Download A characteristic property of spherical caps by Ripoll J. PDF

By Ripoll J.

Show description

Read or Download A characteristic property of spherical caps PDF

Best nonfiction_1 books

Racing in the Street: The Bruce Springsteen Reader

For greater than 3 a long time, Bruce Springsteen’s skill to precise in phrases and track the private hopes, fears, loves, and sorrows of commonplace american citizens has made him a hero to his hundreds of thousands of dedicated lovers. Racing on the street is the 1st entire selection of writings approximately Springsteen, that includes the main insightful, revealing, well-known, and notorious articles, interviews, experiences, and different writings.

Wrightscapes - Frank Lloyd Wrights LandscapeDesigns

Here's the 1st publication to envision the environmental panorama designs of Frank Lloyd Wright, most likely the world's top identified and so much influential architect. WRIGHTSCAPES analyzes eighty five of his works, and will pay specific cognizance to web site making plans, panorama layout, neighborhood scale, and local making plans.

Extra resources for A characteristic property of spherical caps

Example text

It is simpler to handle this quantity rather than the initial function, as the negative frequencies have been removed. Many authors use the time dependence exp(−j ωt), where the positive frequencies are removed. The complex representation of a wave travelling in the direction of positive x will be exp[j (k ∗ x − ωt)], because decreasing the amplitude in the direction of propagation implies that the new wave number is the complex conjugate of k. When adding the positive frequency components of a real signal to its negative frequency components, the initial real signal must be obtained.

2) where η is the shear viscosity (the volume viscosity is neglected), κ is the thermal conductivity, cp is the specific heat per unit mass at constant pressure. 6 10−2 w m−1 k−1 . The pressure is considered constant on a cross- section of the tube. 1, with a velocity υ(0, 0, υ3 ) parallel to the x3 axis and whose magnitude only depends on x1 . The variation of this velocity with x1 produces viscous stress. Due to the viscosity, the air is subjected to a shear force parallel to the x3 axis, and proportional to ∂υ3 /∂x1 .

The description of sound propagation in porous material can be complicated by the fact that sound also excites and moves the frame of the material. If the frame is motionless, in a first step, the air inside the porous medium can be replaced on the macroscopic scale by an equivalent free fluid. This equivalent fluid has a complex effective density ρ and a complex bulk modulus K. The wave number k and the characteristic impedance Zc of the equivalent fluid are also complex. 7, the porous layer can be replaced by a fluid layer of density ρ/φ and of bulk modulus K/φ.

Download PDF sample

Rated 4.89 of 5 – based on 15 votes