Forced Vibrating Membranes and Resonance - Separation of Variables

Click For Summary
SUMMARY

The discussion focuses on solving the forced vibrating membranes equation, represented as Utt = c²∇²U + Q, where the eigenfunction series solution involves coefficients defined by d²/dt²(A_n) + c²λ_nA_n = q_n. The user attempts to apply the variation of parameters method to derive a single integral term from the homogeneous and particular solutions. Key equations include A_n = c1 * cos(c√λ_n * t) + c2 * sin(c√λ_n * t) and the integral form involving q_n. The solution requires careful manipulation of integrals and verification of trigonometric identities.

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Familiarity with eigenfunction expansions
  • Knowledge of variation of parameters method
  • Proficiency in trigonometric identities
NEXT STEPS
  • Study the method of separation of variables in PDEs
  • Learn about eigenvalue problems in differential equations
  • Explore the variation of parameters technique in detail
  • Review trigonometric identities and their applications in integral calculus
USEFUL FOR

Students and professionals in applied mathematics, particularly those working with differential equations, as well as engineers dealing with vibrational analysis and resonance phenomena.

veneficus5
Messages
14
Reaction score
0

Homework Statement



In the midst of Forced Vibrating Membranes and Resonance Utt = c^2*delsquared(U) + Q(heat source)

Arrive at eigenfunction series solution where the coefficients are given by
d^2/dt^2 (A_n) + c^2*lambda_n*A_n = q_n

Homework Equations



according to the book, I am supposed to arrive here

A_n = c1 * cos (c*sqrt(lambda_n)*t) + c2 * sin (c*sqrt(lambda_n)*t) <--- homogeneous part of solution + particular solution ---> integral from 0 to t of (q_n * sin (c*sqrt(lambda_n)*(t-tau)) / (c*sqrt(lambda_n)) with respect to tau.

The Attempt at a Solution



Now when I try the variation of parameters (given my two homogeneous solutions already which match with the book),
I get
-cos(c*sqrt(lambda_n)*t) * integral of ( q_n * sin (c*sqrt(lambda_n)*t) / c*sqrt(lambda_n) + -sin(c*sqrt(lambda_n)*t) * integral of ( q_n * sin (c*sqrt(lambda_n)*t) / c*sqrt(lambda_n)

How do I reconcile this into the single integral term, the definite integral that I am supposed to get?

Thanks
 
Physics news on Phys.org
veneficus5 said:
-cos(c*sqrt(lambda_n)*t) * integral of ( q_n * sin (c*sqrt(lambda_n)*t) / c*sqrt(lambda_n) + -sin(c*sqrt(lambda_n)*t) * integral of ( q_n * sin (c*sqrt(lambda_n)*t) / c*sqrt(lambda_n)

How do I reconcile this into the single integral term, the definite integral that I am supposed to get?

Thanks

If you write these integrals in terms of the dummy variable \tau, you can simplify the expression using the trig identities for \sin(A\pm B). You should double check your signs, since your expression doesn't seem to reduce to the answer that you claim.
 

Similar threads

  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 22 ·
Replies
22
Views
3K
Replies
7
Views
5K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 27 ·
Replies
27
Views
4K
  • · Replies 6 ·
Replies
6
Views
2K