.TH g_dielectric 1 "Mon 4 Apr 2011" "" "GROMACS suite, VERSION 4.5.4-dev-20110404-bc5695c" .SH NAME g_dielectric - calculates frequency dependent dielectric constants .B VERSION 4.5.4-dev-20110404-bc5695c .SH SYNOPSIS \f3g_dielectric\fP .BI "\-f" " dipcorr.xvg " .BI "\-d" " deriv.xvg " .BI "\-o" " epsw.xvg " .BI "\-c" " cole.xvg " .BI "\-[no]h" "" .BI "\-[no]version" "" .BI "\-nice" " int " .BI "\-b" " time " .BI "\-e" " time " .BI "\-dt" " time " .BI "\-[no]w" "" .BI "\-xvg" " enum " .BI "\-[no]fft" "" .BI "\-[no]x1" "" .BI "\-eint" " real " .BI "\-bfit" " real " .BI "\-efit" " real " .BI "\-tail" " real " .BI "\-A" " real " .BI "\-tau1" " real " .BI "\-tau2" " real " .BI "\-eps0" " real " .BI "\-epsRF" " real " .BI "\-fix" " int " .BI "\-ffn" " enum " .BI "\-nsmooth" " int " .SH DESCRIPTION \&\fB g_dielectric\fR calculates frequency dependent dielectric constants \&from the autocorrelation function of the total dipole moment in \&your simulation. This ACF can be generated by \fB g_dipoles\fR. \&For an estimate of the error you can run g_statistics on the \&ACF, and use the output thus generated for this program. \&The functional forms of the available functions are: \&One parameter: y = Exp[\-a1 x], \&Two parameters: y = a2 Exp[\-a1 x], \&Three parameters: y = a2 Exp[\-a1 x] + (1 \- a2) Exp[\-a3 x]. \&Start values for the fit procedure can be given on the command line. \&It is also possible to fix parameters at their start value, use \fB \-fix\fR \&with the number of the parameter you want to fix. \& \&Three output files are generated, the first contains the ACF, \&an exponential fit to it with 1, 2 or 3 parameters, and the \&numerical derivative of the combination data/fit. \&The second file contains the real and imaginary parts of the \&frequency\-dependent dielectric constant, the last gives a plot \&known as the Cole\-Cole plot, in which the imaginary \&component is plotted as a function of the real component. \&For a pure exponential relaxation (Debye relaxation) the latter \&plot should be one half of a circle. .SH FILES .BI "\-f" " dipcorr.xvg" .B Input xvgr/xmgr file .BI "\-d" " deriv.xvg" .B Output xvgr/xmgr file .BI "\-o" " epsw.xvg" .B Output xvgr/xmgr file .BI "\-c" " cole.xvg" .B Output xvgr/xmgr file .SH OTHER OPTIONS .BI "\-[no]h" "no " Print help info and quit .BI "\-[no]version" "no " Print version info and quit .BI "\-nice" " int" " 19" Set the nicelevel .BI "\-b" " time" " 0 " First frame (ps) to read from trajectory .BI "\-e" " time" " 0 " Last frame (ps) to read from trajectory .BI "\-dt" " time" " 0 " Only use frame when t MOD dt = first time (ps) .BI "\-[no]w" "no " View output \fB .xvg\fR, \fB .xpm\fR, \fB .eps\fR and \fB .pdb\fR files .BI "\-xvg" " enum" " xmgrace" xvg plot formatting: \fB xmgrace\fR, \fB xmgr\fR or \fB none\fR .BI "\-[no]fft" "no " use fast fourier transform for correlation function .BI "\-[no]x1" "yes " use first column as \fI x\fR\-axis rather than first data set .BI "\-eint" " real" " 5 " Time to end the integration of the data and start to use the fit .BI "\-bfit" " real" " 5 " Begin time of fit .BI "\-efit" " real" " 500 " End time of fit .BI "\-tail" " real" " 500 " Length of function including data and tail from fit .BI "\-A" " real" " 0.5 " Start value for fit parameter A .BI "\-tau1" " real" " 10 " Start value for fit parameter tau1 .BI "\-tau2" " real" " 1 " Start value for fit parameter tau2 .BI "\-eps0" " real" " 80 " epsilon0 of your liquid .BI "\-epsRF" " real" " 78.5 " epsilon of the reaction field used in your simulation. A value of 0 means infinity. .BI "\-fix" " int" " 0" Fix parameters at their start values, A (2), tau1 (1), or tau2 (4) .BI "\-ffn" " enum" " none" Fit function: \fB none\fR, \fB exp\fR, \fB aexp\fR, \fB exp_exp\fR, \fB vac\fR, \fB exp5\fR, \fB exp7\fR, \fB exp9\fR or \fB erffit\fR .BI "\-nsmooth" " int" " 3" Number of points for smoothing .SH SEE ALSO .BR gromacs(7) More information about \fBGROMACS\fR is available at <\fIhttp://www.gromacs.org/\fR>.