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AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory, Teddington 9th December 2008

AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

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Page 1: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

AUC and DLS probes for protein aggregation

Steve Harding & Arthur RoweNational Centre for Macromolecular Hydrodynamics

The National Physical Laboratory, Teddington

9th December 2008

Page 2: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Questions

• Aggregation state in response to bioprocessingn-mers present and relative amounts

• Conformation of the monomer species before and after bioprocessing

Page 3: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

A model of chimeric IgG3 wild type.

A model of chimeric IgG3 m15 with 15aa in hinge.

A model of chimeric hinge deleted IgG3 HM5.

Conformation of Engineered antibodies

Lu et al, Biophys. J. 2007

Page 4: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Stability Problems

• Aggregation or bits falling off during purification, sterilisation, shipping and storage processes.

• Temperature of storage and cycles of freeze thaw

Page 5: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Stability/aggregation ProbesAnalytical ultracentrifugation Dynamic Light Scattering

Viscometry SEC/MALLs

Page 6: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Stability/aggregation ProbesAnalytical ultracentrifugation Dynamic Light Scattering

Viscometry SEC/MALLs

Page 7: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Multi-angle DLS

Page 8: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Fixed angle DLS

Cuvettes:

Malvern nanozetasizer 90

Page 9: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Detector/ Correlator-Computer

Correlator-Computer correlates fluctuations in intensity at angle due to the Brownian motion of the macromolecules.

An intensity autocorrelation function g(2)(t) is calculated and its decay with time gives us the diffusion coefficient D 6

Bk TD

R

Page 10: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

0

2

4

6

8

0.1 1 10 100 1000 10000

Inte

nsity

(%)

Size (d.nm)

Size Distribution by Intensity

Record 108: san 003 pure Record 109: san 003 pureRecord 110: san 003 pure Record 111: san 003 pureRecord 112: san 003 pure Record 113: san 003 pure

Page 11: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

0

10

20

30

0.1 1 10 100 1000 10000

Vo

lum

e (

%)

Size (d.nm)

Size Distribution by Volume

Record 108: san 003 pure Record 109: san 003 pureRecord 110: san 003 pure Record 111: san 003 pureRecord 112: san 003 pure Record 113: san 003 pure

Page 12: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Optima XLA/ XLI

Page 13: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,
Page 14: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Sedimentation Equilibrium

Air Solvent

Solution

conc, c

distance, r

Rate of movement of boundary sed. coeff

Centrifugal force

conc, c

distance, r

Centrifugal force Diffusion

so20,w

1S=10-13sec

STEADY STATE PATTERN

FUNCTION ONLY OF MOL. WEIGHT PARAMETERS

Sedimentation Velocity

Page 15: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Data analysis: g*(s) plot

Page 16: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Ultracentrifuge Analysis: IgG4 preparation

Page 17: AUC and DLS probes for protein aggregation Steve Harding & Arthur Rowe National Centre for Macromolecular Hydrodynamics The National Physical Laboratory,

Ultracentrifuge Analysis: IgG4 preparation