Transient Bending Wave Propagation in Anisotropic Plates

1998 ◽  
Vol 65 (4) ◽  
pp. 930-938 ◽  
Author(s):  
K.-E. Fa¨llstro¨m ◽  
O. Lindblom
Keyword(s):  
Experimental Data ◽  
Wave Propagation ◽  
Integral Representation ◽  
Orthotropic Plate ◽  
Representation Formula ◽  
Rotary Inertia ◽  
Anisotropic Plates ◽  
Bending Waves ◽  
Integral Representation Formula ◽  
Bending Wave

In this paper we study transient propagating bending waves. We use the equations of orthotropic plate dynamics, derived by Chow about 25 years ago, where both transverse shear and rotary inertia are included. These equations are extended to include anisotropic plates and an integral representation formula for the bending waves is derived. Chow’s model is compared with the classical Kirchoff’s model. We also investigate the influence of the rotary inertia. Comparisons with experimental data are made as well.

scholarly journals Integral Representation for the Solutions of Autonomous Linear Neutral Fractional Systems with Distributed Delay

Mathematics ◽  
2020 ◽  
Vol 8 (3) ◽  
pp. 364
Author(s):  
Ekaterina Madamlieva ◽  
Mihail Konstantinov ◽  
Marian Milev ◽  
Milena Petkova
Keyword(s):  
Integral Representation ◽  
Distributed Delay ◽  
Representation Formula ◽  
Neutral Systems ◽  
Initial Value ◽  
Fractional Systems ◽  
Integral Representation Formula ◽  
Linear Differential Systems ◽  
Linear Differential ◽  
Fractional Neutral Systems

The aim of this work is to obtain an integral representation formula for the solutions of initial value problems for autonomous linear fractional neutral systems with Caputo type derivatives and distributed delays. The results obtained improve and extend the corresponding results in the particular case of fractional systems with constant delays and will be a useful tool for studying different kinds of stability properties. The proposed results coincide with the corresponding ones for first order neutral linear differential systems with integer order derivatives.

scholarly journals Explicit Stencil Computation Schemes Generated by Poisson's Formula for the 2D Wave Equation

2019 ◽  
Author(s):  
Naum Khutoryansky
Keyword(s):  
Wave Equation ◽  
Finite Difference ◽  
Integral Representation ◽  
Initial Conditions ◽  
Representation Formula ◽  
Time Step ◽  
Stencil Computation ◽  
Integral Representation Formula ◽  
Time Marching ◽  
First Time

An approach to building explicit time-marching stencil computation schemes for the transient 2D acoustic wave equation without using finite-difference approximations is proposed and implemented. It is based on using the integral representation formula (Poisson's formula) that provides the exact solution of the initial-value problem for the transient 2D scalar wave equation at any time point through the initial conditions. For the purpose of constructing a two-step time-marching algorithm, a modified integral representation formula involving three time levels is also employed. It is shown that integrals in the two representation formulas are exactly calculated if the initial conditions and the sought solution at each time level as functions of spatial coordinates are approximated by stencil interpolation polynomials in the neighborhood of any point in a 2D Cartesian grid. As a result, if a uniform time grid is chosen, the proposed time-marching algorithm consists of two numerical procedures: 1) the solution calculation at the first time-step through the initial conditions; 2) the solution calculation at the second and next time-steps using a generated two-step numerical scheme. Three particular explicit stencil schemes (with five, nine and 13 space points) are built using the proposed approach. Their stability regions are presented. The obtained stencil expressions are compared with the corresponding finite-difference schemes available in the literature. Their novelty features are discussed. Simulation results with new and conventional schemes are presented for two benchmark problems that have exact solutions. It is demonstrated that using the new first time-step calculation procedure instead of the conventional one can provide a significant improvement of accuracy even for later time steps.

A Dirichlet Problem for the Inhomogeneous Polyharmonic Equation in the Upper Half Plane

2007 ◽  
Vol 14 (1) ◽  
pp. 33-52
Author(s):  
Heinrich Begehr ◽  
Evgenija Gaertner
Keyword(s):  
Dirichlet Problem ◽  
Green Function ◽  
Differential Operator ◽  
Integral Representation ◽  
Half Plane ◽  
Representation Formula ◽  
Higher Order ◽  
Polyharmonic Equation ◽  
Integral Representation Formula ◽  
Upper Half Plane

Abstract On the basis of a higher order integral representation formula related to the polyharmonic differential operator and obtained through a certain polyharmonic Green function, a Dirichlet problem is explicitly solved in the upper half plane.

Axially Symmetric Stress Distributions in Elastic Solids Containing Penny-Shaped Cracks Under Torsion

1975 ◽  
Vol 42 (4) ◽  
pp. 896-897 ◽  
Author(s):  
M. L. Pasha
Keyword(s):  
Stress Intensity ◽  
Integral Representation ◽  
Elastic Medium ◽  
Stress Intensity Factors ◽  
Representation Formula ◽  
Stress Distributions ◽  
Axially Symmetric ◽  
Intensity Factors ◽  
Elastic Solids ◽  
Integral Representation Formula

We present the axially symmetric stress distributions in elastic solids containing a pair of axially symmetric penny shaped cracks when the infinite elastic medium is kept under torsion. We derive the integral representation formula for the torsion function and the expressions for the stress-intensity factors.

scholarly journals The Newtonian Potential and the Demagnetizing Factors of the General Ellipsoid

2017 ◽  
Author(s):  
Giovanni Di Fratta
Keyword(s):  
Integral Representation ◽  
Explicit Expression ◽  
Representation Formula ◽  
Newtonian Potential ◽  
Bounded Domains ◽  
Dimensional Problem ◽  
Smooth Functions ◽  
Integral Representation Formula ◽  
Transport Theorem ◽  
Stokes Integral

The objective of this paper is to present a modern and concise new derivation for the explicit expression of the interior and exterior Newtonian potential generated by homogeneous ellipsoidal domains in $\mathbb{R}^N$ (with $N \geqslant 3$). The very short argument is essentially based on the application of Reynolds transport theorem in connection with Green-Stokes integral representation formula for smooth functions on bounded domains of$\mathbb{R}^N$, which permits to reduce the N-dimensional problem to a 1-dimensional one. Due to its physical relevance, a separate section is devoted to the derivation of the demagnetizing factors of the general ellipsoid which are one of the most fundamental quantities in ferromagnetism.

Modal density and critical frequency of composite panels considering transverse shear deformation and rotary inertia

2020 ◽  
Vol 26 (17-18) ◽  
pp. 1503-1513
Author(s):  
K Renji
Keyword(s):  
Shear Deformation ◽  
Transverse Shear ◽  
Critical Frequency ◽  
Rotary Inertia ◽  
Transverse Shear Deformation ◽  
Bending Waves ◽  
Modal Density ◽  
The Face ◽  
Orthotropic Properties ◽  
Bending Wave

In this work, expressions for estimating the modal density, speed of the bending wave, critical frequency and coincidence frequency of panels are derived considering orthotropic properties of the face sheets, transverse shear deformation and the rotary inertia. Presence of rotary inertia results in an increase in the modal density and a reduction in the speed of the bending waves. The influence is significant at higher frequencies. The critical and coincidence frequencies increase due to rotary inertia. Results for a typical equipment panel of spacecraft are presented and they show the need for incorporating rotary inertia while determining these parameters.

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