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On the other hand, [[Z.sub.[sigma]] | [sigma] [member of] [GAMMA]} is total in [S.sub.q](M), and condition (1) equivalent to <<[T.sub.n]([Z.sub.[sigma]]), [Z.sub.[tau]])) converges in C for any [sigma], [tau] [member of] [GAMMA], so there exists a linear
operator form [S.sub.q](M) to [S.sup.*.sub.q] (M) such that, for any [xi], [eta] [member of] [S.sub.q](M), we have
We proceed from this block diagram to the vector equations of state in the
operator form:
Considering
operator form of coordinate and momentum
The equation (2.3) can be written in an
operator form as follows
As it is known, the closed subsets of any closure
operator form a complete lattice with respect to the inherited partial order from the underlying complete lattice structure (in this case P(B)).
We now rewrite (4) in the local fractional
operator form as follows:
It follows from this model that LF ripples for open-loop boost converter in
operator form are
In an
operator form, equation (1) can be written as
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operator form Merthyr Tydfil.
To solve problems of the form (1), we write it in an
operator form as
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