We introduce the following transform f(t) = j&J) K(w, t) P(o) dw with the Fourier-type inverse J'(o) = s p(t) K(w, t)fW dt. Unless otherwise indicated, the limits of integration are not finite and will be specified for the particular integral transform. The time-varying system function H(w, t) is d
The correct application of Poynting’s theorem to the time-dependent magnetosphere: reply to Heikkila
✍ Scribed by M. Lockwood; C. J. Davis
- Publisher
- Copernicus Group
- Year
- 1999
- Tongue
- English
- Weight
- 187 KB
- Volume
- 17
- Category
- Article
- ISSN
- 0992-7689
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