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Dirac’s delta function

More exactly to an infinitesimally narrow Gaussian curve of infinite height, having unit area, namely Dirac s delta functional 5(V — V0), where V0 is related to the molecular weight of the injected sample, according to the calibration curve of the column used... [Pg.43]

If spreading phenomena can be neglected, because the MWD is broad enough with respect to the resolution power of the column, Dirac s delta functional can be taken for the kernel of the integral operator (47 b) in Eq. (47 a), giving... [Pg.52]

Note that the current has a paradoxical behavior at times close to zero. When k°ti 3> 1 and /[ —> 0, the current takes the form of a Dirac s delta function, which in practice means that although it could take a very large value, it will be not possible to record it. [Pg.420]

Here, the angular brackets denote an ensemble average, which is the same as time average from the ergodic hypothesis. 8ap and 8,- are Kronecker delta, and 8(f — t ) is Dirac s delta function. [Pg.54]

Here, (> and /> are initial and final states of the supermolecular complex, 11 is the induced incremental polarizability (a second-rank tensor), fio and fij are unit vectors in the direction of the electric polarization of incident and scattered waves, which are often specified in the form of subscripts V and H, for vertical and horizontal, (aif = (Ej- — Ei)lh is the energy difference of initial and final state in units of angular frequency, Pi T) is the population of the initial state (a function of temperature), <5 (to) is Dirac s delta function, and the summation is over all initial and final states of the collisional complex. [Pg.441]

In case of only one relaxation time x (i.e. ideal relaxation, with Dirac s delta-function 5(x) as g(x)) the real and imaginary part of complex e(co) = ( ) + > becomes ... [Pg.551]

The delta function (or Dirac s delta function) is a generalized function that is obtained as a limit when a normalized function f dxf x = 1 becomes zero everywhere except at one point. For example. [Pg.11]

The Fourier transform of an infinite short pulse function h(t) = Kb(t), where 5(f) is Dirac s delta function, equals//(jco) = K, that is, it contains all the frequencies with the same amplitude K. Such a function caimot be realized in practice and must be substituted by a pulse of a short duration At. However, such a function does not have uniform response in the Fourier (i.e., frequency) space. The Fourier transform of such a function, defined as h(t) = 1 for r = 0 to To and h(t) = 0 elsewhere, equals... [Pg.163]

Equation (5), can be also written as a Coulomb interaction between a point charge, located at the position R, represented by a Dirac s delta function and an eDF, yo(r), using the integral ... [Pg.7]

With the collocation method, Dirac s delta function is used as the weight function in the support point x ... [Pg.240]


See other pages where Dirac’s delta function is mentioned: [Pg.10]    [Pg.42]    [Pg.341]    [Pg.307]    [Pg.367]    [Pg.227]    [Pg.123]    [Pg.45]    [Pg.88]    [Pg.79]    [Pg.226]    [Pg.44]    [Pg.1356]    [Pg.332]    [Pg.335]    [Pg.49]    [Pg.165]    [Pg.223]    [Pg.1837]    [Pg.240]    [Pg.436]    [Pg.248]    [Pg.368]    [Pg.219]    [Pg.223]    [Pg.1829]    [Pg.88]    [Pg.186]    [Pg.192]    [Pg.203]    [Pg.1538]    [Pg.249]    [Pg.102]    [Pg.519]    [Pg.216]    [Pg.225]    [Pg.146]    [Pg.271]   
See also in sourсe #XX -- [ Pg.368 ]

See also in sourсe #XX -- [ Pg.222 ]




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