

๐‘–๐‘–=1๏ฟฝ

Ii Intercepts Pi Test points n Number of probes

R e f e r e n c e s

Artachoโ€Pรฉrula, E., Roldรกnโ€Villalobos, R. (1995). Estimation of capillary length density in skeletal muscle by unbiased stereological methods: I. Use of vertical slices of known thickness The Anatomical Record, 241 (3), 337-344.

Gokhale, A. M. (1990). Unbiased estimation of curve length in 3โ€D using vertical slices. Journal of Microscopy, 159 (2), 133โ€“141.

Howard, C. V., Reed, M.G. (1998). Unbiased Stereology, Three-Dimensional Measurement in Microscopy (pp. 170โ€“172). BIOS Scientific Publishers.

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Stereological formulas

10

CYCLOIDS FOR SV

Area associated with a point (Ap)

๐ด๐ด๐‘๐‘ = ๐‘”๐‘”2 g2 Grid area

Volume associated with a

point (Vp) ๐‘‰๐‘‰๐‘๐‘ = ๐‘”๐‘”2๐‘š๐‘š๐‘ก๐‘กฬ… g2 Grid area

m Evaluation interval ๐‘ก๐‘กฬ… Section cut thickness

Estimated surface area per unit volume (est Sv) ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐‘†๐‘†๐‘ฃ๐‘ฃ = 2 ๏ฟฝ

2๐‘๐‘๐‘‡๐‘‡๏ฟฝโˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

p/l Points per unit length of cycloid Ii Intercepts with cycloids Pi Point counts

Estimated volume (๐‘‰๐‘‰๏ฟฝ) ๐‘‰๐‘‰๏ฟฝ = ๐‘š๐‘š๐‘ก๐‘กฬ… ๏ฟฝ

๐‘Ž๐‘Ž๐‘๐‘๏ฟฝ๏ฟฝ๐‘ƒ๐‘ƒ๐‘–๐‘–

๐‘š๐‘š

๐‘–๐‘–=1

m Evaluation interval ๐‘ก๐‘กฬ… Section cut thickness a/p Area associated with each point Pi Point counts

Estimated surface area (๏ฟฝฬ‚๏ฟฝ๐‘†) ๏ฟฝฬ‚๏ฟฝ๐‘† = 2 ๏ฟฝ๐‘Ž๐‘Ž๐‘‡๐‘‡๏ฟฝ๐‘š๐‘š๐‘ก๐‘กฬ…๏ฟฝ ๐ผ๐ผ๐‘–๐‘–

๐‘š๐‘š

๐‘–๐‘–=1 m Evaluation interval

๐‘ก๐‘กฬ… Section cut thickness a/l Area per unit length Ii Intercepts with cycloids C

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11

Cycloids for Sv (2)

Coefficient of error for

estimated surface (CE)

๐ถ๐ถ๐ถ๐ถ๏ฟฝ๏ฟฝฬ‚๏ฟฝ๐‘†|๐‘†๐‘†๏ฟฝ =๏ฟฝ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘†โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

VarSRS Variance due to

systematic random sampling

VarSRS =3g0 โˆ’ 4g1 + g2

12

Coefficient of error for surface

density (CE (Sv))

๐ถ๐ถ๐ถ๐ถ(๐‘†๐‘†๐‘ฃ๐‘ฃ) = ๏ฟฝ๐‘›๐‘›

๐‘›๐‘› โˆ’ 1๏ฟฝโˆ‘ ๐ผ๐ผ๐‘–๐‘–2๐‘›๐‘›๐‘–๐‘–=1

โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1 โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›

๐‘–๐‘–=1+

โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–2๐‘›๐‘›๐‘–๐‘–=1

โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1 โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›

๐‘–๐‘–=1โˆ’ 2

โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1 ๐‘ƒ๐‘ƒ๐‘–๐‘–

โˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1 โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›

๐‘–๐‘–=1๏ฟฝ

n Number of measurements Ii Intercepts with cycloids Pi Point counts

References

Baddeley, A. J., Gundersen, H.J.G., & Cruzโ€Orive, L.M. (1998) Estimation of surface area from vertical sections. Journal of Microscopy, 142 (3), 259โ€“276.

Howard, C. V., Reed, M.G. (1998). Unbiased Stereology, Three-Dimensional Measurement in Microscopy(pp.170โ€“172). BIOS Scientific Publishers.

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DISCRETE VERTICAL ROTATOR

Estimated volume (Est v) ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐‘ฃ๐‘ฃ =

๐œ‹๐œ‹๐‘›๐‘›

.๐‘Ž๐‘Ž๐‘๐‘.๏ฟฝ๐‘ƒ๐‘ƒ๐‘–๐‘–

๐‘›๐‘›

๐‘–๐‘–=1

๐ท๐ท๐‘–๐‘–

n Number of centriolar sections ap Area associated with each point Pi Number of points in each class Di Distance of class from central axis

References

Mironov, A. A. (1998). Estimation of subcellular organelle volume from ultrathin sections through centrioles with a discretized version of the vertical rotator. Journal of microscopy, 192(1), 29-36.

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FRACTIONATOR

Estimate of total number of particles (N) ๐‘๐‘ = ๏ฟฝ๐‘„๐‘„โˆ’ .

1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

๐‘„๐‘„โˆ’ Particles counted ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ Area sampling fraction ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ Section sampling fraction

Variance due to

systematic random sampling โ€“ Gundersen

(VARSRS)

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2) โˆ’ 4๐ต๐ต + ๐ถ๐ถ

12,๐‘š๐‘š = 0

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2) โˆ’ 4๐ต๐ต + ๐ถ๐ถ

240,๐‘š๐‘š = 1

๐ด๐ด = โˆ‘ (๐‘„๐‘„๐‘–๐‘–โˆ’)2๐‘›๐‘›๐‘–๐‘–=1

๐ต๐ต = โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘„๐‘„๐‘–๐‘–+1โˆ’๐‘›๐‘›โˆ’1๐‘–๐‘–=1

๐ถ๐ถ = โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘„๐‘„๐‘–๐‘–+2โˆ’๐‘›๐‘›โˆ’2๐‘–๐‘–=1

s2 Variance due to noise

Variance due to noise - Gundersen (s2) ๐‘Ž๐‘Ž2 = ๏ฟฝ๐‘„๐‘„โˆ’

๐‘›๐‘›

๐‘–๐‘–=1

๐‘„๐‘„โˆ’ Particles counted n Number of sections used

Total variance โ€“ Gundersen (TotalVar)

๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ = ๐‘Ž๐‘Ž2 + ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† VARSRS Variance due to SRS s2 Variance due to noise

Coefficient of error โ€“ Gundersen (CE) ๐ถ๐ถ๐ถ๐ถ =

โˆš๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž2

TotalVar Total variance s2 Variance due to noise

Number-weighted mean section cut thickness

(๐’•๐’•๐‘ธ๐‘ธโˆ’๏ฟฝ๏ฟฝ๏ฟฝ๏ฟฝ๏ฟฝ)

๐‘ก๐‘ก๐‘„๐‘„โˆ’๏ฟฝ๏ฟฝ๏ฟฝ๏ฟฝ =โˆ‘ ๐‘ก๐‘ก๐‘–๐‘–๐‘š๐‘š๐‘–๐‘–=1 ๐‘„๐‘„๐‘–๐‘–โˆ’

โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘š๐‘š๐‘–๐‘–=1

m Number of sections ti Section thickness at site i Qi Particles counted

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Stereological formulas

14

Fractionator (2)

Coefficient of error โ€“ Scheaffer (CE) ๐ถ๐ถ๐ถ๐ถ =

๏ฟฝ๐‘Ž๐‘Ž2 ๏ฟฝ1๐‘Ÿ๐‘Ÿ โˆ’

1๐น๐น๏ฟฝ

๐‘„๐‘„๏ฟฝ

f Number of counting frames ๐น๐น Total possible sampling sites ๐‘Ž๐‘Ž2 Estimated variance ๐‘„๐‘„๏ฟฝ Average particles counted

