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Poynting’s theorem

Poynting s theorem for the energy flow of plane waves in vacuo thus applies to the EM and EMS modes, but not to the S mode. Vector multiplication of Eqs. (52) and (53) by k, and combination with Eq. (49) and the result E C = 0, is easily shown [16,20] to result in a Poynting vector that is parallel with the group velocity C of Eq. (56). Later in Section VII.C.3 we shall return to Poynting s theorem in the case of axisymmetric photon wavepackets. [Pg.23]

Figure 8-1 Derivation of Poynting s theorem and the energy inequality. Figure 8-1 Derivation of Poynting s theorem and the energy inequality.
Expression (8.92) represents a differential form of Poynting s theorem. [Pg.217]

An important property of the energy flow Ft out of domain V), containing sources j , is that its integral over a time period, Ftdt, is always non-negative independently of the type of the extraneous sources. To prove this we introduce a domain Oft Pi formed by the ball without domain (Figure 8-1). We can apply now Poynting s theorem (8.95) to the volume Oh Vi, taking into account that extraneous currents j = 0 in Or Vi ... [Pg.218]

We can obtain Poynting s theorem by taking the scalar product of the second equation for the total field (8.103) with H and the complex conjugate of the first equation (8.102) with E, and subtracting one from the other ... [Pg.220]

This is Poynting s theorem in the frequency domain (Stratton, 1941). It says that the energy flow outside the domain V] is formed by the balance between the energy dissipated in heat per unit volume per second, and the energy introduced through tlie extraneous currents j. ... [Pg.221]

Following the technique outlined above for the time domain case, we apply Poynting s theorem to the volume 0 V], taking into account that extraneous currents j = 0 in Or Vi ... [Pg.221]

We now can write Poynting s theorem (8.108) for the field E, H given within domain V ... [Pg.222]

By means of Poynting s " theorem, it can be shown that gi gi = g- Equation (15.7) holds for a dissymmetric isotropic medium. With Maxwell s equations (15.4), Eq. (15.7), neglecting the rotational term, become... [Pg.420]

Using Poynting s theorem, finally, after some mathematics, the extinction cross section Cext for the dipole is obtained as... [Pg.189]

According to the energy conservation law Poynting s theorem, the work done by the electric field is... [Pg.287]

According to Poynting s theorem, the extinction spectra, Pexi (o), the scattering spectra, Pscaipi) and the absorption spectra, Pabs oi), are given respectively by ... [Pg.132]


See other pages where Poynting’s theorem is mentioned: [Pg.215]    [Pg.216]    [Pg.216]    [Pg.216]    [Pg.217]    [Pg.218]    [Pg.220]    [Pg.233]    [Pg.56]    [Pg.313]    [Pg.310]    [Pg.38]    [Pg.4]   
See also in sourсe #XX -- [ Pg.216 ]

See also in sourсe #XX -- [ Pg.4 ]




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