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A straightforward computation of energy velocity is proposed.
The proof of the next proposition is a straightforward computation of matrix products.
Straightforward computation of multi-body functions is very expensive therefore it imposes great challenges to query processing.
While computation of the CW amplitude is straightforward, computation of the CW phase is not such an unambiguous procedure.
Straightforward computation of the probability mass function (p.m.f). of Y t) using (4) is based on an enumerative approach.
The BMI-based condition is converted into the linear matrix inequality (LMI -based condition by utiLMI -basednge of variables for straightforward conditionon of the obyerver gain matrix.
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Simple and closed form empirical formulas have been derived to allow straightforward computations of the modal resonant frequencies.
for any n 1, n 2, n 3, n 4 ∈ N, so we can show that the sequence ( φ n 1, n 2, n 3, n 4 ) fulfills (3.6) by a straightforward computation because of the continuity of the function R + → R, t → R t φ ( x ), for any φ ∈ C b, 1 ( H ).
The following lemma can be proved by means of a straightforward computation.
Moreover, a straightforward computation shows that the following points of (mathbb{R}^{2}_) hold the required conditions: x=biggl c-frac{b}{2},frac{b}{2}biggr),qquad y=biggl( frac{b}{2},d-frac{b}{2}biggr), qquad z=biggl(frac{b}{2}, frac{b}{2}biggr).
A straightforward computation shows that K and W satisfy the assumptions of Theorem 1.1.
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