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exercises:2017_uzh_acpc2:prot_fol [2017/05/17 12:00] – [Background] vrybkinexercises:2017_uzh_acpc2:prot_fol [2020/08/21 10:15] (current) – external edit 127.0.0.1
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 ====== Protein Folding in Solution ====== ====== Protein Folding in Solution ======
-In this exercise, you will calculate the protein folding free energy in aqueous solution using thermodynamic integration, a method based on molecular dynamics (MD). The protein will be described by the empirical force field, CHARMM.+In this exercise, you will calculate the protein folding free energy in aqueous solution using thermodynamic integration, a method based on molecular dynamics (MD). The protein will be described by the empirical force field, CHARMM, [[http://mackerell.umaryland.edu/charmm_ff.shtml]]
  
 ===== Background ===== ===== Background =====
-A model protein you will have to deal with is the alanine decapeptide. The folding/unfolding will be achieved by fixing the distance between the end carbon atoms in the chain: atoms 7 and 98. This distance is called a collective variable. At each distance one runs the MD simulation (constrained MD) to extract the time-averaged forces acting on the collective variable, $F(x)$. Then, a free energy difference can be calculated via thermodynamic integration (TI):+A model protein you will have to deal with is the alanine decapeptide. The folding/unfolding will be achieved by stretching/compressing the chain and fixing the distance between the end carbon atoms in it: atoms 7 and 98. This distance is called a collective variable. At each distance one runs the MD simulation (constrained MD) to extract the time-averaged forces acting on the collective variable, $F(x)$. Then, a free energy difference can be calculated via thermodynamic integration (TI):
  
 \begin{equation} \begin{equation}
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 Here $a$ and $b$ are the initial and the final values of the collective variable. TI is a general method, which can be applied to a variety of processes, e.g. phase transitions, electron transfer etc.  Here $a$ and $b$ are the initial and the final values of the collective variable. TI is a general method, which can be applied to a variety of processes, e.g. phase transitions, electron transfer etc. 
  
-===== 1. Task: Familiarize yourself =====+===== Task 1: Familiarize yourself =====
 Download the files: {{ :exercises:2017_uzh_acpc2:deca_ala.tar.gz |}} Download the files: {{ :exercises:2017_uzh_acpc2:deca_ala.tar.gz |}}
  
  
-**deca_ala.pdb** (protein data base) file contains the coordinates +''deca_ala.pdb'' (protein data base) file contains the coordinates 
  
-**deca_ala.psf** (protein structure file) file contains connectivity data+''deca_ala.psf'' (protein structure file) file contains connectivity data
  
-**par_all27_prot_lipid.inp** contains the force field parameters+''par_all27_prot_lipid.inp'' contains the force field parameters
  
-**md_1836.inp** is the CP2K input file+''md_1836.inp'' is the CP2K input file
  
- Open the **deca_ala.pdb** protein data bank format file with **vmd**. Create a new representation for the protein, e.g. of type **Ribbon** to observe the alpha-helix.+ Open the ''deca_ala.pdb'' protein data bank format file with **vmd**. Create a new representation for the protein, e.g. of type **Ribbon** to observe the alpha-helix.
 {{ :exercises:2017_uzh_acpc2:deca_ala.gif?400 |}} {{ :exercises:2017_uzh_acpc2:deca_ala.gif?400 |}}
 +
 +===== Task 2: Perform constrained MD simulations =====
 +For that you have to run MD for different values of the distance between atoms 7 and 98, in each run it will be constrained. In the original file ''md_1836.inp'' it is set to $18.36$ Å as is in the ''deca_ala.pdb'' file.  
 +
 +   - Run CP2K with ''md_1836.inp''
 +   - Copy ''md_1836.inp'' to smth. like ''md_1536.inp'';
 +   - Modify the PROJECT_NAME and ''TARGET'' value in the ''CONSTRAINT'' section for a new value: here 15.36;
 +   - Run CP2K with the new input file;
 +   - Repeat for several values in the range $15$ to $20 $ Å.
 +
 +<note tip>
 +  * To avoid confusion, try to perfrom every task in a new directory 
 +  * You may increase or decrease the number of MD steps, which is set to 5000 in the file, to speed-up the calculation or else get a better statiscics.
 +</note>
 +
 +==== Constraint section TO BE modified for constrained MD ====
 +<code - constraint section>
 + &CONSTRAINT
 +    &COLLECTIVE
 +      COLVAR 1
 +      INTERMOLECULAR
 +      TARGET [angstrom] 18.36
 +    &END COLLECTIVE
 +    &LAGRANGE_MULTIPLIERS
 +      COMMON_ITERATION_LEVELS 1
 +    &END
 + &END CONSTRAINT
 +</code>
 +
 +===== Task 3: Evaluate the free energy difference =====
 +⇒ Each constrained MD will produce a ''.LagrangeMultLog''-files, which look like this:
 +<code>
 +Shake  Lagrangian Multipliers:           -63.547262596
 +Rattle Lagrangian Multipliers:            63.240598387
 +Shake  Lagrangian Multipliers:            -0.326901815
 +Rattle Lagrangian Multipliers:            -0.318145579
 +</code>
 +
 +<note warning>
 +Make sure that you get the units right. The Largange multipliers are written in atomic units (Hartree/bohr), while the distances are in Angstrom.
 +</note>
 +
 +  * From these files you can calculate the average Lagrange multiplier of the Shake-algorithm like this:
 +<code>
 +grep Shake yourprojectname.LagrangeMultLog | awk '{c++ ; s=s+$4}END{print s/c}'
 +</code>
 +
 +  * The average Lagrange multiplier is the average force $F(x)$ required to constrain the atoms at the distance $x$.
 +  * From these forces the free energy difference can be obtained via TI (see **Background**)
 +
 +
 +<note tip>
 +  * Calculate $\Delta A$ numerically using the trapezoidal rule (or equivalent) with EXCEL, ORIGIN or any scripting language.
 +</note>
 +
 +
exercises/2017_uzh_acpc2/prot_fol.1495022445.txt.gz · Last modified: 2020/08/21 10:15 (external edit)