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slowly varying envelope approximation : ウィキペディア英語版
slowly varying envelope approximation
In physics, the slowly varying envelope approximation (SVEA, sometimes also called slowly varying amplitude approximation or SVAA) is the assumption that the envelope of a forward-travelling wave pulse varies slowly in time and space compared to a period or wavelength. This requires the spectrum of the signal to be narrow-banded—hence it also referred to as the narrow-band approximation.
The slowly varying envelope approximation is often used because the resulting equations are in many cases easier to solve than the original equations, reducing the order of—all or some of—the highest-order partial derivatives. But the validity of the assumptions which are made need to be justified.
==Example==

For example, consider the electromagnetic wave equation:
:\nabla^2 E - \mu_0\, \varepsilon_0\, \frac = 0.
If k0 and ''ω''0 are the wave number and angular frequency of the (characteristic) carrier wave for the signal ''E''(r,''t''), the following representation is useful:
:E(\mathbf,t) = \Re\left\_0\, \cdot\, \mathbf - \omega_0\, t )} \right\},
where \scriptstyle \Re\ denotes the real part of the quantity between brackets.
In the ''slowly varying envelope approximation'' (SVEA) it is assumed that the complex amplitude ''E''0(r, ''t'') only varies slowly with r and ''t''. This inherently implies that ''E''0(r, ''t'') represents waves propagating forward, predominantly in the k0 direction. As a result of the slow variation of ''E''0(r, ''t''), when taking derivatives, the highest-order derivatives may be neglected:〔

:\displaystyle \left| \nabla^2 E_0 \right| \ll \left| \vec k_0\cdot \nabla E_0 \right| and \displaystyle \left| \frac \right| \ll \left| \omega_0\, \frac \right|, with k_0 = |\mathbf_0|.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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