Hidden fields
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" E are the complete elliptic integrals of the first and second kind respectively... "
Physical Review - Página 469
1912
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Boundary Integral and Singularity Methods for Linearized Viscous Flow

C. Pozrikidis - 1992 - 276 páginas
...-3.A2/-.2 i -2\ i /-2 -2\2T + Jx (<TO + a ) + (a0 - a ) J — f 'f2 where f2 — x2 + (a — <r0)2, and F and E are the complete elliptic integrals of the first and second kind with argument k, defined as f"/2 d<a f"/2 fW= ; ; — m BW- (1-fc2cos2w)1/2da> (2.4.10)...
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Rethinking Neural Networks: Quantum Fields and Biological Data

John Carew Eccles - 1993 - 566 páginas
...In the next step we perform the singularities absorbing substitution Hence, = r_ sin 2 0. where A', E are the complete elliptic integrals of the first and second kind, respectively, T/2 T/2 ^j\ - ri sin 2 0 - 2 _) = / Jl-risi r* • sn The elliptic integrals for the parameter value...
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Wavelets and Their Applications

J.S. Byrnes, Kathryn A. Hargreaves, Karl Berry - 1994 - 432 páginas
...perform the singularities-absorbing substitution £, = r-sin28. (4.17) ( Schempp, Segman Hence, where K, E are the complete elliptic integrals of the first and second kind, respectively, K(ri) = J72 I . d8, n/2 Y~r-sm e (4.19) The elliptic integrals for the parameter value r2. can be evaluated...
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Water Wave Propagation Over Uneven Bottoms: Linear wave propagation, Parte1

Maarten W. Dingemans - 2000 - 508 páginas
...J(l-msm2vfdv = - (2 - TO) E(m)-- (1 - m)K(m) , (3.159) o where m is the elliptic parameter and K(m) and E(m) are the complete elliptic integrals of the first and second kind respectively (see also note 6.2). Then we have (3.160) and we obtain Sir h cosh2 kh with m = P + q (3.161b) as is...
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Heavy Elements and Related New Phenomena, Volumen1

Walter Greiner, Raj K. Gupta - 1999 - 528 páginas
...= y(x) or yi — y(x')). The integrand reads F(lt x, = (yyi ^ + a - (x — f + (x — ,) M K and K' are the complete elliptic integrals of the first and second kind, respectively: 7r/2 7r/2 K(k) = f (1 - k2sin2t)-l/2dt ; K'(k) = f (1 - k2sm2t)l/2dt (32) and a2 = (y+y^ + ^-z')2,...
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Plasma Physics: Proceedings of the 1997 Latin American Workshop (VII LAWPP ...

Pablo Martín, Julio Puerta - 1999 - 1080 páginas
...[6(2 — rn)G 6 — 5(1 — m)G 4 ]/7; G 10 = [8(2 — m)G 8 — 7(1 — rn)G 6 ]/9 and K(rn), E(rn) are the complete elliptic integrals of the first and second kind, respectively. In order to find the extremum values of 8 W the Euler—Lagrange method can be used and the following...
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Materials Instabilities: Proceedings of the First Latin American Summer School

Daniel Walgraef - 2000 - 356 páginas
...His explicit out-of-plane normal stress in the loop plane (ie, z = 0) az reads: <o<s<D. (99) where K and E are the complete elliptic integrals of the first and second kind, respectively, x is the distance from loop center, and R the loop radius. In order to evaluate the accuracy of the...
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Geosynthetics and Geosystems in Hydraulic and Coastal Engineering

Krystian Pilarczyk - 2000 - 944 páginas
...tension t can be computed from the solution k of the equation 2[K(k)-E(k)]Pbot=l (12) where K(k) and E(k) are the complete elliptic integrals of the first and second kind, respectively. In this formulation, for a solution to exist, it is required that 0 < k2 < 1, so that / must be less...
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Proceedings of the 7th International Conference on Clustering Aspects of ...

M. Korolija, Z. Basrak, R. Caplar - 2000 - 476 páginas
...(surface equation y — y(x) or j/i = y(x')). In the integrand F(x,x') = {yyi[(K-2D)/3]2 dx K and K' are the complete elliptic integrals of the first and second kind, respectively: /•T/2 K(k) = / (1 - k2sm2t)~1/2dt (11) Jo /•ff/2 K'(k) = (I- fcWi)1/2^ (12) Jo and a2 = (y + y,)2...
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Boundary Element Analysis: Theory and Programming

Mohammed Ameen - 2001 - 288 páginas
...y-\ (2.60) and «,/ = H0." = UQ,' = u:g = 0. In the above, 2Rr 2 i+r The quantities K(m) and £(w) are the complete elliptic integrals of the first and second kind respectively. Also, m is called the parameter of the elliptic integral and k is the modulus. From the above displacement...
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