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Solution Behavior. Crystal structure is solution structureWe had hoped so Proofs NMR data Protein crystals are mostly solvent Random coil loops the exception. -Localized by crystallization. . Solute. To be soluble the solute must interact with the solution more favorable than its self. C
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1. Physical and Chemical Properties of Proteins in Solution Hydrodynamics
Or
How to study the structure of a protein you haven’t crystallized.
2. Solution Behavior Crystal structure is solution structure
We had hoped so
Proofs
NMR data
Protein crystals are mostly solvent
Random coil loops the exception.
-Localized by crystallization.
3. Solute To be soluble the solute must interact with the solution more favorable than its self.
Charge
4. Solution Behavior Solubility
Varies tremendously
From insoluble to 350 mg/ml
Solubility in Aqueous media
Depends on surface charge
pH
Salts
Often used in purification
Co-solvents
May also be used in purification
5. Behavior in Aqueous solutions Solubility in Aqueous media
Depends on surface charge
pH
Salts
Often used in purification
Co-solvents
May also be used in purification
6. Solution Behavior Solvent Factors governing solubility
pH
Isoelectric point
7. Solution Behavior Solvent Factors governing solubili
8. Surface/shape effects on proteins in solution
9. Diffusion Molecules undergo Brownian motion
Translational motion is Diffusion
dc/dt= D(d2C/dx)
Integrated it looks like
D= x2/2t
distance is proportional to the square root of time
10. Diffusion Rate of motion is dependent on
Size
Shape
Spherical a=b
Oblate spheroids a>b Axis of rotation is b
Prolate Spheroids a>b axis of rotation is a
solvent protein interactions
Values for diffusion are for Hydrated spheres
11. Diffusion Observed rates of diffusion are expressed as Einstien Sutherland eq.
f=kbT/D
Frictional ratio expressed as
f/fo
Always greater than unity because of hydration.
1.05-1.38
12. Selected hydrodynamic data1
13. Sedimentation analysis Hydrodynamic properties assessed by movement though a gravitational field.
dr/dt = {[Mw(1-??)]/Naf }?2r
Rearranged to focus on sedimentation we get the Svedberg eq.
s= [Mw(1-??)]/Naf = [Mw(1-??)]/DRT
S=10-13 s =Svedberg
S is Mass, shape dependent as well as density.
14. Gel Filtration
See chapter one for details
15. Rotation Very sensitive to shape
Measured as relaxation time tR
Correlation time + 1/3 relaxation
Rotational difusion constant 1/(2 tR)
tR=3Vh0 /kbT
Primarily Measured by Fluorescence polarization
Two phenomena measured
NMR on smaller molecules
16. Spectral Properties Absorbance
Phe Tyr and Trp
l max is environmentally dependent
use cosolvents to change enviroment
protected groups don’t shift.
Average of the whole molecule
17. Spectral Properties Fluorescence
Phe Tyr and Trp
l max is environmentally dependent
Trp exposed vs buried
Tyr not seen unless no Trp
Phe not seen unless no Trp and Tyr
18. Spectral Properties Circular dichroism (CD) and Optical Rotary dispersion (ORD).
sensitive to conformation
Strong signals indicate Alpha helix and Beta sheet.
interfering signals from disulfides and aromatic residues
Reasonable probe of changes to environment of those residues
19. Short peptides = Sum of the amino acids
Proteins ? Sum of the amino acids
Compact folding
Resist protease degradation
Stable with breaks in the peptide change
One Primary fold
Shifts in structure occur mostly in quatanary structure or domain structure.
Why = Chapter 7
20. Ionization of side chains ionizable side chains on the surface of a protein behave as those in free solution
Ionizable side chains in the interior of a protein may have radically shifted pKa’s
21. Chemical Propreties Principle actor in this case is the principle of effective concentration.
Proteins holds groups in positions that result in hyperactivity of the groups.
22. Definition Domain: Region of a protein that folds to a stable structure mostly independent of other structure in the protein (other domains).