Average number of particles โ€“

Scheaffer (๐‘ธ๐‘ธ๏ฟฝ) ๐‘„๐‘„๏ฟฝ =โˆ‘ ๐‘„๐‘„๐‘–๐‘–๐‘“๐‘“๐‘–๐‘–=1๐‘Ÿ๐‘Ÿ

Qi Particles counted f Number of counting frames

Estimated variance - Scheaffer (s2) ๐‘Ž๐‘Ž2 =

โˆ‘ (๐‘„๐‘„๐‘–๐‘– โˆ’ ๐‘„๐‘„๏ฟฝ)2๐‘“๐‘“๐‘–๐‘–=1๐‘Ÿ๐‘Ÿ โˆ’ 1

f Number of counting frames Qi Particles counted Q๏ฟฝ Average particles counted

Estimated variance of estimated cell population - Scheaffer

๐ถ๐ถ๐‘“๐‘“๐‘๐‘๐น๐น2๐‘Ž๐‘Ž2

๐‘Ÿ๐‘Ÿ Cfp Finite population correction

๐‘Ž๐‘Ž2 Estimated variance f Number of counting frames ๐น๐น Total possible sampling sites Estimated variance of mean cell

count - Scheaffer ๐ถ๐ถ๐‘“๐‘“๐‘๐‘๐‘Ž๐‘Ž2

๐‘Ÿ๐‘Ÿ Cfp Finite population correction

๐‘Ž๐‘Ž2 Estimated variance f Number of counting frames

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Stereological formulas

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Fractionator (3)

Estimated mean coefficient of error โ€“ Cruz-Orive (est Mean CE) ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐‘€๐‘€๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘›๐‘› ๐ถ๐ถ๐ถ๐ถ (๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐‘๐‘) = ๏ฟฝ

13๐‘›๐‘›

.๏ฟฝ๏ฟฝ๐‘„๐‘„1๐‘–๐‘– โˆ’ ๐‘„๐‘„2๐‘–๐‘–๐‘„๐‘„1๐‘–๐‘– + ๐‘„๐‘„2๐‘–๐‘–

๏ฟฝ2๐‘›๐‘›

๐‘–๐‘–=1

๏ฟฝ

12๏ฟฝ

Q1i Counts in sub-sample 1 Q2i Counts in sub-sample 2 n Size of sub-sample

Predicted coefficient of error for estimated population โ€“ Schmitz-

Hof (CEpred) ๐ถ๐ถ๐ถ๐ถ๐‘๐‘๐‘๐‘๐‘๐‘๐‘๐‘(๐‘›๐‘›๐น๐น) = ๏ฟฝ

๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ(๐‘„๐‘„๐‘๐‘โˆ’)๐‘‰๐‘‰. (๐‘„๐‘„๐‘๐‘โˆ’)2

๐ถ๐ถ๐ถ๐ถ๐‘๐‘๐‘๐‘๐‘๐‘๐‘๐‘(๐‘›๐‘›๐น๐น) =1

๏ฟฝโˆ‘ ๐‘„๐‘„๐‘๐‘โˆ’๐‘†๐‘†๐‘๐‘=1

=1

๏ฟฝโˆ‘ ๐‘„๐‘„๐‘ ๐‘ โˆ’๐‘†๐‘†๐‘ ๐‘ =1

R Number of counting spaces S Number of sections Qrโˆ’ Counts in the โ€œrโ€-th counting space

Qsโˆ’ Counts in the โ€œsโ€-th section

References Geiser, M., Cruzโ€Orive, L.M., Hof, V.I., & Gehr, P. (1990) Assessment of particle retention and clearance in the intrapulmonary conducting airways of hamster lungs with the fractionator. Journal of Microscopy, 160 (1), 75โ€“88.

Glaser, E. M., Wilson, P.D. (1998). The coefficient of error of optical fractionator population size estimates: a computer simulation comparing three estimators. Journal of Microscopy, 192 (2), 163โ€“171.

Gundersen, H.J.G., Vedel Jensen, E.B., Kieu, K., & Nielsen, J. (1999). The efficiency of systematic sampling in stereologyโ€”reconsidered. Journal of Microscopy, 193 (3), 199โ€“211.

Gundersen, H. J. G., Jensen, E.B. (1987). The efficiency of systematic sampling in stereology and its prediction. Journal of Microscopy, 147 (3), 229โ€“263.

Howard, V., Reed, M. (2005). Unbiased stereology: three-dimensional measurement in microscopy (vol. 4, chapter 12). Garland Science/Bios Scientific Publishers.

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Stereological formulas

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Fractionator (4)

Scheaffer, R.L., Ott, L., & Mendenhall, W. (1996). Elementary survey sampling (chapter 7). Boston: PWS-Kent.

Schmitz, C., Hof, P.R. (2000). Recommendations for straightforward and rigorous methods of counting neurons based on a computer simulation approach. Journal of Chemical Neuroanatomy, 20 (1), 93โ€“114.

West, M. J., Slomianka, L., & Gundersen, H.J.G. (1991). Unbiased stereological estimation of the total number of neurons in the subdivisions of the rat hippocampus using the optical fractionator. The Anatomical Record, 231 (4), 482โ€“497.

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Stereological formulas

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ISOTROPIC FAKIR

Estimated total surface area ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก๐‘†๐‘† = 2

1๐‘›๐‘›

.๏ฟฝ๐‘ฃ๐‘ฃ๐‘‡๐‘‡๐‘–๐‘–

. ๐ผ๐ผ๐‘–๐‘–

๐‘›๐‘›

๐‘–๐‘–=1

n Number of line sets (always set to 3) ๐‘ฃ๐‘ฃ๐‘Ž๐‘Ž๐‘–๐‘– Inverse of the probe per unit volume

Ii Intercepts with test lines

References

Kubรญnovรก, L., Janacek, J. (1998). Estimating surface area by the isotropic fakir method from thick slices cut in an arbitrary direction. Journal of Microscopy, 191 (2), 201โ€“211.

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Stereological formulas

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ISOTROPIC VIRTUAL PLANES

Length per unit volume ๐ฟ๐ฟ๐‘‰๐‘‰ =2๐‘๐‘(๐‘๐‘๐‘‡๐‘‡๐‘š๐‘š)๐‘Ž๐‘Ž(๐‘๐‘๐‘‡๐‘‡๐‘Ž๐‘Ž๐‘›๐‘›๐‘Ÿ๐‘Ÿ) .

โˆ‘๐‘„๐‘„โˆ‘๐‘๐‘(๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ) p(box) Number of corners considered

a(plane) Exact sampling area p(ref) Number of corners in region โˆ‘๐‘„๐‘„ Total number of transects

Estimated total length ๐ฟ๐ฟ =1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.1โ„Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.1๐‘๐‘๐‘Ž๐‘Ž๐‘‘๐‘‘

. 2๏ฟฝ๐‘„๐‘„

Or ๐ฟ๐ฟ = 1๐‘ ๐‘ ๐‘ ๐‘ ๐‘“๐‘“

. ๐‘๐‘๐‘‘๐‘‘.๐‘๐‘๐‘๐‘๐‘Ž๐‘Ž(๐‘๐‘๐‘๐‘๐‘‘๐‘‘)

. ๐‘ก๐‘กฬ…โ„Ž(๐‘๐‘๐‘๐‘๐‘‘๐‘‘) .๐‘‘๐‘‘. 2โˆ‘๐‘„๐‘„

๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ =๐‘Ž๐‘Ž(๐‘๐‘๐‘‡๐‘‡๐‘š๐‘š)๐‘‘๐‘‘๐‘š๐‘š.๐‘‘๐‘‘๐‘‘๐‘‘

โ„Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ =โ„Ž(๐‘๐‘๐‘‡๐‘‡๐‘š๐‘š)

๐‘ก๐‘กฬ…

๐‘๐‘๐‘Ž๐‘Ž๐‘‘๐‘‘ =๐ถ๐ถ[๐‘Ž๐‘Ž(๐‘๐‘๐‘‡๐‘‡๐‘Ž๐‘Ž๐‘›๐‘›๐‘Ÿ๐‘Ÿ)]๐‘ฃ๐‘ฃ(๐‘๐‘๐‘‡๐‘‡๐‘š๐‘š) =

1๐‘‘๐‘‘

ssf Section sampling fraction asf Area sampling fraction hsf Height sampling fraction psd Probe sampling density โˆ‘๐‘„๐‘„ Total number of transects a(box) Area of sampling box h(box) Depth of sampling box d Sampling plane separation dx, dy Distances in XY ๐‘ก๐‘กฬ… Average section thickness a(plane) Sampling plane area E Expected value v(box) Volume of sampling box

