Symbolic notation of clathrates

2018 ◽  
Vol 30 (5-6) ◽  
pp. 510-513
Author(s):  
Janusz Lipkowski ◽  
Jerry L. Atwood
Keyword(s):  
1955 ◽  
Vol 22 (2) ◽  
pp. 215-221
Author(s):  
J. Denavit ◽  
R. S. Hartenberg

Abstract A symbolic notation devised by Reuleaux to describe mechanisms did not recognize the necessary number of variables needed for complete description. A reconsideration of the problem leads to a symbolic notation which permits the complete description of the kinematic properties of all lower-pair mechanisms by means of equations. The symbolic notation also yields a method for studying lower-pair mechanisms by means of matrix algebra; two examples of application to space mechanisms are given.


1937 ◽  
Vol 2 (3) ◽  
pp. 97-112 ◽  
Author(s):  
Carl G. Hempel

1. The problem. The aim of the following considerations is to introduce a new type of non-Aristotelian logic by generalizing the truth-table methods so far employed for establishing non-Aristotelian sentential calculi. We shall expound the intended generalization by applying it to the particular set of pluri-valued systems introduced by J. Łukasiewicz. One will remark that the points of view illustrated by this example may serve to generalize quite analogously any other plurivalued systems, such as those originated by E. L. Post, by H. Reichenbach, and by others.2. J. Łukasiewicz's plurivalued systems of sentential logic. First of all, we consider briefly the structure of the Łukasiewicz systems themselves.As to the symbolic notation in which to represent those systems, we make the following agreements: For representing the expressions of the (two- or plurivalued) calculus of sentences, we make use of the Principia mathematica symbolism; however, we employ brackets instead of dots. We call the small italic letters “p”, “q”, “r”, … sentential variables or elementary sentences, and employ the term “sentence” as a general designation of both elementary sentences and the composites made up of elementary sentences and connective symbols (“~”, “ν” “.”, “⊃” “≡”).Now, the different possible sentences (or, properly speaking, the different possible shapes of sentences, such as “p”, “p∨q”, “~p.(q∨ r)”, etc.) are the objects to which truth-values are ascribed; and just as in every other case one wants a designation for an object in order to be able to speak of it, we want now a system of designations for the sentences with which we are going to deal in our truth-table considerations.


1971 ◽  
Vol 93 (1) ◽  
pp. 102-112 ◽  
Author(s):  
P. N. Sheth ◽  
J. J. Uicker

Revisions of the Denavit-Hartenberg symbolic notation are proposed which extend its use to the entire domain of rigid link mechanisms. The extended notation provides a clear separation of the pair variables and the invariant parameters of a mechanism and thus provides a framework in which higher pairs can be systematically modeled. The new symbolism can be used directly with the existing matrix methods of kinematic analysis, and a numerical scheme is presented to reduce the task of data collection for these methods.


2000 ◽  
Vol 10 (04) ◽  
pp. 949-1015 ◽  
Author(s):  
ALI R. BAGHAI-WADJI

In this chapter it is shown that three dimensional governing- and constitutive equations in transversally inhomogeous piezoelectric media can be diagonalized. A symbolic notation has been introduced which allows to perform the diagonalization simply by inspection. Diagonalized differential equations transform into eigenvalue forms in Fourier domain. Solving for the corresponding eigenpairs, the construction of various Green's functions has been demonstrated by several examples. In addition novel ideas for the calculation of self-actions in the boundary element method have been discussed. The work consists of four sections. Following a brief introduction in the first section, the diagonalization procedure is described in the second section. The presented methodology is a refinement of the author's ideas which were presented in various short courses. The third section on Green's function theory and the calculation of self-actions in the boundary element builds upon the author's lecture notes. The fourth section briefly summarizes our discussion and suggests directions for possible future research.


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