[gmx-developers] details about Heat capacity caculation
Haiqing Zhao
haizhao at mtu.edu
Tue Nov 1 20:15:28 CET 2011
Hi, David,
thanks for reply.
I checked it. Version 4.5.5 really makes a difference from 4.5.3 which I used.
In 4.5.5, Cv works exactly well by nmol*(RMSD(E))^2/RT^2. (Even though I dont know here why need to multiply the # of molecular.)
But still I'm sure the Cp is not from simple Enthalpy Fluctuation, as you see from the example below--167296 J/mol, and there is several orders mistake.
Please help me check it.
Thanks.
e.g.
Enthalpy -17216.8 4.2 167.296 22.4922 (kJ/mol)
You may want to use the -driftcorr flag in order to correct
for spurious drift in the graphs. Note that this is not
a substitute for proper equilibration and sampling!
Temperature dependent fluctuation properties at T = 300.076.
Heat capacities obtained from fluctuations do *not* include
quantum corrections. If you want to get a more accurate estimate
please use the g_dos program.
WARNING: Please verify that your simulations are converged and perform
a block-averaging error analysis (not implemented in g_energy yet)
Volume = 1.8548e-05 m^3/mol
Enthalpy = -37.0255 kJ/mol
Coefficient of Thermal Expansion Alpha_P = 0.0129106 (1/K)
Isothermal Compressibility Kappa = 3.00555e-10 (J/m^3)
Adiabatic bulk modulus = 3.32718e+09 (m^3/J)
Heat capacity at constant pressure Cp = 80.3937 J/mol K
On Nov 1, 2011, at 2:05 PM, David van der Spoel wrote:
> On 2011-11-01 16:54, Haiqing Zhao wrote:
>>
>> Dear Gmxers,
>>
>> I have one question about how Gromacs calculate the heat capacity. I dont think it is only Enthalpy fluctuation÷(kT^2) in NPT ensemble. And also I checked it in NVT, it is not simply Total energy(/internal energy) fluctuation÷(kT^2).
>>
> Which gmx version? It's more or less correct in 4.5.4 but you really need qm correctiions. Check g_dos for that
>
>
>
>
>> One data for NPT is: ( -nmol 465 -nconstr 3 )
>>
>> Energy Average Err.Est. RMSD Tot-Drift
>> -------------------------------------------------------------------------------
>> Potential -44.6187 0.007 0.293318 0.0281861 (kJ/mol)
>> Kinetic En. 7.59226 0.0032 0.19886 0.0201858 (kJ/mol)
>> Total Energy -37.0264 0.0091 0.359776 0.0483719 (kJ/mol)
>> Temperature 300.076 0.13 7.85971 0.797822 (K)
>> Pressure 0.663728 0.16 447.392 -0.388627 (bar)
>> Volume 14.3219 0.0093 0.133543 -0.0667073 (nm^3)
>> pV 0.438734 9.5e-05 0.00136276 -0.000679764 (kJ/mol)
>> Enthalpy -17216.8 4.2 167.296 22.4922 (kJ/mol)
>>
>> Temperature dependent fluctuation properties at T = 300.076. #constr/mol = 3
>> Isothermal Compressibility: 3.00555e-05 /bar
>> Adiabatic bulk modulus: 33271.8 bar
>> Heat capacity at constant pressure Cp: 67.9219 J/mol K
>> Thermal expansion coefficient alphaP: 9.66233e-05 1/K
>>
>> And data for NVT, ( -nmol 7631 -nconstr 3 )
>>
>> Energy Average Err.Est. RMSD Tot-Drift
>> -------------------------------------------------------------------------------
>> Total Energy -33.2264 0.0003 0.0900307 -0.000219237 (kJ/mol)
>> Temperature 300.008 0.0063 1.95324 -0.0148441 (K)
>>
>> Temperature dependent fluctuation properties at T = 300.008. #constr/mol = 3
>> Heat capacity at constant volume Cv: 70.1813 J/mol K
>>
>> (BTW, I found that (1)if you choose Enthalpy as output, g_energy will always give Cp, no matter what ensemble it is. (2)And only you choose tot energy and temp as output, no other terms, g_energy will give you Cv. If not, you cannot get Cv by g_energy.)
>>
>> I appreciate if anybody could help me to check it.
>> Thanks!!
>>
>> ---------------------------------------------
>> Haiqing Zhao
>> PH.D. candidate
>> in Computational Biophysics
>> Michigan Technological University
>> http://www.phy.mtu.edu/~haizhao
>>
>
>
> --
> David van der Spoel, Ph.D., Professor of Biology
> Dept. of Cell & Molec. Biol., Uppsala University.
> Box 596, 75124 Uppsala, Sweden. Phone: +46184714205.
> spoel at xray.bmc.uu.se http://folding.bmc.uu.se
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