molecular simulation strategies for large scale thermodynamic … · 2017. 2. 6. ·...
TRANSCRIPT
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Molecular Simulation Strategies for
Large Scale Thermodynamic Data
Generation
Athens, 2. Sept. 2011
Gábor Rutkai
Rolf Lustig
Jadran Vrabec
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
R. Span, “Multiparameter Equations of State”, Springer, Berlin (2000)
complete thermodynamic knowledge : ~10 substances
For pure chemical substances…
satisfactory knowledge :
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Equations of state for CO2 (Span and Wagner, 1996)
0 ResF , , ,R T
7
0 0 0 0 0
1 2 3 i i
i 4
, ln a a a ln a ln 1 exp n
i i i i i7 34
t d t d cRes
i i
i 1 i 8
, a a exp
i i39
t d 2 2
i i i i i
i 35
a exp ( ) ( )
Ideal part:
Residual part:
Helmholtz Energy: T = 216 … 1100 K, p = 0 … 800 MPa
i42
b 2 2
i i i
i 40
a exp C ( 1) D ( 1)
Total:
49 Parameters
153 Exponents
5 013 exp. Data
TTc / c /
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Contribution of molecular simulation
• powerful predictive capabilities (thermodynamic data)
• works under any physical conditions
• low cost
Why is molecular simulation not a mainstream solution for
thermodynamic data retrieval?
• suitable molecular models
• today’s MS software: only a few independent properties
• new properties require implementation
• development is impossible for an inexperienced user
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
• Cv
Equilibrium thermodynamic properties
particular thermodynamic property
specific statistical mechanical ensembles or special techniques
NVT NpT • Cp
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Approach
For any thermodynamic property the underlying statistical
mechanical ensemble is in principle irrelevant*.
* H.W. Graben, J.R. Ray, Mol. Phys., 80, 1183-1193 (1993)
NVT • Cp • Cv
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Project with ms2*(www.ms-2.de):
• large set of thermodynamic properties from one NVT simulation
• truly independent thermodynamic information
• generation of an extensive dataset in an automatizable fashion
* S. Deublein et al., Comp. Phys. Comm., 182, 2350-2367 (2011).
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
The fundamental equation
(Helmholtz representation) (Massieu-Planck representation)
dnpdVTdSdU dnT
dVT
pdU
TdS
1
Legendre transformation
dnpdVSdTdF dnT
dVT
p
TUdd
1
(Energy representation) (Entropy representation)
TF /
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Derivatives of the Massieu-Planck potential
UV
U
2U2
2
V
U
3U3
3
V
U
…
TF /
mn
nmmn
nmT
T
/1/1
2
2
V
U
nU
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
......n
iajb
iajb
n
n
iajbn
n
r
ur
V
U
K. Meier and S. Kabelac, J. Chem. Phys., 124, 064104 (2006)
How to Calculate ? nn VU /
iajbiajb ru
2
)(
1
)(
11
1
13
1
iajb
ijiajb
iajb
iajb
iajb
jM
b
iM
a
N
ij
N
i rr
ur
VV
Up
rr
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Derivatives of the Massieu-Planck potential
TF /
mn
nmmn
nmT
T
/1/1
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Derivatives of the Massieu-Planck potential
011 Tp 10TU 10011 TH
20vC
0201
2
110120
1
1
pC
20
2
11010201
2 121Tw
21101
2
2002
110102
//
/
TT
TVJT
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
*T. Merker, J. Vrabec and H. Hasse, Fluid Phase Equilib., submitted (2011)
6CLJ united-atom model*
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EOSEOSsim HHH /100
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
• ms2 (MD, MC)
• 20 h (8 “nehalem” core per simulation)
• automatized (no user interaction)
• T = 500 K
• ρ = 6.35 – 8.0 mol L-1
• 40 state points
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane T = 500 K
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
T = 500 K
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Cyclohexane
...,,,,/100 pvEOSEOSsim CCHXXXX
H %5.1
EoS: R. Span, and W. Wagner, Int. J. Thermophys., 24, 41-109 (2003).
U %6.1
VC %8.0
pC %2.3
w %7.5
p %8.2
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Conclusion
• Good cyclohexane potential model
• Apporach is feasible for EoS development
• Large set of independent thermodynamic properties
• From a single NVT simulation per state point
• Execution of NVT simulations is well automatizable
• Computational cost is an additional pair potential evaluation
for each volume derivative order
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Thank you for listening!
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Derivative with respect to the Temperature
NVTZTF ln
V
NVT
NVT
NVT
V
NVT
V T
Z
ZTZ
T
ZT
T
FS
1ln
ln
2T
UTNVTZln
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Derivative with respect to the Temperature
NVTZTTF ln NVTZln
V
NVT
NVTV
NVT
V
Z
Z
Z
1ln
NN
NN
V
NVT
NVTV dUVN
dUUVNZ
Zr
r
exp
!
1
exp!
1
1
NNNVT dUVN
Z r exp!1
NNNVT dUUVN
Zr
exp
!
1
U
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Derivative with respect to the Temperature
NVTZTF ln NVTZln
V
NVT
VT
Z
T
)/1(
ln
)/1(
U
V
NVTNVT
V T
ZTZ
T
F
lnln
2T
U
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PROF. DR.-ING. HABIL. JADRAN VRABEC ThET
Pair potentials
612
4iajbiajb
iajbrr
u
LJ LRC (site-site cutoff):
drr
ur
VN
V
U iajb
rc
3
LRC
3
12 .........
LRC
n
iajb
n
n
r
n
n
r
ur
V
U
c
3
RF
RF
12
11
c
iajb
iajb
jbia
iajbr
r
r
qqu
(Lennard-Jones potential) (reaction-field correction)