Total plane area ๐ด๐ด = ๏ฟฝ๏ฟฝ๐ด๐ด๐‘–๐‘–,๐‘—๐‘—

๐‘ ๐‘ 

๐‘—๐‘—=1

๐‘Ž๐‘Ž

๐‘–๐‘–=1

l Number of layouts s Number of sampling sites Ai,j Plane area inside of each sampling box for

each layout

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Stereological formulas

19

Isotropic Virtual Planes (2)

Coefficient of error

(Gundersen) ๐ถ๐ถ๐ถ๐ถ =๏ฟฝ3(๐ด๐ด โˆ’ ๐‘ƒ๐‘ƒ๐‘‡๐‘‡๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘›๐‘› ๐‘›๐‘›๐‘‡๐‘‡๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ)

12 + ๐‘ƒ๐‘ƒ๐‘‡๐‘‡๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘›๐‘› ๐‘›๐‘›๐‘‡๐‘‡๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

โˆ‘๐‘„๐‘„,๐‘š๐‘š = 0

๐ถ๐ถ๐ถ๐ถ =๏ฟฝ3(๐ด๐ด โˆ’ ๐‘ƒ๐‘ƒ๐‘‡๐‘‡๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘›๐‘› ๐‘›๐‘›๐‘‡๐‘‡๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ)โˆ’ 4๐ต๐ต + ๐ถ๐ถ

240 + ๐‘ƒ๐‘ƒ๐‘‡๐‘‡๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘›๐‘› ๐‘›๐‘›๐‘‡๐‘‡๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

โˆ‘๐‘„๐‘„,๐‘š๐‘š = 1

Poisson noise is โˆ‘Qi

A = ๏ฟฝ(Qi. Qi)

B = ๏ฟฝ(Qi. Qi+1)

C = ๏ฟฝ(Qi. Qi+2)

A,B,C Covariogram values Qi Particles counted

Plane areas ๐‘‰๐‘‰๏ฟฝโƒ‘ = (๐ด๐ด,๐ต๐ต,๐ถ๐ถ)

๐‘๐‘๐‘‡๐‘‡๐‘Ž๐‘Ž๐‘›๐‘›๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž:๐ด๐ด๐‘š๐‘š + ๐ต๐ต๐‘‘๐‘‘ + ๐ถ๐ถ๐ถ๐ถ + ๐ท๐ท๐‘–๐‘– = 0, ๐ท๐ท๐‘–๐‘– = ๐ท๐ท + ๐‘‘๐‘‘. ๐‘ƒ๐‘ƒ

๐‘๐‘๐‘‡๐‘‡๐‘š๐‘š: ๏ฟฝ๏ฟฝ(๐‘š๐‘š,๐‘‘๐‘‘, ๐ถ๐ถ)๏ฟฝ๐‘š๐‘š0 โ‰ค ๐‘š๐‘š โ‰ค ๐‘š๐‘š0 + ๐‘๐‘๐‘‘๐‘‘๐‘‘๐‘‘0 โ‰ค ๐‘‘๐‘‘ โ‰ค ๐‘‘๐‘‘0 + ๐‘๐‘๐‘๐‘๐ถ๐ถ0 โ‰ค ๐ถ๐ถ โ‰ค ๐ถ๐ถ0 + ๐‘๐‘๐‘ง๐‘ง

๏ฟฝ๏ฟฝ

๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž: (๐‘๐‘๐‘‡๐‘‡๐‘š๐‘š โˆฉ ๐‘๐‘๐‘‡๐‘‡๐‘Ž๐‘Ž๐‘›๐‘›๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž)

A,B,C,D Given constants d Distance between planes i Integer x0,y0,z0 Vertex of a sampling box bx,by,bz Dimensions of a sampling

box

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Stereological formulas

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Isotropic Virtual Planes (3)

Average number of counts ๐‘„๐‘„๏ฟฝ =

โˆ‘ โˆ‘ ๐‘„๐‘„๐‘–๐‘– ๐‘—๐‘—๐‘Ž๐‘Ž๐‘—๐‘—๐‘—๐‘—=1

๐‘๐‘๐‘–๐‘–=1

โˆ‘ ๐‘‡๐‘‡๐‘—๐‘—๐‘๐‘๐‘—๐‘—=1

p Number of probes Lj Number of layouts in each probe Qi j Number of counts in each probe and layout

Total corners of sampling boxes inside the region of interest

๐ถ๐ถ = ๏ฟฝ๐ถ๐ถ๐‘–๐‘–

๐‘๐‘

๐‘–๐‘–=1

p Number of probes Ci Number of sampling boxes inside region of interest

References

Larsen, J. O., Gundersen, H.J.G., & Nielsen, J. (1998). Global spatial sampling with isotropic virtual planes: estimators of length density and total length in thick, arbitrarily orientated sections. Journal of Microscopy, 191, 238โ€“248.

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Stereological formulas

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IUR PLANES OPTICAL FRACTIONATOR

Estimated length ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐ฟ๐ฟ = 2.๐‘Ž๐‘Ž๐‘‡๐‘‡๏ฟฝ๐ผ๐ผ .

1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.๐‘ก๐‘กโ„Ž

a/l Area per unit length of test line โˆ‘๐ผ๐ผ Number of intersections ssf Section sampling fraction asf Area sampling fraction t Section cut thickness h Height of counting frame

Area sampling fraction ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ =

๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž(๐น๐น๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘š๐‘š๐‘Ÿ๐‘Ÿ)๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž(๐‘š๐‘š,๐‘‘๐‘‘ ๐‘Ž๐‘Ž๐‘ก๐‘ก๐‘Ÿ๐‘Ÿ๐‘๐‘) =

๐‘š๐‘š๐ถ๐ถ๐น๐น .๐‘‘๐‘‘๐ถ๐ถ๐น๐น๐‘š๐‘š๐‘ ๐‘ ๐‘ก๐‘ก๐‘๐‘๐‘๐‘.๐‘‘๐‘‘๐‘ ๐‘ ๐‘ก๐‘ก๐‘๐‘๐‘๐‘

xCF,yCF XY dimensions of counting frame xstep, ystep Dimensions of grid area(Frame) Area of counting frame area(x,y step) Area of grid

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Stereological formulas

22

L-CYCLOID OPTICAL FRACTIONATOR

Estimated length of lineal structure ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐ฟ๐ฟ = 2.

๐‘Ž๐‘Ž๐‘‡๐‘‡๏ฟฝ๐ผ๐ผ .

1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.๐‘ก๐‘กโ„Ž

a/l Area per unit cycloid length โˆ‘๐ผ๐ผ Number of intercepts ssf Section sampling fraction asf Area sampling fraction t Section cut thickness h Height of counting frame

Area sampling fraction ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ =

๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž(๐น๐น๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘š๐‘š๐‘Ÿ๐‘Ÿ)๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž(๐‘š๐‘š,๐‘‘๐‘‘ ๐‘Ž๐‘Ž๐‘ก๐‘ก๐‘Ÿ๐‘Ÿ๐‘๐‘) =

๐‘š๐‘š๐ถ๐ถ๐น๐น .๐‘‘๐‘‘๐ถ๐ถ๐น๐น๐‘š๐‘š๐‘ ๐‘ ๐‘ก๐‘ก๐‘๐‘๐‘๐‘.๐‘‘๐‘‘๐‘ ๐‘ ๐‘ก๐‘ก๐‘๐‘๐‘๐‘

xCF,yCF XY dimensions of counting frame xstep, ystep Dimensions of grid area(Frame) Area of counting frame area(x,y step) Area of grid

References Stocks, E. A., McArthur, J.C., Griffen, J.W., & Mouton, P.R. (1996). An unbiased method for estimation of total epidermal nerve fiber length. Journal of Neurocytology, 25 (1), 637โ€“644.

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Stereological formulas

23

MERZ

Length of semi-circle (L) ๐ฟ๐ฟ =12๐œ‹๐œ‹๐‘‘๐‘‘

d Circle diameter

Surface area per unit volume (Sv) ๐‘†๐‘†๐‘ฃ๐‘ฃ =2โˆ‘ ๐ผ๐ผ๐‘‡๐‘‡๐‘๐‘โˆ‘๐‘ƒ๐‘ƒ

I Number of intercepts l/p Length of semi-circle per point P Number of points

References

Howard, C. V., Reed, M. G. (2010). Unbiased stereology. Liverpool, UK: QTP Publications. {See equation 6.4}

Weibel, E.R. (1979). Stereological Methods. Vol. 1: Practical methods for biological morphometry. London, UK: Academic Press.

