Deflection of Beam on Elastic Foundation-Finite Element Method-Assignment Solution, Exercises of Mathematical Methods for Numerical Analysis and Optimization

This assignment solution was submitted to Amar Sharma for Finite Element Method course at Aligarh Muslim University. It includes: Deflection, Beam, Elastic, Foundation, Dimensionless, Quantity, Transverse, Deflection, Galerkin, Method

Typology: Exercises

2011/2012

Uploaded on 07/08/2012

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Problem 5.3
The deflection of a beam on an elastic foundation is governed by the equation
(d4w/ dx4 ) +w=1, where x and w are dimensionless quantities. The boundary
conditions for a simply supported beam are given by transverse deflection =w=0
and bending moment = (d2w/ dx2 ) =0
By taking a two term trial solution W(x) = C1f1(x) +C2f2(x) with f1(x) =sinπx f2(x)
=sin3πx, find the solution of the problem using the Galerkin method.
SOLUTION
(d4w/ dx4 ) +w-1=0
Boundary conditions
W=0 d2w/dx2=0
At supports x=0, x=1
2 term trial solution is
W(x)= C1f1(x) +C2f2(x) with f1(x)= sinπx
F2(x) =sin3πx
Use of Glarkin method :
In Galerkin method ∫v fiRdv=0
So w(x) = C1sinπx+ C2 sin3πx
D4w/dx4= (π)4C1 sinπx+(3π)4C2sin3πx
Substitute values in governing equation, we obtain
R = (π)4 C1 sinπx +(3π)4C2sin3πx+C1 sinπx+C2 sin3πx-1
R= (π4+1)C1 sinπx+(81π4+1)C2 sin3πx-1
1f1(x)Rdx=01(sinπx)[ (π4+1)C1 sinπx+(81π4+1)C2 sin3πx]
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Problem 5.

The deflection of a beam on an elastic foundation is governed by the equation (d^4 w/ dx^4 ) +w=1, where x and w are dimensionless quantities. The boundary conditions for a simply supported beam are given by transverse deflection =w= and bending moment = (d^2 w/ dx^2 ) =

By taking a two term trial solution W(x) = C 1 f1(x) +C 2 f2(x) with f 1 (x) =sinπx f 2 (x) =sin3πx, find the solution of the problem using the Galerkin method.

SOLUTION

(d^4 w/ dx^4 ) +w-1=

Boundary conditions

W=0 d^2 w/dx^2 =

At supports x=0, x=

2 term trial solution is

W(x)= C 1 f1(x) +C 2 f2(x) with f 1 (x)= sinπx

F 2 (x) =sin3πx

Use of Glarkin method :

In Galerkin method ∫v fiRdv=

So w(x) = C 1 sinπx+ C 2 sin3πx

D^4 w/dx^4 = (π)^4 C 1 sinπx+(3π)^4 C 2 sin3πx

Substitute values in governing equation, we obtain

R = (π)^4 C 1 sinπx +(3π)^4 C 2 sin3πx+C 1 sinπx+C 2 sin3πx-

R= (π^4 +1)C 1 sinπx+(81π^4 +1)C 2 sin3πx-

∫1f1(x)Rdx=∫01(sinπx)[ (π^4 +1)C 1 sinπx+(81π^4 +1)C 2 sin3πx]

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By using orthogonality property

0 ∫^1 sin(mπx)sin(nπx)={ 0^ m≠n , ½ m=n

0 ∫^1 sin(mπx)=2/mπ^ if m is odd

So

0 ∫^1 f1(x)Rdx=C 1 /2 (π^4 +1)-2/π=

C 1 =4/π (π^4 +1)

0 ∫^1 f1(x) Rdx=^ ∫^ sin3πx[ (π^4 +1)C 1 sinπx+(81π^4 +1)C 2 sin3πx]

0 ∫^1 f1(x)Rdx=C 2 /2(81π^4 +1)-2/3π=

So w(x) =4/π[1/ (π4+1) *sinπx+sin3πx/(243π4+3)]

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