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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 havent 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 dont 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 pKas 
 
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).