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Stereological formulas

24

NUCLEATOR

Area estimate ๐‘Ž๐‘Ž = ๐œ‹๐œ‹๐‘‡๐‘‡2๏ฟฝ l Length of rays

Volume estimate ๐‘ฃ๐‘ฃ๐‘๐‘๏ฟฝ๏ฟฝ๏ฟฝ๏ฟฝ =

4๐œ‹๐œ‹3๐‘‡๐‘‡๐‘›๐‘›3๏ฟฝ l Length of rays

Estimated coefficient of error

๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐ถ๐ถ๐‘‰๐‘‰(๐‘‰๐‘‰) =๏ฟฝ 1๐‘›๐‘› โˆ’ 1โˆ‘ (๐‘‰๐‘‰๐‘–๐‘– โˆ’ ๐‘‰๐‘‰๏ฟฝ)2๐‘›๐‘›

๐‘–๐‘–=1

๐‘‰๐‘‰๏ฟฝ

n Number of nucleator estimates Ri Area/volume estimate for each sampling site

Average area/volume estimate ๐‘‰๐‘‰๏ฟฝ =

1๐‘›๐‘›๏ฟฝ๐‘‰๐‘‰๐‘–๐‘–

๐‘›๐‘›

๐‘–๐‘–=1

n Number of nucleator estimates Ri Area/volume estimate for each sampling site

Relative efficiency ๐ถ๐ถ๐ถ๐ถ๐‘›๐‘›(๐‘‰๐‘‰) =๐ถ๐ถ๐‘‰๐‘‰(๐‘‰๐‘‰)โˆš๐‘›๐‘›

n Number of nucleator estimates CV (R) Estimated coefficient of variation

Geometric mean of area/volume estimate ๐‘Ÿ๐‘Ÿ๏ฟฝ

1๐‘›๐‘›โˆ‘ ๐‘Ž๐‘Ž๐‘›๐‘›๐‘†๐‘†๐‘–๐‘–๐‘›๐‘›

๐‘–๐‘–=1 ๏ฟฝ n Number of nucleator estimates Ri Area/volume estimate for each sampling site

References Gundersen, H.J.G. (1988). The nucleator. Journal of Microscopy, 151 (1), 3โ€“21.

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Stereological formulas

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OPTICAL FRACTIONATOR

Estimate of total number of particles (N) ๐‘๐‘ = ๏ฟฝ๐‘„๐‘„โˆ’.

๐‘ก๐‘กโ„Ž

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

๐‘„๐‘„โˆ’ Particles counted t Section mounted thickness h Counting frame height ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ Area sampling fraction ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ Section sampling fraction

Variance due to

systematic random sampling โ€“ Gundersen

(VARSRS)

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2) โˆ’ 4๐ต๐ต + ๐ถ๐ถ

12,๐‘š๐‘š = 0

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2) โˆ’ 4๐ต๐ต + ๐ถ๐ถ

240,๐‘š๐‘š = 1

๐ด๐ด = โˆ‘ (๐‘„๐‘„๐‘–๐‘–โˆ’)2๐‘›๐‘›๐‘–๐‘–=1

๐ต๐ต = โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘„๐‘„๐‘–๐‘–+1โˆ’๐‘›๐‘›โˆ’1๐‘–๐‘–=1

๐ถ๐ถ = โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘„๐‘„๐‘–๐‘–+2โˆ’๐‘›๐‘›โˆ’2๐‘–๐‘–=1

s2 Variance due to noise

Variance due to noise - Gundersen (s2) ๐‘Ž๐‘Ž2 = ๏ฟฝ๐‘„๐‘„โˆ’

๐‘›๐‘›

๐‘–๐‘–=1

๐‘„๐‘„โˆ’ Particles counted n Number of sections used

Total variance โ€“ Gundersen (TotalVar)

๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ = ๐‘Ž๐‘Ž2 + ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† VARSRS Variance due to SRS s2 Variance due to noise

Coefficient of error โ€“ Gundersen (CE) ๐ถ๐ถ๐ถ๐ถ =

โˆš๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž2

TotalVar Total variance s2 Variance due to noise

Number-weighted mean section cut thickness

(๐’•๐’•๐‘ธ๐‘ธโˆ’๏ฟฝ๏ฟฝ๏ฟฝ๏ฟฝ๏ฟฝ)

๐‘ก๐‘ก๐‘„๐‘„โˆ’๏ฟฝ๏ฟฝ๏ฟฝ๏ฟฝ =โˆ‘ ๐‘ก๐‘ก๐‘–๐‘–๐‘š๐‘š๐‘–๐‘–=1 ๐‘„๐‘„๐‘–๐‘–โˆ’

โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘š๐‘š๐‘–๐‘–=1

m Number of sections ti Section thickness at site i Qi Particles counted

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Stereological formulas

26

Optical Fractionator (2)

Coefficient of error โ€“ Scheaffer (CE) ๐ถ๐ถ๐ถ๐ถ =

๏ฟฝ๐‘Ž๐‘Ž2 ๏ฟฝ1๐‘Ÿ๐‘Ÿ โˆ’

1๐น๐น๏ฟฝ

๐‘„๐‘„๏ฟฝ

f Number of counting frames ๐น๐น Total possible sampling sites ๐‘Ž๐‘Ž2 Estimated variance ๐‘„๐‘„๏ฟฝ Average particles counted

Average number of particles โ€“

Scheaffer (๐‘ธ๐‘ธ๏ฟฝ) ๐‘„๐‘„๏ฟฝ =โˆ‘ ๐‘„๐‘„๐‘–๐‘–๐‘“๐‘“๐‘–๐‘–=1๐‘Ÿ๐‘Ÿ

Qi Particles counted f Number of counting frames

Estimated variance - Scheaffer (s2) ๐‘Ž๐‘Ž2 =

โˆ‘ (๐‘„๐‘„๐‘–๐‘– โˆ’ ๐‘„๐‘„๏ฟฝ)2๐‘“๐‘“๐‘–๐‘–=1๐‘Ÿ๐‘Ÿ โˆ’ 1

f Number of counting frames Qi Particles counted Q๏ฟฝ Average particles counted

Estimated variance of estimated cell population - Scheaffer

๐ถ๐ถ๐‘“๐‘“๐‘๐‘๐น๐น2๐‘Ž๐‘Ž2

๐‘Ÿ๐‘Ÿ Cfp Finite population correction

๐‘Ž๐‘Ž2 Estimated variance f Number of counting frames ๐น๐น Total possible sampling sites Estimated variance of mean cell

count - Scheaffer ๐ถ๐ถ๐‘“๐‘“๐‘๐‘๐‘Ž๐‘Ž2

๐‘Ÿ๐‘Ÿ Cfp Finite population correction

๐‘Ž๐‘Ž2 Estimated variance f Number of counting frames

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Stereological formulas

27

Optical Fractionator (3)

Estimated mean coefficient of error โ€“ Cruz-Orive (est Mean CE) ๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐‘€๐‘€๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘›๐‘› ๐ถ๐ถ๐ถ๐ถ (๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘ก๐‘ก ๐‘๐‘) = ๏ฟฝ

13๐‘›๐‘›

.๏ฟฝ๏ฟฝ๐‘„๐‘„1๐‘–๐‘– โˆ’ ๐‘„๐‘„2๐‘–๐‘–๐‘„๐‘„1๐‘–๐‘– + ๐‘„๐‘„2๐‘–๐‘–

๏ฟฝ2๐‘›๐‘›

๐‘–๐‘–=1

๏ฟฝ

12๏ฟฝ

Q1i Counts in sub-sample 1 Q2i Counts in sub-sample 2 n Size of sub-sample

Predicted coefficient of error for estimated population โ€“ Schmitz-

Hof (CEpred) ๐ถ๐ถ๐ถ๐ถ๐‘๐‘๐‘๐‘๐‘๐‘๐‘๐‘(๐‘›๐‘›๐น๐น) = ๏ฟฝ

๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ(๐‘„๐‘„๐‘๐‘โˆ’)๐‘‰๐‘‰. (๐‘„๐‘„๐‘๐‘โˆ’)2

๐ถ๐ถ๐ถ๐ถ๐‘๐‘๐‘๐‘๐‘๐‘๐‘๐‘(๐‘›๐‘›๐น๐น) =1

๏ฟฝโˆ‘ ๐‘„๐‘„๐‘๐‘โˆ’๐‘†๐‘†๐‘๐‘=1

=1

๏ฟฝโˆ‘ ๐‘„๐‘„๐‘ ๐‘ โˆ’๐‘†๐‘†๐‘ ๐‘ =1

R Number of counting spaces S Number of sections Qrโˆ’ Counts in the โ€œrโ€-th counting space

Qsโˆ’ Counts in the โ€œsโ€-th section

References Geiser, M., Cruzโ€Orive, L.M., Hof, V.I., & Gehr, P. (1990) Assessment of particle retention and clearance in the intrapulmonary conducting airways of hamster lungs with the fractionator. Journal of Microscopy, 160 (1), 75โ€“88.

