SDA
Simulation of Diffusional Association
(version 5.01)


Additional and auxiliary programs


SDA-KOFF
This program can use the same input file as sda, doing simulations starting from a docked configuration (as given by pdb files used as input to SDA).  The output of this program is a table of residence times (in ps), during which the contacts within a specified distance are maintained.  This can be considered to provide an estimate of the lifetime of the complex defined via these contacts.


SDA-SITE
This program calculates the fraction of trajectories starting with one complex (given by the original pdb files and potentials and charges derived from them) and ending with formation of another complex (defined by reaction criteria files).  To use it, prepare first standard SDA simulation files using the starting complex of 2 solutes.  To define the end-point of trajectories, you can either define reaction criteria manually, or use the SDA routine da-pairs with the same first solute and the second solute docked at the target position.  Parameter b (starting sphere) will not be used, parameter c (trajectory truncation distance) is used the same way as in the standard version.


SDA-ENER
This program
can use the same input file as sda to read in data about the solute molecules (pdb, charge, grid file names).
It will read in the protein coordinates from the file fort.55 and write coordinate information and energies to the file fort.56 . If the force field parameters in the input file are changed, or another grid/charge files are specified there, then this program will recalculate another set of energies for the same solute configurations.  It is important to have the same pdb files for both solutes; charges and grids can be recalculated from these pdb files using different calculation parameters.


SDA3G
This program
uses hydrophobic forces derived from a hydrophobic PMF (Lin, Fawzi, Head-Gordon (2007). Structure 15, 727) instead of buried surface area.  Use program mk_hd3g_grd.f to generate relevant grids.  Usage is the same as the standard SDA program.  Note that hdfct in this case is a simple scaling factor to scale the PMF, hdfct=1.0 is the recommended value.  Simulations may, however, last a long time with hdfct=1.0 .

ECM

A more detailed description of the ECM program is here .
ECM is located in the directory ecm/ of the SDA distribution.
To run SDA, the effective charges for 2 proteins can be prepared using a script like the one below:

#------------------------------------------
cp p1.pdb dum.pdb
\rm dum.grd; ln -s ep1.grd dum.grd
$ECM_BIN/ecm_mksites < p1.pdb > p1.tcha
$ECM_BIN/ecm_expand < ecm.in > ecm.ou
$ECM_BIN/ecm_regularize >> ecm.ou
$ECM_BIN/ecm_mkreglev  1.0 < ecm.ou > reg_lev
$ECM_BIN/ecm_mkecharges < reg_lev >> ecm.ou
\rm dum.echa dum.echa_E; mv ecm.ou ecm.ou-1
mv dum.echa_R p1.echa
#------------------------------------------
cp p2.pdb dum.pdb; cp p2.tcha dum.tcha
\rm dum.grd; ln -s ep2.grd dum.grd
$ECM_BIN/ecm_mksites < p2.pdb > p2.tcha
$ECM_BIN/ecm_expand < ecm.in > ecm.ou
$ECM_BIN/ecm_regularize >> ecm.ou
$ECM_BIN/ecm_mkreglev 1.0 < ecm.ou > reg_lev
$ECM_BIN/ecm_mkecharges < reg_lev >> ecm.ou
\rm dum.echa dum.echa_E; mv ecm.ou ecm.ou-2
mv dum.echa_R p2.echa
#------------------------------------------
The first part of this script is for the first solute and the second - for the second.  To generate effective charges for solute 1, ECM uses its pdb file p1.pdb (in standard PDB file format) and the file with the electrostatic potential ep1.grd (UHBD format).  Several ECM routines (located in a directory defined before running the script above as environmental variable ECM_BIN) perform the task of fitting electrostatic potentials to effective charges.  The parameter at the command line of the program ecm_mkreglev (1.0 in the script) defines the maximal deviation of the effective charges from the test charge values. The test charge sites and values are computed by ECM routine ecm_mksites and can be modified before executing further steps of the ECM script above.
Input file for the expansion routine can have a form like this :
------------------ pdb file name
dum.pdb
------------------ file with test charges for the molecule
dum.tcha
------------------ grid file name and its UHBD format (0-binary, 1 -ascii)
dum.grd
0
------------------ probe radius (A), skin thickness (A): expansion done in [probe; probe+skin] interval
4.0, 3.0
------------------ ionic strength (mM), solvent relative dielectric constant
 50., 78.
------------------ file to write effective charges to
dum.echa
------------------ nothing else

