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Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical...

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Treatment of Non- ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.
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Page 1: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Treatment of Non-ideality in Sedimentation Velocity

Experiments

Walter Stafford,Boston Biomedical Research Institute,

Watertown, MA 02472 U.S.A.

Page 2: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Hydrodynamicvs

Thermodynamicnon-ideality

s f (c)Dg(c)

Page 3: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

s f (c)Generally empirical

backflow (A.J. Rowe …)charge effects (Donnan equilibrium)

Except for large asymmetric proteins,charge effects usually dominate backflow.

Page 4: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Dg(c)Both hydrodynamic and thermodynamic contributions

Except for large asymmetric proteins,charge effects usually dominate excluded volume effects.

Page 5: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

f (c) f (0) 1K sc

Frictional coefficient

HYDRODYNAMIC

Affects both s and D

Page 6: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Hydrodynamic c-dependence= same for s and D

sso

1 ksc and D

Do1 ksc

FC=gradient of centrifugal potential FD=gradient of chemical potential

frictional resistance is the same for both

Page 7: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Thermodynamicconcentration dependence

1 ln(y)

ln(c)

Excluded volume and Donnan equilibrium

Page 8: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Colligative virial coefficients

ln(y) BcCc2 Dc3 ...

B, C and D are the 2nd, 3rd and fourth virial colligative coefficients, respectively.(McMillan and Mayer, 1945, statistical thermodynamics)

Page 9: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Combined hydrodynamic and thermodynamic concentration

dependence of D

D D o

1 ln(y)

ln(c)

1 ksc

Page 10: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

ln(yi ) Bici Cici2 Dic i

3 ...

ci ln(yi )

ci

ln(yi )

ln(ci )2Bci 3Cci

2 4Dci3 ...

Page 11: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

DDo12BM1c

1 ksc

Expansion truncated after the 2nd virial term …

(Cf. Also Harding and Johnson, 1985; and Alex Solovyova et al, 2001)

Page 12: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

DDo 12BM1c ksc

Expansion truncated after the 2nd virial term …And further approximation …

(both Harding and Johnson, 1985; and Alex Solovyova et al, 2001)

1

1ax1 ax ... for small a

Page 13: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Multiple Species

Self-associating system

Page 14: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

ln(yi ) Bici Cici2 Dic i

3 ...

ln(yi ) Biici Bijc jji

n

Ciici2 Cijkc jck

ji

n

ki

n

Diic i3 Dijklc jckcl

li

n

ki

n

ji

n

...

Cross terms …

Single species (no cross terms)

Multiple species (cross terms)

Page 15: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Self-associating system all species must have the same charge to mass ratio

andfrictional ratio

However …

Page 16: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Di Dio 12BM1cT

1 ksjc jj1

n

Page 17: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

g(s) 6

Non-ideal reversible monomer-dimer system

Protein-X

Lowest cIntermediate c

Highest c

Page 18: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.
Page 19: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Sedanal

Global fitting with SEDANAL

= 280 nm and 220 nm; path length = 12mm and 3 mm

Page 20: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.
Page 21: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Global fitting with SEDANAL

= 280 nm; path length = 12mm and 3 mm

Page 22: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Future plans

Extend to higher concentrations

Page 23: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Higher order terms

Add higher order terms …

Page 24: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

ln(yi )

ln(ci )2Bci 3Cci

2 4Dci3 ...

Page 25: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Donnan equilibriumFor uni-univalent electrolyte

e.g. NaCl

BZ 2

4M22m3

C 0

D Z 4

64M24m3

3

Roark and Yphantis 1971 Biochemistry

Page 26: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

BZ 2

4M22m3

DB2

4m3

Page 27: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

"Significant" is >= 1% contribution

Page 28: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Excluded volume effects

BM1 4vL

d

Page 29: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Hard sphere approx.or some other model

ln(i) f (c,{a})

Page 30: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Hard Sphere models

Minton 2007 J. Pharm Sci.

Page 31: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Minton 2007, Biophys J.

Scattering …

Page 32: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

M1 M1,app 1 ln(y1)

ln(c1)

ln(y1)

ln(c j )M j ,app

ji

n

M1 ln(y1)

ln(c j )M j ,app

ji

n

M1,app 1 ln(y1)

ln(c1)

M1,app

M1 1 ln(y1) ln(c j )

M j ,app

M1ji

n

1 ln(y1) ln(c1)

M1,app

M1 1 ln(y1) ln(c j )

M j ,app

M1ji

n

1 ln(y1) ln(c1)

sRTc

1 ln(y1) ln(c j )

M j ,app

M1ji

n

D 1 ln(y1) ln(c1)

D1,app D1 1 ln(y1)

ln(c1)

1 ln(y1) ln(c j )

M j ,app

M1ji

n

Poly-disperse system

Page 33: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

D1,app D 1 ln(y1)

ln(c1)

1 ln(y1) ln(c j )

M j ,app

M1ji

n

Page 34: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

Conclusions

Non-ideality in interacting systemsSimple linear approachExpand to higher order terms of virial

expansion with cross-termsOr use direct function

Page 35: Treatment of Non-ideality in Sedimentation Velocity Experiments Walter Stafford, Boston Biomedical Research Institute, Watertown, MA 02472 U.S.A.

TMP

TURBO-MOLECULAR PUMP


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