mechanical quadrature - определение. Что такое mechanical quadrature
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Что (кто) такое mechanical quadrature - определение

NUMERICAL INTEGRATION
Gaussian integration; Gaussian numerical integration; Gauss quadrature; Gauss legendre quadrature; Gaussian Quadrature; Gauss–Lobatto quadrature; Gauss-Lobatto quadrature
  • 2}} – 3''x'' + 3}}), the 2-point Gaussian quadrature rule even returns an exact result.
  • ''n'' {{=}} 5)}}

Gauss–Jacobi quadrature         
Gauss-Jacobi Mechanical Quadrature; Gauss–Jacobi mechanical quadrature; Gauss-Jacobi quadrature; Gauss-Jacobi mechanical quadrature; Gauss–Gegenbauer quadrature; Gauss-Gegenbauer quadrature
In numerical analysis, Gauss–Jacobi quadrature (named after Carl Friedrich Gauss and Carl Gustav Jacob Jacobi) is a method of numerical quadrature based on Gaussian quadrature. Gauss–Jacobi quadrature can be used to approximate integrals of the form
Mechanical counter         
  • Early IBM tabulating machine using mechanical counters
  • Mechanical counter wheels showing both sides. The bump on the wheel shown at the top engages the ratchet on the wheel below every turn.
DIGITAL COUNTERS BUILT USING MECHANICAL COMPONENTS
Counter (mechanical); Mechanical counters; Veeder-Root Counter; Veeder-Root counter
Mechanical counters are digital counters built using mechanical components. Long before electronics became common, mechanical devices were used to count events.
Mechanical television         
  • A color televisor. A test card (the famous [[test card F]]) can just be seen through the lens on the right.
  • thumb
  • Ernst Ruhmer demonstrating his experimental television system, which was capable of transmitting 5×5 [[pixel]] images of simple shapes over telephone lines, using a 25-element selenium cell receiver (1909)<ref>[https://babel.hathitrust.org/cgi/pt?id=mdp.39015031441952;view=1up;seq=489 "Another Electric Distance-Seer"], ''Literary Digest'', September 11, 1909, page 384.</ref>
  • Flying spot scanner in a television studio in 1931. This type was used for "head shots" of performers speaking, singing or playing instruments. A bright spot of light projected from the lens at center scanned the subject's face, and the light reflected at each point was picked up by the 8 [[phototube]]s in the dish-shaped mirrors.
  • 315x315px
  • Jenkins Television Co. rotating disk television camera, 1931
  • Television Machine with 4 LED Strips
  • The [[Nipkow disk]]. This schematic shows the circular paths traced by the holes, that may also be square for greater precision. The area of the disk outlined in black shows the region scanned.
A TELEVISION SYSTEM THAT RELIES ON A MECHANICAL SCANNING DEVICE, TO BOTH SCAN AND REPRODUCE THE VIDEO SIGNAL.
Mechanical Television; Electromechanical television; Mechanical TV; Televisor; Baird Televisor; Televisors; Televisory; Mechanical televisions; Baird system; Mechanical scan television
Mechanical television or mechanical scan television is a television system that relies on a mechanical scanning device, such as a rotating disk with holes in it or a rotating mirror drum, to scan the scene and generate the video signal, and a similar mechanical device at the receiver to display the picture. This contrasts with vacuum tube electronic television technology, using electron beam scanning methods, for example in cathode ray tube (CRT) televisions.

Википедия

Gaussian quadrature

In numerical analysis, a quadrature rule is an approximation of the definite integral of a function, usually stated as a weighted sum of function values at specified points within the domain of integration. (See numerical integration for more on quadrature rules.) An n-point Gaussian quadrature rule, named after Carl Friedrich Gauss, is a quadrature rule constructed to yield an exact result for polynomials of degree 2n − 1 or less by a suitable choice of the nodes xi and weights wi for i = 1, …, n. The modern formulation using orthogonal polynomials was developed by Carl Gustav Jacobi in 1826. The most common domain of integration for such a rule is taken as [−1, 1], so the rule is stated as

1 1 f ( x ) d x i = 1 n w i f ( x i ) , {\displaystyle \int _{-1}^{1}f(x)\,dx\approx \sum _{i=1}^{n}w_{i}f(x_{i}),}

which is exact for polynomials of degree 2n − 1 or less. This exact rule is known as the Gauss-Legendre quadrature rule. The quadrature rule will only be an accurate approximation to the integral above if f (x) is well-approximated by a polynomial of degree 2n − 1 or less on [−1, 1].

The Gauss-Legendre quadrature rule is not typically used for integrable functions with endpoint singularities. Instead, if the integrand can be written as

f ( x ) = ( 1 x ) α ( 1 + x ) β g ( x ) , α , β > 1 , {\displaystyle f(x)=\left(1-x\right)^{\alpha }\left(1+x\right)^{\beta }g(x),\quad \alpha ,\beta >-1,}

where g(x) is well-approximated by a low-degree polynomial, then alternative nodes xi' and weights wi' will usually give more accurate quadrature rules. These are known as Gauss-Jacobi quadrature rules, i.e.,

1 1 f ( x ) d x = 1 1 ( 1 x ) α ( 1 + x ) β g ( x ) d x i = 1 n w i g ( x i ) . {\displaystyle \int _{-1}^{1}f(x)\,dx=\int _{-1}^{1}\left(1-x\right)^{\alpha }\left(1+x\right)^{\beta }g(x)\,dx\approx \sum _{i=1}^{n}w_{i}'g\left(x_{i}'\right).}

Common weights include 1 1 x 2 {\textstyle {\frac {1}{\sqrt {1-x^{2}}}}} (Chebyshev–Gauss) and 1 x 2 {\displaystyle {\sqrt {1-x^{2}}}} . One may also want to integrate over semi-infinite (Gauss-Laguerre quadrature) and infinite intervals (Gauss–Hermite quadrature).

It can be shown (see Press, et al., or Stoer and Bulirsch) that the quadrature nodes xi are the roots of a polynomial belonging to a class of orthogonal polynomials (the class orthogonal with respect to a weighted inner-product). This is a key observation for computing Gauss quadrature nodes and weights.