Glaser, E. M., Wilson, P.D. (1998). The coefficient of error of optical fractionator population size estimates: a computer simulation comparing three estimators. Journal of Microscopy, 192 (2), 163โ€“171.

Gundersen, H.J.G., Vedel Jensen, E.B., Kieu, K., & Nielsen, J. (1999). The efficiency of systematic sampling in stereologyโ€”reconsidered. Journal of Microscopy, 193 (3), 199โ€“211.

Gundersen, H. J. G., Jensen, E.B. (1987). The efficiency of systematic sampling in stereology and its prediction. Journal of Microscopy, 147 (3), 229โ€“263.

Howard, V., Reed, M. (2005). Unbiased stereology: three-dimensional measurement in microscopy (vol. 4, chapter 12). Garland Science/Bios Scientific Publishers.

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Stereological formulas

28

Optical Fractionator (4)

Scheaffer, R.L., Ott, L., & Mendenhall, W. (1996). Elementary survey sampling (chapter 7). Boston: PWS-Kent.

Schmitz, C., Hof, P.R. (2000). Recommendations for straightforward and rigorous methods of counting neurons based on a computer simulation approach. Journal of Chemical Neuroanatomy, 20 (1), 93โ€“114.

West, M. J., Slomianka, L., & Gundersen, H.J.G. (1991). Unbiased stereological estimation of the total number of neurons in the subdivisions of the rat hippocampus using the optical fractionator. The Anatomical Record, 231 (4), 482โ€“497.

Page 29: ย ยท Stereological formulas . 25 . OPTICAL FRACTIONATOR . Estimate of total number of particles (N) โ„Ž. ๐‘๐‘= ๐‘„๐‘„ โˆ’. ๐‘ก๐‘ก. 1 ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ. 1 ๐‘Ž๐‘Ž๐‘Ž

Stereological formulas

29

OPTICAL ROTATOR

Volume of particle ๐‘ฃ๐‘ฃ๏ฟฝ = ๐‘Ž๐‘Ž๏ฟฝ๐‘”๐‘”(๐‘ƒ๐‘ƒ๐‘–๐‘–)

+/โˆ’

๐‘–๐‘–

a Reciprocal line density a=k.h k Length of slice h Systematic spacing

For vertical slabs and lines parallel to vertical

axis

๐‘”๐‘”(๐‘ƒ๐‘ƒ) = ๐‘‘๐‘‘1, ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ ๐‘‘๐‘‘2 < ๐‘ก๐‘ก

๐‘”๐‘”(๐‘ƒ๐‘ƒ) =๐œ‹๐œ‹2 ๐‘‘๐‘‘1

๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘ƒ๐‘ƒ๐‘›๐‘› ๏ฟฝ ๐‘ก๐‘ก๐‘‘๐‘‘2๏ฟฝ

, ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ ๐‘ก๐‘ก โ‰ค ๐‘‘๐‘‘2

d1 Distance along test line d2 Distance from origin to test line t ยฝ thickness of optical slice

For vertical slabs and lines perpendicular to

vertical axis

๐‘”๐‘”(๐‘ƒ๐‘ƒ) = ๐‘‘๐‘‘1, ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ ๏ฟฝ๐‘‘๐‘‘12 + ๐ถ๐ถ2 < ๐‘ก๐‘ก

๐‘”๐‘”(๐‘ƒ๐‘ƒ) = ๐‘Ÿ๐‘Ÿ ๏ฟฝ๏ฟฝ๐‘ก๐‘ก2 โˆ’ ๐ถ๐ถ2๏ฟฝ , ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ |๐ถ๐ถ| < ๐‘ก๐‘ก โ‰ค ๏ฟฝ๐‘‘๐‘‘12 + ๐ถ๐ถ2

๐‘”๐‘”(๐‘ƒ๐‘ƒ) = ๐‘Ÿ๐‘Ÿ(0), ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ ๐‘ก๐‘ก โ‰ค |๐ถ๐ถ|

๐‘Ÿ๐‘Ÿ(๐‘š๐‘š) = ๐‘š๐‘š +๐œ‹๐œ‹2๏ฟฝ

1

๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘ƒ๐‘ƒ๐‘›๐‘› ๏ฟฝ ๐‘ก๐‘กโˆš๐‘ข๐‘ข2 + ๐ถ๐ถ2

๏ฟฝ๐‘‘๐‘‘๐‘ข๐‘ข

๐‘๐‘1

๐‘‘๐‘‘

d1 Distance along test line t ยฝ thickness of optical slice z Distance in z from intercept to origin

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Stereological formulas

30

Optical Rotator (2)

For isotropic

slabs

๐‘”๐‘”(๐‘ƒ๐‘ƒ) = ๐‘‘๐‘‘1, ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ ๐‘‘๐‘‘3 < ๐‘ก๐‘ก

๐‘”๐‘”(๐‘ƒ๐‘ƒ) =12๐‘ก๐‘ก

[โ„Ž(๐‘ก๐‘ก,๐‘‘๐‘‘2) + ๐‘˜๐‘˜(๐‘ก๐‘ก,๐‘‘๐‘‘1,๐‘‘๐‘‘2,๐‘‘๐‘‘3)], ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ ๐‘‘๐‘‘2 < ๐‘ก๐‘กโ‰ค ๐‘‘๐‘‘3

โ„Ž(๐‘ก๐‘ก,๐‘‘๐‘‘) = ๐‘ก๐‘ก2๏ฟฝ1 โˆ’๐‘‘๐‘‘2

๐‘ก๐‘ก2

๐‘˜๐‘˜(๐‘ก๐‘ก,๐‘‘๐‘‘1,๐‘‘๐‘‘2,๐‘‘๐‘‘3) = ๐‘‘๐‘‘1๐‘‘๐‘‘3 + ๐‘‘๐‘‘22๐‘‡๐‘‡๐‘‡๐‘‡๐‘”๐‘” ๏ฟฝ๐‘‘๐‘‘1 + ๐‘‘๐‘‘3

๐‘ก๐‘ก + ๏ฟฝ๐‘ก๐‘ก2 โˆ’ ๐‘‘๐‘‘22๏ฟฝ

d1 Distance along test line d2 Distance from origin to test line d3 Distance from intercept to origin t ยฝ thickness of optical slice

Estimated surface area

๏ฟฝฬ‚๏ฟฝ๐‘† = ๐‘Ž๐‘Ž๏ฟฝ๐‘‡๐‘‡๐‘—๐‘—๐‘”๐‘”๏ฟฝ๐‘‡๐‘‡๐‘—๐‘—๏ฟฝ๐‘—๐‘—

๐‘”๐‘”(๐‘‡๐‘‡) = 2, ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ ๐‘‘๐‘‘2 < ๐‘ก๐‘ก

๐‘”๐‘”(๐‘‡๐‘‡) = ๐œ‹๐œ‹.1

๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘ƒ๐‘ƒ๐‘›๐‘› ๏ฟฝ ๐‘ก๐‘ก๐‘‘๐‘‘2๏ฟฝ

, ๐‘ƒ๐‘ƒ๐‘Ÿ๐‘Ÿ ๐‘ก๐‘ก โ‰ค ๐‘‘๐‘‘2

a Reciprocal line density lj Number of intersections between grid line and cell boundary d2 Distance from origin to test line t ยฝ thickness of optical slice

References Tandrup, T., Gundersen, H.J.G., & Vedel Jensen, E.B. (1997). The optical rotator Journal of microscopy, 186 (2), 108โ€“120.

