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Area theorem

A mapping is said to be symplectic or canonical if it preserves the differential form dp A dq which defines the symplectic structure in the phase space. Differential forms provide a geometric interpretation of symplectic-ness in terms of conservation of areas which follows from Liouville s theorem [14]. In one-degree-of-freedom example symplecticness is the preservation of oriented area. An example is the harmonic oscillator where the t-flow is just a rigid rotation and the area is preserved. The area-preserving character of the solution operator holds only for Hamiltonian systems. In more then one-degree-of-freedom examples the preservation of area is symplecticness rather than preservation of volume [5]. [Pg.335]

Theorems of Pappus (for volumes and areas of surfaces of revolution)... [Pg.430]

These theorems are useful for determining volumes V and surface areas S of solids of revolution if the centers of gravity are known. If S and V are known, the centers of gravity may be determined. [Pg.430]

Flachen-satz, m. theorem of conservation of areas, -wert, m. surface value, -winkel, m. plane angle, -zahl,/. number of faces square number. [Pg.156]

If a well proves productive, the ensuing completion operation may require an area in excess of the drilling area. This may mean allocations for frac tank placement, blenders, pump trucks, bulk trucks and nitrogen trucks. In today s economic climate, the operator should weigh the probability of success, Bayes theorem (Equation 4-373), with the cost of constructing and reclaiming an additional area needed for stimulation (Equation 4-374). Plans such as these... [Pg.1350]

The two specific areas of research in which Polya s Theorem has been most extensively applied are graphical and chemical enumeration, a fact which Polya clearly foresaw in his choice of title. Applications in other fields are far from rare, however, and it is fitting to give a brief account of a few such uses of the theorem. [Pg.134]

Thus, the first chapter touches on an aspect of electrochemistry for which the author has become justly well known application of the Wagner and Traud theorem of 1938 according to which electrochemical systems may function on a single electrode. In the next chapter, the article by Koczorowski treats a seldom-visited but truly fundamental area, that of voltaic measurements at liquid interfaces. [Pg.289]

As time increases from —oo to 0, the half width of the wave packet y(x, t) continuously decreases and the maximum amplitude continuously increases. At t = 0 the half width attains its lowest value of flja and the maximum amplitude attains its highest value of 1 /a/2, and both values are in agreement with the wave packet in equation (1.20). As time increases from 0 to oo, the half width continuously increases and the maximum amplitude continuously decreases. Thus, as f- increases, the wave packet y(x, t) remains gaussian in shape, but broadens and flattens out in such a way that the area under the square y(x, t) of the wave packet remains constant over time at a value of (2-y/ a), in agreement with ParsevaTs theorem (1.18). [Pg.18]

Perhaps of greater interest to us are results derived by the same authors71 that relate surface and bulk electronic properties of jellium. Considering two jellium slabs, one extending from —L to -D and the other from D to L, they calculated the force per unit area exerted by one on the other. According to the Hellmann-Feynman theorem, this is just the sum of the electric fields acting... [Pg.51]

This section provides a short introductory survey of an area of science which is not only mathematically exacting, but also of fundamental importance for certain aspects of biogenesis. Thermodynamics, a sub-discipline of physics, deals not only with heat and dynamics , but formulated more generally, thermodynamics is concerned with energy and entropy and deals with theorems which are valid across almost all areas of physics. [Pg.237]

The elements A and B therefore have equal areas. Liouville s theorem states that an element in phase space is conserved, which means that the element within which a system can be found is constant. Further, if the range Ae in the phase space is divided into equal elements, the system spends equal times passing through these elements, or cells. [Pg.435]


See other pages where Area theorem is mentioned: [Pg.71]    [Pg.167]    [Pg.173]    [Pg.175]    [Pg.167]    [Pg.173]    [Pg.175]    [Pg.160]    [Pg.59]    [Pg.59]    [Pg.71]    [Pg.167]    [Pg.173]    [Pg.175]    [Pg.167]    [Pg.173]    [Pg.175]    [Pg.160]    [Pg.59]    [Pg.59]    [Pg.2381]    [Pg.14]    [Pg.14]    [Pg.336]    [Pg.145]    [Pg.889]    [Pg.15]    [Pg.172]    [Pg.733]    [Pg.18]    [Pg.192]    [Pg.64]    [Pg.195]    [Pg.229]    [Pg.399]    [Pg.643]    [Pg.221]    [Pg.222]    [Pg.223]    [Pg.225]    [Pg.225]    [Pg.226]    [Pg.118]    [Pg.118]    [Pg.442]    [Pg.15]   
See also in sourсe #XX -- [ Pg.59 ]




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Theorem, equal-areas

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