Molecular docking of α-cyclodextrin inclusion complexes by genetic algorithm and empirical binding free energy function

2001 ◽  
Vol 342 (3-4) ◽  
pp. 387-396 ◽  
Author(s):  
Wensheng Cai ◽  
Baoyun Xia ◽  
Xueguang Shao ◽  
Qingxiang Guo ◽  
B. Maigret ◽  
...  
Author(s):  
Garrett M. Morris ◽  
David S. Goodsell ◽  
Robert S. Halliday ◽  
Ruth Huey ◽  
William E. Hart ◽  
...  

ChemInform ◽  
2011 ◽  
Vol 42 (30) ◽  
pp. no-no
Author(s):  
Wen Sheng Cai ◽  
Teng Wang ◽  
Ying Zhe Liu ◽  
Peng Liu ◽  
Christophe Chipot ◽  
...  

2001 ◽  
Vol 535 (1-3) ◽  
pp. 115-119 ◽  
Author(s):  
Wensheng Cai ◽  
Baoyun Xia ◽  
Xueguang Shao ◽  
Qingxiang Guo ◽  
B. Maigret ◽  
...  

2011 ◽  
Vol 15 (6) ◽  
pp. 839-847 ◽  
Author(s):  
Wen Sheng Cai ◽  
Teng Wang ◽  
Ying Zhe Liu ◽  
Peng Liu ◽  
Christophe Chipot ◽  
...  

1983 ◽  
Vol 48 (10) ◽  
pp. 2888-2892 ◽  
Author(s):  
Vilém Kodýtek

A special free energy function is defined for a solution in the osmotic equilibrium with pure solvent. The partition function of the solution is derived at the McMillan-Mayer level and it is related to this special function in the same manner as the common partition function of the system to its Helmholtz free energy.


2021 ◽  
Vol 183 (3) ◽  
Author(s):  
Bart van Ginkel ◽  
Bart van Gisbergen ◽  
Frank Redig

AbstractWe study a model of active particles that perform a simple random walk and on top of that have a preferred direction determined by an internal state which is modelled by a stationary Markov process. First we calculate the limiting diffusion coefficient. Then we show that the ‘active part’ of the diffusion coefficient is in some sense maximal for reversible state processes. Further, we obtain a large deviations principle for the active particle in terms of the large deviations rate function of the empirical process corresponding to the state process. Again we show that the rate function and free energy function are (pointwise) optimal for reversible state processes. Finally, we show that in the case with two states, the Fourier–Laplace transform of the distribution, the moment generating function and the free energy function can be computed explicitly. Along the way we provide several examples.


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