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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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