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1D Wave EquationThe derivation and solution for modeling a fixed-free cantilever

beam

Nick BrunoMAT 661

Spring 2010

If time… Extension to voltage in polyvinylidene fluoride (PVDF) strip

IntroductionThe lateral response of a vibrating cantilever beam is studied using the

wave equation by:

Deriving a fourth order wave equation considering a free body diagram.

Solving the equation using the technique of separation of variables with a Fourier expansion.

Finding orthogonal eigenfunctions and producing eigenvalues using root finding.

Applying initial conditions which are used to determine coefficients which yield a complete system time response.

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Introduction

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PZT - Lead zirconate titanate (MFC)

Derivation

A one dimensional beam will be considered with an applied distributed vertical load as seen below:

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Derivation

Summing all the forces in the z direction and moments about the origin “O” results in the following equations:

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We also know:

Derivation

Making substitutions with the latter yields:

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Which simplifies to a fourth order PDE for a uniform beam…

orwhere

Free vibration

Separation of VariablesLetting the response equal the product of independent

functions, separating the variables, and setting them equal to a positive separation constant yields the following:

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Application of Boundary Conditions

The boundary conditions for a cantilever beam are defined by:

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No Displacement @ x =0 No Slope @ x =0 No Bending

Moment @ x = LNo Shear Force @ x = L

These translate to the following for our eigenvalue problem:

We will use these

Application of Boundary Conditions

This results in a system of equations that can be used to determine the eigenvalues and a relation between coefficients C1 and C2

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In order for a non-trivial solution to be found

so equating zero with the determinant of the 2X2 matrix seen will yield eigenvalues for the system

Application of Boundary Conditions

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Application of Boundary Conditions

The relation between C1 and C2 can be found as follows:

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Application of Initial ConditionsRemember from before…

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The chosen initial conditions for the beam are as follows:

whereδ= 0.004 [m] = Initial displacement at the tipL = 0.107 [m] = Length of the beamthus,

Orthogonality?Before solving for An we must first check orthogonality of the

eigenfunctions.

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Check

Example Solution

Use inner products

No weight function!

Assuming convergence

Summary of Data

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Summary of Data

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Summary of Data

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Summary of Data

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Summary of Data

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Summary of Data

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u

ut utt

Summary of Data

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Summary of Data

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V * %e

Comparable

Sodano et al. 2003

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