weakly$91350$ - definitie. Wat is weakly$91350$
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Wat (wie) is weakly$91350$ - definitie

WEAK DERIVATION
Weakly Differentiable; Weakly differentiable

Weak NP-completeness         
SET OF COMPUTATIONAL PROBLEMS FOR WHICH THERE IS AN ALGORITHM SOLVING THEM IN POLYNOMIAL TIME IN THE DIMENSION OF THE PROBLEM AND THE MAGNITUDES OF THE DATA INVOLVED (IF GIVEN AS INTEGERS), RATHER THAN THE BASE-TWO LOGARITHMS OF THEIR MAGNITUDES
Weakly NP-complete; Weakly NP-hard
In computational complexity, an NP-complete (or NP-hard) problem is weakly NP-complete (or weakly NP-hard) if there is an algorithm for the problem whose running time is polynomial in the dimension of the problem and the magnitudes of the data involved (provided these are given as integers), rather than the base-two logarithms of their magnitudes. Such algorithms are technically exponential functions of their input size and are therefore not considered polynomial.
Non-coordinating anion         
  • pmid=18049748}}</ref> illustrating its high symmetry. Color code: green = F, red = O.
  •  year = 2000 }}</ref> which is closely related to [[Brookhart's Acid]]
  • center
ANION WHICH INTERACTS ONLY WEAKLY WITH CATIONS
Non-coordinating anions; Noncoordinating; Noncoordinating anion; Weakly coordinating anion; Poorly-coordinating anion; Poorly coordinating anion; Weakly-coordinating anion; Non-coordinating ion; Weakly coordinating anions
Anions that interact weakly with cations are termed non-coordinating anions, although a more accurate term is weakly coordinating anion. Non-coordinating anions are useful in studying the reactivity of electrophilic cations.
Weakly o-minimal structure         
Weakly o-minimal strcuture
In model theory, a weakly o-minimal structure is a model theoretic structure whose definable sets in the domain are just finite unions of convex sets.

Wikipedia

Weak derivative

In mathematics, a weak derivative is a generalization of the concept of the derivative of a function (strong derivative) for functions not assumed differentiable, but only integrable, i.e., to lie in the Lp space L 1 ( [ a , b ] ) {\displaystyle L^{1}([a,b])} .

The method of integration by parts holds that for differentiable functions u {\displaystyle u} and φ {\displaystyle \varphi } we have

a b u ( x ) φ ( x ) d x = [ u ( x ) φ ( x ) ] a b a b u ( x ) φ ( x ) d x . {\displaystyle {\begin{aligned}\int _{a}^{b}u(x)\varphi '(x)\,dx&={\Big [}u(x)\varphi (x){\Big ]}_{a}^{b}-\int _{a}^{b}u'(x)\varphi (x)\,dx.\\[6pt]\end{aligned}}}

A function u' being the weak derivative of u is essentially defined by the requirement that this equation must hold for all infinitely differentiable functions φ vanishing at the boundary points ( φ ( a ) = φ ( b ) = 0 {\displaystyle \varphi (a)=\varphi (b)=0} ).