In this study, the dispersal caused by transverse Poisson’s effect in a magneto-electro-elastic (MEE) circular rod is taken into consideration using nonlinear longitudinal wave equation (LWE), mathematical physics problem. Using generalized exp-function method, we investigate families of solitary solutions one-dimensional LWE. computer program Wolfram Mathematica 10, these new exact and LWE are...

The design of an optimized near-perfect reconstruction (NPR) type trans-multiplexer has been proposed. Cosine modulation has been used to design the synthesis and analysis sections of the trans-multiplexer. The design of transmultiplexer was reduced to design of single low-pass prototype FIR filter which is designed using variable window function (Kaiser, Cosh and DolphChebyshev). An unconstrai...

Thermodynamic properties of the anisotropic BlurneEmery-Griffiths model are discussed in the new type of effective-field theory, A new disordered phase which may correspond to the staggered quadrupolar phase predicted by the Monte Carlo simulation is found and its physical contents are investigated. The anisotropic Blume-Emery-Griffiths (BEG) a where V, = ( p = X, y) gives the two differential ...

In this paper, we consider the correspondence between tachyon dark energy model and Tsallis holographic scenario in an FRW universe.We demonstrate description of universe reconstruct potential basic results dynamics scalar field which describe cosmology. a flat universe, energy, independent existence interaction matter or not, \dot{T}^2 must always be zero. Therefore, equation state {\omega}_D ...

Assume cosh−1 (−I) 3 {∑π I′=i J (h) ( 0 + g′, 1 Θ̄ ) , W (μ) ∼ א0 ∫ א0 e ⋃ ψI,ζ∈θ tan (א0) dZ, t̃(Õ) ⊃ e . The goal of the present article is to construct additive matrices. We show that i−∞ > min g′→0 a (γ, . . . , c(ρ)) ∨ · · · × −1א0

35 where the expectation value is deened by hA(x)i = R dx e ?x 2 p 2 cosh m (p 2x)A(x) R dx e ?x 2 p 2 cosh m (p 2x) : (62) Inserting in (56) this value of we have searched among the 5 values of g the one which gives the maximum free energy when the stability is marginal (i.e. when (56) is saturated). We have found that the eigenvalue g 5 is the one which gives the maximal free energy. This lea...