coordinate systems
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11—20 of 22 matching pages
11: 30.14 Wave Equation in Oblate Spheroidal Coordinates
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§30.14(i) Oblate Spheroidal Coordinates
…12: 14.19 Toroidal (or Ring) Functions
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►This form of the differential equation arises when Laplace’s equation is transformed into toroidal coordinates
, which are related to Cartesian coordinates
by
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13: 23.20 Mathematical Applications
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23.20.2
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14: 30.13 Wave Equation in Prolate Spheroidal Coordinates
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§30.13(i) Prolate Spheroidal Coordinates
…15: Bibliography P
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Comoving coordinate system for relativistic hydrodynamics.
Phy. Rev. C 75, pp. (024907–1)–(024907–10).
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16: 18.39 Applications in the Physical Sciences
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►By (1.5.17) the first term in (18.39.21), which is the quantum kinetic energy operator , can be written in spherical coordinates
as
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17: Bibliography M
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Field Theory Handbook. Including Coordinate Systems, Differential Equations and Their Solutions.
2nd edition, Springer-Verlag, Berlin.
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18: 32.6 Hamiltonian Structure
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– can be written as a Hamiltonian system
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19: Guide to Searching the DLMF
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Table 2: Wildcard Examples
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►If a query does not return any hits, the DLMF search system relaxes the query to match and retrieve what may be intended by the original query.
…Therefore, if your query is
Query | What it stands for |
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co$te |
Coordinate, conjugate, correlate,… |
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Ai^2+Bi^2
, the system modifies the query so it will find the equations containing the latter expressions.
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►To recognize the math symbols and structures, and to accommodate equivalence between various notations and various forms of expression, the search system maps the math part of your queries into a different form.
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►The syntax of the special functions can be LaTeX-like or as employed in widely used computer algebra systems.
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20: 28.33 Physical Applications
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►Physical problems involving Mathieu functions include vibrational problems in elliptical coordinates; see (28.32.1).
…In elliptical coordinates (28.32.2) becomes (28.32.3).
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►If the parameters of a physical system vary periodically with time, then the question of stability arises, for example, a mathematical pendulum whose length varies as .
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Daymond (1955) for vibrating systems.
McLachlan (1947, Chapter XV) for amplitude distortion in moving-coil loud-speakers, frequency modulation, dynamical systems, and vibration of stretched strings.