Lecture 11
Jump to navigation
Jump to search
Contents
how find structure?
- PDB - 80,000 structures
- x-ray crystallography - not simple, can't do within a week, cost time money effort, and no guarante to get structure
- make one by using homology modeling, if lucky enough
- but novel protein? amyloid beta doesn't crystallize
- use a template - don't need to invent wheel all the time!
- the template is the homologous protein for which we already know structure
how claim 2 structures are similar?
- RMSD - root mean squared division
- structurally align as much as possible
- then measure distance
- homework - calculate RMSD - "c-alpha" "all atom rmsd"
structure building
- how to use template to model homologous sequence
- sequence alignment - like 85% done
- backbone chain optimization - change template to account for gap - done by energy minimization technique
- then optimize side chain
- then evaluate how correct your projection is through theoretical ways and experimental ways - USE BOTH
- making model is easy - validating is not easy
- theoretical: hydrophobic stays on one side, phillic on the other
troubleshooting
- protein quality check software, molecular dynamics, monte carlo, energy minimization
- if homology low - fundamental problem
journal club
- conformational sampling - building reliable models - THE BOTTLENECK
- computational cost increases dramatically with chain length
- longer aa, becomes longer beads on a string instead of lobular, can break up into modules and
- rosetta algorithm - crowd sourcing to figure out inter domain interaction, David Baker 2011 "Crowdsourcing to write algorithms"
CASP - protein structure prediction competition
- homology modelling has thus far beaten energy minimization every time
- protein docking capri
- most accurate = lowest energy - free energy scatter plots
- refined natives = blue points
- energy landscape
protein folding
- achieve most thermodynamically stable state
- leviathan paradox
- folded state goes through local intermediates but eventually reach global minimum
- lattice model
- beads in a lattice
- off-lattice model
- all atom model
S6 folding
- energy landscape
- transition state
- enthalpy - heat released
- entropy
- gibbs free energy
- phi-value - minimize this thermodynamic state
disulfide bonds tendamistat
- covalent interact btw residuues containing sulfide
- order of oxydation and reduction - order matters in way it folds
- limits folding space to make fast? kinetic roadblocks of transitional intermediate bonds to make slow?
- "go-model" simulation
- graph showing which residues interact with which
=beta hairpins
bbl folding
- type 0 folding no high free energy barrier - has one minimum, no high activation, no energy barrier
- type 1 - high free enrgy barrier, two state
- CL2 - well known protein that has two state
chaperonin assisted folding
- chaperones = GroEL protein
- makes crowded state around protein
- in vivo folding - geometrically confines - accellerates folding folding, lowering entropy
- but crowdined environment retards folding
- so try folding in a cylinder
protein self interaction
- discrete molecular dynamics
- discrete models of potentials, reduces equations to set of algebraic eqs
- reduces computational intensity
- protein tested EAK peptide
- electrostatic interaction
- discreteMD - reduced computation for molecular dynamics
- 1 femtosecond = delta t to calculate energy = model interaction over 1 MILIsecond - takes months - discreteMD reducees by 2 ords magnitute
metal co-factor assisted folding
pathway
- alpha helix
- beta helix - rate limiting
- zinc-binding - plays significant role - stablizes interactions
- "molecular machines"