compendium |
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effective powerAssume the terminal variables on a passive dipole (terminal voltage u(t) and terminal current i(t) ) are nonsinusoidal periodic time-fuctions: |
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(38) |
Again these spectral displays can be represented as the sum of cosine- and sine- elements (applieance of the addition theorem ): | |
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(39) |
For the active power exchange inside the dipole we obtain from: | |
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(40) |
together with the property of orthogonality of the trigonometric function inside the interval of [t0, t0+T] | |
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(41) |
The constant components and the overtones themselves supply the known parts of the total active power exchange in the dipole. |
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