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Statistical Mechanics of Proteins  Equilibrium and non-equilibrium properties of proteins  Free diffusion of proteins  Coherent motion in proteins:

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Presentation on theme: "Statistical Mechanics of Proteins  Equilibrium and non-equilibrium properties of proteins  Free diffusion of proteins  Coherent motion in proteins:"— Presentation transcript:

1 Statistical Mechanics of Proteins  Equilibrium and non-equilibrium properties of proteins  Free diffusion of proteins  Coherent motion in proteins: temperature echoes  Simulated cooling of proteins Ioan Kosztin Department of Physics & Astronomy University of Missouri - Columbia

2 Temperature Echoes in Proteins  Coherent motion in proteins: Echoes  Generation of echoes in ubiquitin via velocity reassignments 1)Temperature quench echoes 2)Constant velocity reassignment echoes 3)Velocity reassignment echoes kinetic temperature: temperature  velocities

3 Coherent Dynamics of Proteins  the internal dynamics of globular proteins comprises a wide range of time scales (10 -15 — 1 sec) coherence  motions of ps (10 -12 s) time scale have some coherence, related to concerted motions of many atoms in different parts of the portein MD simulations temperature echo technique  the coherence of proteins internal dynamics can be investigated via MD simulations by employing the temperature echo technique Questions: What are, and how do we generate temperature echoes ?

4 Temperature Echoes Temperature time protein in equilibrium probing signal synchronization signal temperature echoes   are sharp, resonance-like features in the time evolution of the protein’s temperature can be produced through 2 consecutive velocity reassignments (a kind of “interference” effect!)

5 Velocity Reassignments  protein ≈ collection of weakly interacting harmonic oscillators having different frequencies  at t 1 =0 the 1 st velocity reassignment: v i (0)= 1 u i synchronizes the oscillators (i.e., make them oscillate in phase)  at t 2 =  (delay time) the 2 nd velocity reassignment: v i (  )= 2 u i probes the degree of coherence of the system at that moment  degree of coherence is characterized by: - the time(s) of the echo(es) - the depth of the echo(es)

6 Producing Temperature Echoes by Velocity Reassignments in Proteins 1 st velocity assignment 2nd velocity assignment time No heat bath coupling RelaxationEquilibration coupling to a heat bath: T=To No heat bath coupling Equilibrium Relaxation No heat bath coupling echo Temperature quench echoes:Const velocity reassignment echoes:Velocity reassignment echoes:

7 Generating T-Quench Echo: Step1 your system is ubiquitin (1UBQ) in vacuum, pre-equilibrated at T 0 =300K run all simulations in the microcanonical (NVE) ensemble psf, pdb and starting binary coordinate and velocity files are available in “common/” use NAMD2 configuration file “equil.conf” located in “01_equil_NVE/” to complete a 500 fs (# simulation steps) run extract the temperature time series T(t) from the NAMD2 log (output) file plot T(t) calculate: 1 0

8 Temperature Autocorrelation Function time [fs] C(t) [K 2 ] Temperature relaxation time: Mean temperature: RMS temperature:

9 Generating T-Quench Echo: Step2  1/2 Perform the 1 st temperature quench start a new simulation using configuration file “quench.conf” located in “02_quencha/” use the restart coordinate file from the previous run set all velocities to zero (i.e., set T=0) run the simulation for  number of steps (time step = 1 fs) extract (from the log file) and plot T(t) 1 0

10 Generating T-Quench Echo: Step3  1/2 1/4 22 1/8 1 0 Perform the 2 nd temperature quench start a new simulation using configuration file “quench.conf” located in “03_quenchb/” use the restart coordinate file from the previous run set again all velocities to zero (i.e., set T=0) run the simulation for 3  number of steps (time step = 1 fs) extract (from the log file) and plot T(t) You should discover a temperature echo at 2 

11 Explanation of the T-Quench Echo Assumption: protein ≈ collection of weakly interacting harmonic oscillators with dispersion Step1: Step2: Step3:

12 T-Quench Echo: Harmonic Approximation The average must be taken over the distribution of initial phases θ 0, amplitudes A 0 and angular velocities ω

13 T-Quench Echo: Harmonic Approximation  1/2 1/4 22 1/8 1 0

14 T(t) and C TT (t) It can be shown that:

15 T-Quench Echo: Harmonic Approximation time [fs] Temperature [K] 500

16 Dephasing Time of T-Quench Echoes

17 Constant Velocity Reassignment Echo ? 1 2/3 1/3 Can we get temperature echo(es) by reassigning the same set of atomic velocities (corresponding to T 0 !) at t = 0 and t =  ? 0 Answer: YES!

18 Is it possible to produce temperature echo with a single velocity reassignment ? YES! Reset all velocities at time  to the values at a previous instant of time, i.e., t = 0


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