"from the [TT]ener.edr[tt] file.[PAR]",
"With [TT]-fee[tt] an estimate is calculated for the free-energy",
- "difference with an ideal gas state: [BR]",
- " [GRK]Delta[grk] A = A(N,V,T) - A[SUB]idealgas[sub](N,V,T) = kT [LN][CHEVRON][EXP]U[SUB]pot[sub]/kT[exp][chevron][ln][BR]",
- " [GRK]Delta[grk] G = G(N,p,T) - G[SUB]idealgas[sub](N,p,T) = kT [LN][CHEVRON][EXP]U[SUB]pot[sub]/kT[exp][chevron][ln][BR]",
+ "difference with an ideal gas state::",
+ "",
+ " [GRK]Delta[grk] A = A(N,V,T) - A[SUB]idealgas[sub](N,V,T) = kT [LN][CHEVRON][EXP]U[SUB]pot[sub]/kT[exp][chevron][ln]",
+ " [GRK]Delta[grk] G = G(N,p,T) - G[SUB]idealgas[sub](N,p,T) = kT [LN][CHEVRON][EXP]U[SUB]pot[sub]/kT[exp][chevron][ln]",
+ "",
"where k is Boltzmann's constant, T is set by [TT]-fetemp[tt] and",
"the average is over the ensemble (or time in a trajectory).",
"Note that this is in principle",
"only correct when averaging over the whole (Boltzmann) ensemble",
"and using the potential energy. This also allows for an entropy",
- "estimate using:[BR]",
- " [GRK]Delta[grk] S(N,V,T) = S(N,V,T) - S[SUB]idealgas[sub](N,V,T) = ([CHEVRON]U[SUB]pot[sub][chevron] - [GRK]Delta[grk] A)/T[BR]",
+ "estimate using::",
+ "",
+ " [GRK]Delta[grk] S(N,V,T) = S(N,V,T) - S[SUB]idealgas[sub](N,V,T) = ([CHEVRON]U[SUB]pot[sub][chevron] - [GRK]Delta[grk] A)/T",
" [GRK]Delta[grk] S(N,p,T) = S(N,p,T) - S[SUB]idealgas[sub](N,p,T) = ([CHEVRON]U[SUB]pot[sub][chevron] + pV - [GRK]Delta[grk] G)/T",
- "[PAR]",
+ "",
"When a second energy file is specified ([TT]-f2[tt]), a free energy",
- "difference is calculated [BR] dF = -kT [LN][CHEVRON][EXP]-(E[SUB]B[sub]-E[SUB]A[sub])/kT[exp][chevron][SUB]A[sub][ln] ,",
+ "difference is calculated::",
+ "",
+ " dF = -kT [LN][CHEVRON][EXP]-(E[SUB]B[sub]-E[SUB]A[sub])/kT[exp][chevron][SUB]A[sub][ln] ,",
+ "",
"where E[SUB]A[sub] and E[SUB]B[sub] are the energies from the first and second energy",
"files, and the average is over the ensemble A. The running average",
"of the free energy difference is printed to a file specified by [TT]-ravg[tt].",