gmx tcaf [-f[<.trr/.cpt/...>]] [-s[<.tpr/.gro/...>]] [-n[<.ndx>]] [-ot[<.xvg>]] [-oa[<.xvg>]] [-o[<.xvg>]] [-of[<.xvg>]] [-oc[<.xvg>]] [-ov[<.xvg>]] [-b<time>] [-e<time>] [-dt<time>] [-[no]w] [-xvg<enum>] [-[no]mol] [-[no]k34] [-wt<real>] [-acflen<int>] [-[no]normalize] [-P<enum>] [-fitfn<enum>] [-beginfit<real>] [-endfit<real>]

`gmx tcaf` computes tranverse current autocorrelations.
These are used to estimate the shear viscosity, eta.
For details see: Palmer, Phys. Rev. E 49 (1994) pp 359-366.

Transverse currents are calculated using the
k-vectors (1,0,0) and (2,0,0) each also in the *y*- and *z*-direction,
(1,1,0) and (1,-1,0) each also in the 2 other planes (these vectors
are not independent) and (1,1,1) and the 3 other box diagonals (also
not independent). For each k-vector the sine and cosine are used, in
combination with the velocity in 2 perpendicular directions. This gives
a total of 16*2*2=64 transverse currents. One autocorrelation is
calculated fitted for each k-vector, which gives 16 TCAFs. Each of
these TCAFs is fitted to f(t) = exp(-v)(cosh(Wv) + 1/W sinh(Wv)),
v = -t/(2 tau), W = sqrt(1 - 4 tau eta/rho k^2), which gives 16 values of tau
and eta. The fit weights decay exponentially with time constant w (given with `-wt`) as exp(-t/w), and the TCAF and
fit are calculated up to time 5*w.
The eta values should be fitted to 1 - a eta(k) k^2, from which
one can estimate the shear viscosity at k=0.

When the box is cubic, one can use the option `-oc`, which
averages the TCAFs over all k-vectors with the same length.
This results in more accurate TCAFs.
Both the cubic TCAFs and fits are written to `-oc`
The cubic eta estimates are also written to `-ov`.

With option `-mol`, the transverse current is determined of
molecules instead of atoms. In this case, the index group should
consist of molecule numbers instead of atom numbers.

The k-dependent viscosities in the `-ov` file should be
fitted to eta(k) = eta_0 (1 - a k^2) to obtain the viscosity at
infinite wavelength.

**Note:** make sure you write coordinates and velocities often enough.
The initial, non-exponential, part of the autocorrelation function
is very important for obtaining a good fit.

Options to specify input files:

`-f`[<.trr/.cpt/...>] (traj.trr)- Full precision trajectory:
*trr**cpt**tng* `-s`[<.tpr/.gro/...>] (topol.tpr) (Optional)- Structure+mass(db):
*tpr**gro**g96**pdb*brk ent `-n`[<.ndx>] (index.ndx) (Optional)- Index file

Options to specify output files:

`-ot`[<.xvg>] (transcur.xvg) (Optional)- xvgr/xmgr file
`-oa`[<.xvg>] (tcaf_all.xvg)- xvgr/xmgr file
`-o`[<.xvg>] (tcaf.xvg)- xvgr/xmgr file
`-of`[<.xvg>] (tcaf_fit.xvg)- xvgr/xmgr file
`-oc`[<.xvg>] (tcaf_cub.xvg) (Optional)- xvgr/xmgr file
`-ov`[<.xvg>] (visc_k.xvg)- xvgr/xmgr file

Other options:

`-b`<time> (0)- First frame (ps) to read from trajectory
`-e`<time> (0)- Last frame (ps) to read from trajectory
`-dt`<time> (0)- Only use frame when t MOD dt = first time (ps)
`-[no]w`(no)- View output
*.xvg*,*.xpm*,*.eps*and*.pdb*files `-xvg`<enum>- xvg plot formatting: xmgrace, xmgr, none
`-[no]mol`(no)- Calculate TCAF of molecules
`-[no]k34`(no)- Also use k=(3,0,0) and k=(4,0,0)
`-wt`<real> (5)- Exponential decay time for the TCAF fit weights
`-acflen`<int> (-1)- Length of the ACF, default is half the number of frames
`-[no]normalize`(yes)- Normalize ACF
`-P`<enum> (0)- Order of Legendre polynomial for ACF (0 indicates none): 0, 1, 2, 3
`-fitfn`<enum> (none)- Fit function: none, exp, aexp, exp_exp, exp5, exp7, exp9
`-beginfit`<real> (0)- Time where to begin the exponential fit of the correlation function
`-endfit`<real> (-1)- Time where to end the exponential fit of the correlation function, -1 is until the end