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Stereological formulas

31

PETRIMETRICS

Total length (๐‘ณ๐‘ณ๏ฟฝ) ๐ฟ๐ฟ๏ฟฝ =๐œ‹๐œ‹2

.๐‘Ž๐‘Ž๐‘‡๐‘‡

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.๏ฟฝ๐ผ๐ผ

๐ฟ๐ฟ๏ฟฝ = ๐‘‘๐‘‘.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.๏ฟฝ๐ผ๐ผ

a/l = 2d/ฯ€ Grid constant (2d/ฯ€ units or ratio of area to length of

semi-circle probe) asf Area fraction (ratio of area of counting frame to grid-

step) I Number of intersections counted d = 2*Merz-radius where the Merz-radius refers to the radius of the semi-circle used to probe.

References Howard, C. V., & Reed, M. G. (2005). Unbiased stereology. New York: Garland Science (prev. BIOS Scientific Publishers).

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Stereological formulas

32

PHYSICAL FRACTIONATOR

Total number of particles (N) ๐‘๐‘ = ๏ฟฝ๐‘„๐‘„โˆ’ .1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

๐‘„๐‘„โˆ’ Particles counted ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ Area sampling fraction ๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ Section sampling fraction

Variance due to noise (s2) ๐‘Ž๐‘Ž2 = ๏ฟฝ๐‘„๐‘„โˆ’

๐‘›๐‘›

๐‘–๐‘–=1

๐‘„๐‘„โˆ’ Particles counted n Number of sections used

Variance due to systematic random sampling (VARSRS) ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =

3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2) โˆ’ 4๐ต๐ต + ๐ถ๐ถ12

,๐‘š๐‘š = 0

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2) โˆ’ 4๐ต๐ต + ๐ถ๐ถ

240,๐‘š๐‘š = 1

๐ด๐ด = โˆ‘ (๐‘„๐‘„๐‘–๐‘–โˆ’)2๐‘›๐‘›๐‘–๐‘–=1

๐ต๐ต = โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘„๐‘„๐‘–๐‘–+1โˆ’๐‘›๐‘›โˆ’1๐‘–๐‘–=1

๐ถ๐ถ = โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘„๐‘„๐‘–๐‘–+2โˆ’๐‘›๐‘›โˆ’2๐‘–๐‘–=1

s2 Variance due to noise

Total variance (TotalVar) ๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ = ๐‘Ž๐‘Ž2 + ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† VARSRS Variance due to SRS s2 Variance due to noise

Coefficient of error (CE) ๐ถ๐ถ๐ถ๐ถ =

โˆš๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž2

TotalVar Total variance s2 Variance due to noise

References Gundersen, Hans-Jรธrgen G. "Stereology of arbitrary particles*." Journal of Microscopy 143, no. 1 (1986): 3-45. Sterio, D. C. "The unbiased estimation of number and sizes of arbitrary particles using the disector." Journal of Microscopy 134, no. 2 (1984): 127-136.

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Stereological formulas

33

PLANAR ROTATOR

Volume for isotropic planar rotator

๐‘‰๐‘‰ = 2๐‘ก๐‘ก๏ฟฝ๐‘”๐‘”๐‘–๐‘–๐‘–๐‘–

t Separation between test lines gi Isotropic planar rotator function

Volume for vertical planar rotator

๐‘‰๐‘‰ = ๐œ‹๐œ‹๐‘ก๐‘ก๏ฟฝ๐‘‡๐‘‡๐‘–๐‘–2

๐‘–๐‘–

t Separation between test lines li Intercept length along a test line

Isotropic planar rotator function ๐‘”๐‘”๐‘–๐‘–(๐‘‡๐‘‡) = ๐‘‡๐‘‡๏ฟฝ๐‘‡๐‘‡2 + ๐‘Ž๐‘Ž๐‘–๐‘–2 + ๐‘Ž๐‘Ž๐‘–๐‘–2๐‘‡๐‘‡๐‘›๐‘› ๏ฟฝ

๐‘‡๐‘‡๐‘Ž๐‘Ž๐‘–๐‘–

+ ๏ฟฝ๏ฟฝ๐‘‡๐‘‡๐‘Ž๐‘Ž๐‘–๐‘–๏ฟฝ2

+ 1๏ฟฝ

๐‘”๐‘”๐‘–๐‘–+ = ๏ฟฝ ๐‘”๐‘”๐‘–๐‘–๏ฟฝ๐‘‡๐‘‡๐‘–๐‘– ๐‘—๐‘—+๏ฟฝ โˆ’ ๏ฟฝ ๐‘”๐‘”๐‘–๐‘–๏ฟฝ๐‘‡๐‘‡๐‘–๐‘– ๐‘—๐‘—+๏ฟฝ๐‘—๐‘— ๐‘๐‘๐‘๐‘๐‘๐‘๐‘—๐‘— ๐‘๐‘๐‘ฃ๐‘ฃ๐‘๐‘๐‘›๐‘›

๐‘”๐‘”๐‘–๐‘–โˆ’ = ๏ฟฝ ๐‘”๐‘”๐‘–๐‘–๏ฟฝ๐‘‡๐‘‡๐‘–๐‘– ๐‘—๐‘—โˆ’๏ฟฝ โˆ’ ๏ฟฝ ๐‘”๐‘”๐‘–๐‘–๏ฟฝ๐‘‡๐‘‡๐‘–๐‘– ๐‘—๐‘—โˆ’๏ฟฝ๐‘—๐‘— ๐‘๐‘๐‘๐‘๐‘๐‘๐‘—๐‘— ๐‘๐‘๐‘ฃ๐‘ฃ๐‘๐‘๐‘›๐‘›

๐‘”๐‘”๐‘–๐‘– =12

(๐‘”๐‘”๐‘–๐‘–+ + ๐‘”๐‘”๐‘–๐‘–โˆ’)

l Intercept length along a test line ai Distance from origin to test line j Number of grid lines lij Number of intersections between the j-th

grid line and the cell boundary

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34

Planar Rotator (2)

Isotropic planar rotator function (contโ€™d) ๐‘‡๐‘‡๐‘–๐‘–+2 = ๏ฟฝ ๐‘‡๐‘‡๐‘–๐‘– ๐‘—๐‘—+2

๐‘—๐‘— ๐‘๐‘๐‘ฃ๐‘ฃ๐‘๐‘๐‘›๐‘›

โˆ’ ๏ฟฝ ๐‘‡๐‘‡๐‘–๐‘– ๐‘—๐‘—+2

๐‘—๐‘— ๐‘๐‘๐‘๐‘๐‘๐‘

๐‘‡๐‘‡๐‘–๐‘–โˆ’2 = ๏ฟฝ ๐‘‡๐‘‡๐‘–๐‘– ๐‘—๐‘—โˆ’2

๐‘—๐‘— ๐‘๐‘๐‘ฃ๐‘ฃ๐‘๐‘๐‘›๐‘›

โˆ’ ๏ฟฝ ๐‘‡๐‘‡๐‘–๐‘– ๐‘—๐‘—โˆ’2

๐‘—๐‘— ๐‘๐‘๐‘๐‘๐‘๐‘

๐‘‡๐‘‡๐‘–๐‘–2 =12 ๏ฟฝ๐‘‡๐‘‡๐‘–๐‘–+

2 + ๐‘‡๐‘‡๐‘–๐‘–โˆ’2 ๏ฟฝ

l Intercept length along a test line ai Distance from origin to test line j Number of grid lines lij Number of intersections between the j-th

grid line and the cell boundary

References Jensen Vedel, E.B., Gundersen, H.J.G. (1993). The rotator Journal of Microscopy, 170 (1), 35โ€“44.

