weakly$91350$ - traducción al griego
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weakly$91350$ - traducción al griego

WEAK DERIVATION
Weakly Differentiable; Weakly differentiable

weakly      
adv. ασθενώς
optical fibre         
  • Cross-section of a fiber drawn from a D-shaped '''preform'''
  • Colladon's "light fountain"
  • Diffuse reflection
  • An overview of the operating principles of the optical fiber
  • A [[TOSLINK]] fiber optic audio cable with red light shone in one end
  • A [[frisbee]] illuminated by fiber optics
  • acrylic]] rod, illustrating the total internal reflection of light in a multi-mode optical fiber.
  • An optical fiber lamp
  • Illustration of the modified chemical vapor deposition (inside) process
  • Light reflected from optical fiber illuminates exhibited model
  • multi-mode fibers]].
  • The propagation of light through a [[multi-mode optical fiber]].
  • An aerial optical fiber splice enclosure lowered during installation. The individual fibers are fused and stored within the enclosure for protection from damage
  • An [[optical fiber cable]]
  • Optical fiber types
  • The P<sub>4</sub>O<sub>10</sub> cagelike structure—the basic building block for phosphate glass
  • Specular reflection
  • ST connectors]] on [[multi-mode fiber]]
  • Theoretical loss spectra (attenuation, dB/km) for Silica optical fiber (dashed blue line) and typical ZBLAN optical fiber (solid gray line) as a function of wavelength (microns).
  • Experimental attenuation curve of low loss multimode silica and ZBLAN fiber. Black triangle points and gray arrows illustrate a four order of magnitude reduction in the attenuation of silica optical fibers over four decades from ~1000&nbsp;dB/km in 1965 to ~0.17&nbsp;dB/km in 2005.
  • The structure of a typical [[single-mode fiber]].<br />
1. Core: 8&nbsp;µm diameter<br />
2. Cladding: 125&nbsp;µm dia.<br />
3. Buffer: 250&nbsp;µm dia.<br />
4. Jacket: 400&nbsp;µm dia.
LIGHT-CONDUCTING FIBER
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Definición

Increasing
·p.pr. & ·vb.n. of Increase.

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} ).