

Study with the several resources on Docsity
Earn points by helping other students or get them with a premium plan
Prepare for your exams
Study with the several resources on Docsity
Earn points to download
Earn points by helping other students or get them with a premium plan
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
1 / 2
This page cannot be seen from the preview
Don't miss anything!


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]
docsity.com
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)]
docsity.com