1964
DOI: 10.1021/ed041p619
|View full text |Cite
|
Sign up to set email alerts
|

Systematic names for the tartaric acids

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
7
0

Year Published

1965
1965
2015
2015

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 6 publications
(7 citation statements)
references
References 0 publications
0
7
0
Order By: Relevance
“…In bulk, the one-body direct correlation function becomes spatially constant and Equation (15) is equivalent to the first of Baxter's sum rules [11]:…”
Section: Integration Of the Direct Correlation Functionsmentioning
confidence: 99%
“…In bulk, the one-body direct correlation function becomes spatially constant and Equation (15) is equivalent to the first of Baxter's sum rules [11]:…”
Section: Integration Of the Direct Correlation Functionsmentioning
confidence: 99%
“…The particle densities n k depend on the temperature T and on the number density n of the system. In 1964, Baxter [1] proved an elegant hierarchy relating the derivative of n k with respect to density with an integral of n k+1 , namely…”
Section: Multi-particle Correlation Functionsmentioning
confidence: 99%
“…In order to study this question we use the infinite hierarchy of equations derived by Baxter [1]. The hierarchy relates the spatial integrals of (k + 1)-particle correlation functions to k-particle correlations and their derivatives with respect to the density, for k = 2, 3, .…”
Section: Introductionmentioning
confidence: 99%
“…Thus the entropy of a free spin with average magnetisation m i is simply the Gibbs mixing entropy of two ideal gases with mole fractions (1 + m i )/2 and (1 − m i )/2, per particle. Now, the excess term includes all other contributions to the free energy and is difficult to write down except in a few cases [26,77]. We will content ourselves with a mean-field approximation, which becomes exact when each spin interacts infinitely weakly with an infinite number of other spins.…”
Section: Placing the Glass Transition On The Map Thermodynamics-wise:...mentioning
confidence: 99%
“…One can now use Eqs. ( 73), (77), and (54) to determine the Helmholtz free energy F of the solid as a function of the density-which is specified automatically given a lattice-and the effective spring constant α. This free energy is further optimised with respect to α thus giving an approximation for the free energy of the solid as a function of the density, thus allowing one to compute the pressure.…”
Section: B Emergence Of the Molecular Fieldmentioning
confidence: 99%