Alternatively, a recent version of ecm does all steps (after assigning test charge sites with ecm_mksites) with a single program, ecm_all, call. No re-calculation of charges using previously calculated fitting results is possible in ecm_all.
Usage:
ecm_all -fp fpdb -ft ftch -fg fgrd -gf gform -pr prob -sk skin -is ios -es epssol -rl reg_lev -rc regch -fe fech
where
fpdb pdb file name (dum.pdb)
ftch test charge file name (dum.tcha)
fgrd
electrostatic potential grid filename (dum.grd)
gform
ep grid file format, 0 =bin, 1 =ascii (0)
prob probe radius - to construct skin (4Å)
skin skin thickness (3Å)
ios ionic strength in mM (150 mM)
epssol solvent dielectric constant (78.5)
reglev regularisation level
regch max charge deviation after regularisation (1.0 e)
fec effective charge file name (dum.echa)
If some parameter is not specified, default values (in brackets) will be used. Note that only one version (_R, not divided by solvent dielectric) of effective charges are written.  You can use auxiliary program auxi/echa4toecha5 to do conversions if necessary.


mk_ed_grd

This program is located in the auxi/ directory of the SDA distribution.
mk_ed_grd reads in parameters from the input file, reads the pdb file for a solute as specified in the input file (p1.pdb in the file below) and write the electrostatic desolvation penalty potentials to the file specified in the input file (p1ed.grd). > mk_ed_grd < input_file > output_log_file
The input file can look like this:

#------------------------------ h,ndimx,ndimy,ndimz
1.0, 110,110,110
#------------------------------ iostr,epssol,rion
 50.  78.  2.0
#------------------------------ pfile
p1.pdb
#------------------------------ gfile, iform
p1ed.grd
0

Here, the first 4 parameters give the electrostatic desolvation grid spacing (Å) and the grid dimensions along the x,y,z directions.  The second set of parameters are for the ionic strength (mM), solvent dielectric constant and ion radius (A) relevant to defining the ionic strength conditions.  The last parameter is to define if the UHBD format output file is to be written in binary (0) or ascii (1) format. >
The output grid contains the electrostatic desolvation penalties for a unit charge due to the low dielectric cavity of the solute treated as a collection of atom-centered spheres having radii equal to atomic van der Waals radii, see reference.  For a fractional charge, one has to multiply the values on the grid with the square of the charge.  For more than one charge, this approach gives approximate desolvation penalties, because no mutual influence of these charges are taken into account .  The solute's low dielectric cavity as a region inside a molecular surface can be modeled by using a correction factor to this penalty, see reference .



mk_hd_grd

This program is located in the auxi/ directory of the SDA distribution.
mk_hd_grd reads in parameters from the input file, reads the pdb file for a solute as specified in the input file (p1.pdb in the file below) and write the hydrophobic desolvation penalty potentials to the file specified in the input file (p1hd.grd).  Usage:
mk_hd_grd < input_file > output_log_file
The input file can look like this:

#------------------------------ h,ndimx,ndimy,ndimz
1.0, 110,110,110
#------------------------------ a,b,factor
3.10, 4.35, 0.5
#------------------------------ pfile
p1.pdb
#------------------------------ gfile, iform
p1hd.grd
0


Here the first 4 parameters give the hydrophobic desolvation grid spacing (Å) and the grid dimensions along the x,y,z directions.  The second set of parameters specifies the region where this potential is defined and the scaling factor for the calculated potential.  The last parameter is to define if UHBD format output file is to be written in binary (0) or ascii (1) format.

This program assigns a value of gamma (parameter "factor" in the input file above) to a point if this point is within distance a (in Å) from the surface of the protein, zero if a point is further than b (in Å) from the surface and a linearly interpolated value if a point is inbetween:

In SDA, the solvent accessibilities of the atoms of the second solute are multiplied by the value of this grid at the location of the atoms of the second solute.  It appears that many different values of parameters a and b give the buried areas to an accuracy of ca 10%:


The errors above are for estimating the buried area for a collection of encounter complexes up to a constant factor, different values of a and b approximate the buried area with different factors.
Recommended values are a=3.10 Å and b= 4.35 Å and factor=0.5.  The value factor=0.5 is to compensate for the factor of 2 in calculating the buried area by multiplying the solvent accessible areas of atoms with the grid values calculated using the above values of a and b. With these parameters, the procedure used in SDA gives the most accurate approximation to the buried area.  With this parameters in mk_hd_grd, the parameter hdfct is a parameter to multiply the buried area to get the hydrophobic desolvation energy in units of kcal/mole/Å2. > If other values of a and b are used, it is recommended to calculate the hydrophobic desolvation energies for a set of encounter complexes using SDA and compare them to energies calculated differently to relate SDA energies to energies calculated using buried areas.