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POINT SAMPLED INTERCEPT

Volume based on intercept length (๐‘ฝ๐‘ฝ๐’—๐’—๏ฟฝ)

๐‘‰๐‘‰๏ฟฝ๏ฟฝ๐‘‰๐‘‰ =๐œ‹๐œ‹3๐‘‡๐‘‡0ฬ…3 =

๐œ‹๐œ‹3๐‘›๐‘›

๏ฟฝ ๐‘‡๐‘‡0,๐‘–๐‘–3

๐‘›๐‘›

๐‘–๐‘–=1

n Number of intercepts l Intercept length

Volume-weighted mean volume (๐’—๐’—๏ฟฝ๐‘ฝ๐‘ฝ) ๐’—๐’—๏ฟฝ๐‘ฝ๐‘ฝ =

โˆ‘ ๏ฟฝฬ…๏ฟฝ๐’๐ŸŽ๐ŸŽ๐Ÿ‘๐Ÿ‘๐’๐’๐’Š๐’Š=๐Ÿ๐Ÿ

๐’๐’.๐…๐…๐Ÿ‘๐Ÿ‘

n Number of intercepts l Intercept length

Coefficient of error (CE)

๐ถ๐ถ๐ถ๐ถ๏ฟฝ๐‘‡๐‘‡0ฬ…3๏ฟฝ = ๏ฟฝโˆ‘ ๏ฟฝ๐‘‡๐‘‡0ฬ…3๏ฟฝ

2๐‘›๐‘›๐‘–๐‘–=1

๏ฟฝโˆ‘ ๐‘‡๐‘‡0ฬ…3๐‘›๐‘›๐‘–๐‘–=1 ๏ฟฝ

2 โˆ’1๐‘›๐‘›

n Number of intercepts l Intercept length

Coefficient of variance (CV) ๐ถ๐ถ๐ถ๐ถ๏ฟฝ๐‘‡๐‘‡0ฬ…3๏ฟฝ = ๐ถ๐ถ๐ถ๐ถ(๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘‰๐‘‰).โˆš๐‘›๐‘› n Number of intercepts l Intercept length ๐’—๐’—๏ฟฝ๐‘ฝ๐‘ฝ Volume-weighted mean volume

Variance (VarianceV) ๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘ƒ๐‘ƒ๐‘Ž๐‘Ž๐‘›๐‘›๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘‰๐‘‰(๐‘ฃ๐‘ฃ) = ๏ฟฝ๐œ‹๐œ‹3

. ๐‘†๐‘†๐ท๐ท๏ฟฝ๐‘‡๐‘‡0ฬ…3๏ฟฝ๏ฟฝ = ๏ฟฝ๐ถ๐ถ๐‘‰๐‘‰๏ฟฝ๐‘‡๐‘‡0ฬ…3๏ฟฝ. ๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘‰๐‘‰๏ฟฝ L Intercept length ๐’—๐’—๏ฟฝ๐‘ฝ๐‘ฝ Volume-weighted mean volume CV Coefficient of variance

References

Gundersen, H.J.G., Jensen. E.B. (1985). Stereological Estimation of the Volume-Weighted Mean Volume of Arbitrary Particles Observed on Random Sections. Journal of Microscopy, 138, 127โ€“142.

Sรธrensen, F.B. (1991). Stereological estimation of the mean and variance of nuclear volume from vertical sections. Journal of Microscopy, 162 (2), 203โ€“229.

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SIZE DISTRIBUTION

Volume-weighted mean particle volume

๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘‰๐‘‰ = ๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘๐‘. [1 + ๐ถ๐ถ๐‘‰๐‘‰๐‘๐‘2(๐‘ฃ๐‘ฃ)] v๏ฟฝN Number-weighted mean volume

CVN(v) Coefficient of variation

Number-weighted mean volume ๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘๐‘ =

โˆ‘๐‘†๐‘†โˆ‘๐‘‰๐‘‰

๐‘†๐‘† = ๐‘„๐‘„.๐‘‰๐‘‰

R Number of contours Q Number of points per contour

Variance

๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘๐‘(๐‘ฃ๐‘ฃ) =๏ฟฝโˆ‘๐‘‡๐‘‡ โˆ’ (โˆ‘๐‘†๐‘†)2

โˆ‘๐‘‰๐‘‰ ๏ฟฝ . ๐‘ฃ๐‘ฃ(๐‘๐‘)2

โˆ‘๐‘‰๐‘‰ โˆ’ 1

๐‘‡๐‘‡ = ๐‘„๐‘„2.๐‘‰๐‘‰

R Number of contours Q Number of points per contour v(p) Volume associated with a point

Standard deviation ๐‘†๐‘†๐ท๐ท๐‘๐‘(๐‘ฃ๐‘ฃ) = ๏ฟฝ๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘๐‘(๐‘ฃ๐‘ฃ)

๐‘†๐‘†๐ท๐ท๐‘๐‘(๐‘ฃ๐‘ฃ) = ๏ฟฝ๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘๐‘ . (๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘‰๐‘‰ โˆ’ ๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘๐‘)

v๏ฟฝN Number-weighted mean volume v๏ฟฝV Volume-weighted particle volume VarN Variance

Coefficient of variation ๐ถ๐ถ๐‘‰๐‘‰๐‘๐‘(๐‘ฃ๐‘ฃ) =

๐‘†๐‘†๐ท๐ท๐‘๐‘(๐‘ฃ๐‘ฃ)๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘๐‘

๐ถ๐ถ๐‘‰๐‘‰๐‘๐‘(๐‘ฃ๐‘ฃ) = ๏ฟฝ๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘‰๐‘‰ โˆ’ ๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘๐‘๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘๐‘

v๏ฟฝN Number-weighted mean volume v๏ฟฝV Volume-weighted particle volume SDN Standard deviation

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Size distribution (2)

Coefficient of error ๐ถ๐ถ๐ถ๐ถ๐‘๐‘(๐‘ฃ๐‘ฃ) =

๐ถ๐ถ๐‘‰๐‘‰๐‘๐‘(๐‘ฃ๐‘ฃ)โˆš๐‘‰๐‘‰

CVN Coefficient of variation R Number of contours

References Sรธrensen, F.B. (1991). Stereological estimation of the mean and variance of nuclear volume from vertical sections. Journal of Microscopy, 162 (2), 203โ€“229.

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SPACEBALLS

Length estimate ๐ฟ๐ฟ = 2.๏ฟฝ๏ฟฝ๐‘„๐‘„๐‘–๐‘–

๐‘›๐‘›

๐‘–๐‘–=1

๏ฟฝ .๐‘ฃ๐‘ฃ๐‘Ž๐‘Ž

.1๐‘Ž๐‘Ž๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ

This equation does not include the terms F2 (area-fraction) and F3 (thickness-fraction) used by Mouton et al. (equation 2, 2002), but includes that information in v (volume sampled).

n Number of sections used Qi Intersection counted v Volume (grid X * grid Y* section

thickness) a Surface area of the sphere ssf Section sampling fraction

Variance due to noise

๐‘Ž๐‘Ž2 = ๏ฟฝ๐‘„๐‘„๐‘–๐‘–

๐‘›๐‘›

๐‘–๐‘–=1

Qi Intersection counted

Variance due to systematic random

sampling

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2)โˆ’ 4๐ต๐ต + ๐ถ๐ถ

12,๐‘š๐‘š = 0

๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† =3(๐ด๐ด โˆ’ ๐‘Ž๐‘Ž2)โˆ’ 4๐ต๐ต + ๐ถ๐ถ

240,๐‘š๐‘š = 1

๐ด๐ด = โˆ‘ (๐‘„๐‘„๐‘–๐‘–โˆ’)2๐‘›๐‘›๐‘–๐‘–=1

๐ต๐ต = โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘„๐‘„๐‘–๐‘–+1โˆ’๐‘›๐‘›โˆ’1๐‘–๐‘–=1

๐ถ๐ถ = โˆ‘ ๐‘„๐‘„๐‘–๐‘–โˆ’๐‘„๐‘„๐‘–๐‘–+2โˆ’๐‘›๐‘›โˆ’2๐‘–๐‘–=1

s2 Variance due to noise m Smoothness class of sampled function

Total variance ๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ = ๐‘Ž๐‘Ž2 + ๐‘‰๐‘‰๐ด๐ด๐‘‰๐‘‰๐‘†๐‘†๐‘†๐‘†๐‘†๐‘† VARSRS Variance due to SRS s2 Variance due to noise

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Stereological formulas

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Spaceballs (2)

Coefficient of error ๐ถ๐ถ๐ถ๐ถ =

โˆš๐‘‡๐‘‡๐‘‡๐‘‡๐‘ก๐‘ก๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘‰๐‘‰๐‘Ž๐‘Ž๐‘Ÿ๐‘Ÿ๐‘Ž๐‘Ž2

TotalVar Total variance s2 Variance due to noise

References

Mouton, P. R., Gokhale, A.M., Ward, N.L., & West, M.J. (2002). Stereological length estimation using spherical probes. Journal of Microscopy, 206 (1), 54โ€“64.

