Exact(4)
Having established the potential energy difference of the beam during debonding (ΔΕ pot ), it requires to determine the term of left hand side of Eq. (5), ΔD, which states the total energy dissipation of the beam during debonding failure.
In their definition, dirty values are infrequent right hand side (RHS) values within the set of left hand side (LHS) matched tuples, which makes them also follow the "majority policy".
Integrating the above inequalities over ( 0, T ) and noticing (3.13), we see that the terms of left hand side in these inequalities can all be estimated by ε ∬ Q T ( D 6 u σ ) 2 d x d t and a constant number C. Then by the boundary value condition and (3.10), we have ∬ Q T ( D 4 u σ ) 2 d x d t ≤ ε ∬ Q T ( D 6 u σ ) 2 d x d t + C, (3.14).
Follow-up assessments of left hand side treatment occurred a further 5 weeks later.
Similar(56)
The terms on left hand side of Eqs.
As an extension of research, we have investigated modification of left-hand side (LHS) of biphenyl analogues containing an acylsulfonamide moiety in the development of potent and selective human β3-adrenergic receptor (AR) agonists.
While uncertainty in the right-hand side (RHS) and in the objective function's coefficients (OFC) have been thoroughly studied in the literature, the case of left-hand side (LHS) uncertainty has attracted significantly less attention mainly because of the computational implications that arise in such a problem.
The denominator of left-hand side is nonzero by using in Theorem 3.2.
The solution of left-hand side integral depend on the explicit expression of the function f and are denoted as g.
In order to get the estimate for the third term of left-hand side in (3.2), we denote F n ( u ) = ∫ 0 u ( s s β - 2 f n ( s ) ) 1 / q d s, u ∈ ℝ 1.
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