Other programs in the auxi/ directory of the SDA distribution.


apbs2uhbd.f Convert an APBS potential grid (exported as uhbd, in ascii format, in kT/e units) to UHBD format (binary, in kcal/mole). Default conversion factor is 0.6, the user can specify another factor on the command line as the third argument.  Usage:
apbs2uhbd ascii_APBS_file bin_UHBD_file factor_optonal(0.6)
ascii2bin.f
Converts UHBD ascii grid to binary format, usage:
ascii2bin ascii_file binary_file
bin2ascii.f
Converts UHBD binary grid to ascii format, usage:
bin2ascii binary_file ascii_file
echa4toecha5.f Converts effective charges used in version 4 of SDA to effective charges used in SDA version 5, see details here.  The former charges are obtained from the latter by dividing by the solvent dielectric constant. This is read from the ECM written REMARK line of the effective charge file, or set to 78.5 when no such line is found.  If a switch -inv is given in the command line, this program will do inverse conversion. Usage:
echa4toecha5 < sda4_eff_cha_file > sda5_eff_cha_file
echa4toecha5 -inv < sda5_eff_cha_file > sda4_eff_cha_file
mk_hd3g_grd.f Makes a grid of hydrophobic PMF (Lin, Fawzi, Head-Gordon (2007). Structure 15, 727).  These potentials should be used with sda version sda3g .  This program is used the same way as mk_hd_grd, with the input file of the same form, except that  parameters a,b and factor are not used (although the numbers and lines should be present).
ncmx2rmsd_appr.f Calculates (approximately) the RMSD of complexes written in the fort.55 file to the original (as given in input pdb files) complex.  Usage:
ncmx2rmsd_appr ncoa(optional) < fort.55
where the optional parameter ncoa forces the program to process only every ncoa-th record in the SDA trajectory file fort.55.
nda-pairs.f Calculates donor-acceptor pairs for a complex given as 2 pdb files. Usage:
nda-pairs pdb1f pdb2f cutmax
where pdb1f is the filename of the first solute in the complex and pdb2f is the filename for the second solute.  cutmax is a maximal distance (in A) between  donor and acceptor atoms, default value of 4.5 A is used if this parameter is not given.  The results are written to files 1.rxna and 2.rxna - these are donor or acceptor atoms of the first and second solute, respectively; and the atom on the N-th line of 1.rxna is a pair for the atom on the N-th line of 2.rxna.
nhis2dcd.f Converts the trajectory written by SDA in a fort.55 file to a DCD format.  Usage:
nhis2dcd pdbf hisf outf
pdbf - pdb filename of the 2nd (mobile) solute
hisf - trajectory file (fort.55) name
outf - output DCD filename
nhis2his.f Rewrites a trajectory file to another trajectory file with configurations written only every given time interval (in picoseconds). Usage:
nhis2his dt < hisf1 > hisf2
dt - time interval (ps) between snapshots in a new trajectory file
hisf1 - original trajectory file
hisf2 - new (converted) trajectory file
nhis2hisn.f Rewrites a trajectory file to another trajectory file with configurations written only every given number of BD steps. Usage:
nhis2his ncoa < hisf1 > hisf2
ncoa - interval between snapshots in a new trajectory file
hisf1 - original trajectory file
hisf2 - new (converted) trajectory file
nhis2pdbs.f Converts complexes in a file fort.55 to a set of PDB files. Usage:
nhis2pdbs hisf pdbf X nmax
hisf - trajectory file
pdbf - pdb file for the mobile solute
X    - first letter for generated pdb files (these file will have names like X1234.pdb)
nmax - a number of trajectory records to process
nos2rates.f Extracts rates and calculates averages and deviations from a set of sda output files. Usage:
nos2rates outf1 outf2 outf3 ...
outf1 etc - sda output files
nos2times.f
Extracts residence times and calculate averages and deviations from a set of sda-koff output files. Usage:
nos2times outf1 outf2 outf3 ...
outf1 etc - sda-koff output files
nos2fractions.f Extracts a fraction of reactive trajectories and calculates average and deviation from a set of sda-sites output files. Usage:
nos2fractions outf1 outf2 outf3 ...
outf1 etc - sda-sites output files
rewrite-pdb.f
Rewrites ATOM records of pdb file to locate the first atom name letter at position 13.  Optionally writes only heavy atoms.  Usage:
rewrite-pdb < pdb-file > rewritten-pdb-file
rewrite-pdb -noh < pdb-file > pdb-file-without-hydrogens



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