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Stereological formulas

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SURFACE-WEIGHTED STAR VOLUME

Surface-weighted star volume (๐’—๐’—๏ฟฝ๏ฟฝ๐’”๐’”โˆ—) ๐’—๐’—๏ฟฝ๏ฟฝ๐’”๐’”โˆ— =

๐Ÿ๐Ÿ๐…๐…๐Ÿ‘๐Ÿ‘

. ๏ฟฝฬ…๏ฟฝ๐’๐Ÿ๐Ÿ๐Ÿ‘๐Ÿ‘

๐’—๐’—๏ฟฝ๏ฟฝ๐’”๐’”โˆ— =๐Ÿ๐Ÿ๐…๐…๐Ÿ‘๐Ÿ‘ .

โˆ‘ โˆ‘ ๐’๐’๐Ÿ๐Ÿ,(๐’Š๐’Š,๐’‹๐’‹)๐Ÿ‘๐Ÿ‘๐’Ž๐’Ž๐’Š๐’Š

๐’‹๐’‹=๐Ÿ๐Ÿ๐’๐’๐’Š๐’Š=๐Ÿ๐Ÿ

โˆ‘ ๐’Ž๐’Ž๐’Š๐’Š๐’๐’๐’Š๐’Š=๐Ÿ๐Ÿ

n Number of probes l Intercept length mi Number of intercepts

Sum of cubed intercepts in probe (yi) ๐‘‘๐‘‘๐‘–๐‘– = ๏ฟฝ๐‘‡๐‘‡1,(๐‘–๐‘–,๐‘—๐‘—)

3

๐‘š๐‘š๐‘–๐‘–

๐‘—๐‘—=1

mi Number of intercepts l Intercept length

Coefficient of error (CE) ๐ถ๐ถ๐ถ๐ถ๏ฟฝ๏ฟฝฬ…๏ฟฝ๐‘ฃ๐‘ ๐‘ โˆ—๏ฟฝ๏ฟฝ = ๏ฟฝ

๐‘›๐‘›๐‘›๐‘› โˆ’ 1 ๏ฟฝ

โˆ‘๐‘‘๐‘‘๐‘–๐‘–2

โˆ‘๐‘‘๐‘‘๐‘–๐‘– โˆ‘๐‘‘๐‘‘๐‘–๐‘–+

โˆ‘๐‘š๐‘š๐‘–๐‘–2

โˆ‘๐‘š๐‘š๐‘–๐‘– โˆ‘๐‘š๐‘š๐‘–๐‘–โˆ’ 2.

โˆ‘๐‘š๐‘š๐‘–๐‘–๐‘‘๐‘‘๐‘–๐‘–โˆ‘๐‘‘๐‘‘๐‘–๐‘– โˆ‘๐‘š๐‘š๐‘–๐‘–

๏ฟฝ๏ฟฝ12๏ฟฝ

n Number of probes yi Sum of cubed intercepts in probe mi Number of intercepts

References Reed, M. G., Howard, C.V. (1998). Surface-weighted star volume: concept and estimation. Journal of Microscopy, 190 (3), 350โ€“356.

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Stereological formulas

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SURFACTOR

Surface area for single-ray designs

๏ฟฝฬ‚๏ฟฝ๐‘† = 4๐œ‹๐œ‹๐‘‡๐‘‡02 + ๐‘Ž๐‘Ž(๐›ฝ๐›ฝ) l Length of intercept รŸ Angle between test line and surface c(รŸ) Function of the planar angle

Surface area for multi-ray

designs ๐‘บ๐‘บ๏ฟฝ = ๐Ÿ๐Ÿ๐…๐…๏ฟฝ๐’๐’๐’‹๐’‹๐Ÿ๐Ÿ. ๐’„๐’„(๐œท๐œท)๐Ÿ๐Ÿ๐Ÿ๐Ÿ

๐’‹๐’‹=๐Ÿ๐Ÿ

l Length of intercept รŸ Angle between test line and surface c(รŸ) Function of the planar angle r Number of test lines

Function of the planar angle ๐‘Ž๐‘Ž(๐›ฝ๐›ฝ) = 1 + ๏ฟฝ

12๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘ก๐‘ก๐›ฝ๐›ฝ๏ฟฝ . ๏ฟฝ

๐œ‹๐œ‹2โˆ’ ๐‘Ž๐‘Ž๐‘ƒ๐‘ƒ๐‘›๐‘›โˆ’1

1 โˆ’ ๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘ก๐‘ก2๐›ฝ๐›ฝ1 + ๐‘Ž๐‘Ž๐‘‡๐‘‡๐‘ก๐‘ก2๐›ฝ๐›ฝ

๏ฟฝ รŸ Angle between test line and surface

References Jensen, E.B., Gundersen, H.J.G. (1987). Stereological estimation of surface area of arbitrary particles. Acta Stereologica, 6 (3).

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Stereological formulas

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SV-CYCLOID FRACTIONATOR

Estimated surface area per unit volume ๐‘†๐‘†๐‘‰๐‘‰ = 2 ๏ฟฝ

๐‘๐‘๐‘‡๐‘‡๏ฟฝโˆ‘ ๐ผ๐ผ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

โˆ‘ ๐‘ƒ๐‘ƒ๐‘–๐‘–๐‘›๐‘›๐‘–๐‘–=1

p/l Ratio of test points to curve length n Number of micrographs โˆ‘ Ii Total intercept points on curve โˆ‘ P๐‘–๐‘– Total test points

References Baddeley, A. J., Gundersen, H.J.G., & Cruzโ€Orive, L.M. (1986). Estimation of surface area from vertical sections. Journal of Microscopy, 142 (3), 259โ€“276.

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Stereological formulas

43

VERTICAL SPATIAL GRID

Estimated volume ๐‘‰๐‘‰๏ฟฝ = ๐‘Ž๐‘Ž.๐‘‘๐‘‘๐‘๐‘.๏ฟฝ๐‘ƒ๐‘ƒ๐‘–๐‘–

๐‘š๐‘š

๐‘–๐‘–=1

a Area associated with point dz Distance between planes m Number of scanning planes โˆ‘ P Intersections with points

Area associated with point ๐‘Ž๐‘Ž =

๐‘ค๐‘ค2

2๐œ‹๐œ‹ w Horizontal width

Estimated surface area ๏ฟฝฬ‚๏ฟฝ๐‘† = 2.๐‘Ž๐‘Ž.๐‘‘๐‘‘๐‘๐‘

๐‘‡๐‘‡ + 4๐œ‹๐œ‹ .๐‘‘๐‘‘๐‘๐‘

. ๏ฟฝ๐‘ƒ๐‘ƒ๐‘‘๐‘‘๐‘๐‘ + ๐ผ๐ผ๐‘‘๐‘‘๐‘ง๐‘ง๏ฟฝ a Area associated with point dz Distance between planes l Length of cycloid Ixy X,Y intersections Ixz X,Z intersections Length of cycloid ๐‘‡๐‘‡ =

2๐‘ค๐‘ค๐œ‹๐œ‹

w Horizontal width

X,Y intersections ๐ผ๐ผ๐‘‘๐‘‘๐‘๐‘ = ๏ฟฝ๐ผ๐ผ๐‘‘๐‘‘๐‘๐‘,๐‘–๐‘–

๐‘š๐‘š

๐‘–๐‘–=1

m Number of scanning planes

X,Z intersections ๐ผ๐ผ๐‘‘๐‘‘๐‘ง๐‘ง = 2.๏ฟฝ๏ฟฝ๐‘ƒ๐‘ƒ๐‘–๐‘–

๐‘š๐‘š

๐‘–๐‘–=1

โˆ’ ๏ฟฝ ๐‘ƒ๐‘ƒ๐‘–๐‘–,๐‘–๐‘–+1

๐‘š๐‘šโˆ’1

๐‘–๐‘–=1

๏ฟฝ m Number of scanning planes โˆ‘๐‘ƒ๐‘ƒ Intersections with points

References Cruz-Orive, L. M., Howard, C.V. (1995). Estimation of individual feature surface area with the vertical spatial grid. Journal of Microscopy, 178 (2), 146โ€“151.

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Stereological formulas

44

WEIBEL

Surface area per unit volume (Sv) ๐‘†๐‘†๐‘ฃ๐‘ฃ = 2.๏ฟฝ

๐ผ๐ผ๐‘‡๐‘‡2 .๐‘ƒ๐‘ƒ

๏ฟฝ

I Intersections (triangular markers) P Points (end points circular markers) l Length of each line

Note: We use l/2 for the length represented at each point since there are two end points per line.

References Weibel, E.R., Kistler, G.S., & Scherle, W.F. (1966). Practical stereological methods for morphometric cytology. The Journal of cell biology, 30 (1), 23โ€“38.