Doubts in Differential equations

Click For Summary

Discussion Overview

The discussion revolves around second order differential equations, particularly in the context of simple harmonic motion (SHM). Participants explore the nature of solutions to these equations, the validity of different proposed forms, and the implications of adding solutions. The conversation includes technical reasoning, challenges to claims, and inquiries about specific scenarios involving forces and mass systems.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a second order differential equation for SHM and questions why a polynomial solution is not considered valid, suggesting that it could also satisfy the equation.
  • Another participant challenges this claim, pointing out the lack of time dependence in the proposed polynomial solution.
  • A later reply corrects the time variable in the polynomial but still raises questions about the nature of solutions.
  • Another participant suggests that the guessed solution form is based on experience and relies on broader mathematical results to assert that sine and cosine functions are the only solutions for the given differential equation.
  • One participant expresses confusion about the existence of infinite solutions for a different differential equation and questions how to solve for a constant term in the equation.
  • Another participant notes that if coefficients satisfy certain conditions, only specific solutions exist, and proposes a form for the particular solution involving a constant.

Areas of Agreement / Disagreement

Participants express differing views on the validity of certain proposed solutions and the nature of infinite solutions. There is no consensus on the best approach to solving the equations presented, and the discussion remains unresolved regarding the handling of constant terms in the equations.

Contextual Notes

Participants highlight limitations in their reasoning, including assumptions about the forms of solutions and the implications of adding solutions. The discussion reflects a reliance on experience and established mathematical results without reaching definitive conclusions.

siddharth
Homework Helper
Gold Member
Messages
1,145
Reaction score
0
If I have a second order differential equation (like in SHM) ,ie, (d^2x)/(dt^2)=-kx, (1) the solution is of the form Acos(wt+B) (2). This is obviously true because by substituting i get the result. But the answer could very well have been [-(kx^3)/6 +AX^2+BX + C]. Why do we not take this answer to solve the SHM problems?

Also, if I am solving the above differential equation, instead of equating (1) to -kx i could have equated it to zero and found the solution, and added to (2). It would still satisfy the equation. So I could keep adding many such solutions to (2). But then there would be an infinite number of solutions! How is that possible??

And finally what if I have (d^2x)/(dt^2)=-kx + C .What would be the general solution (I know that the frequency will not change).For example if I have a spring with two masses m1 and m2 on either side and I apply a force F1 and F2 respectivley on each of them, what would be the equation of motion of the center of mass?
It would be very helpful if anyone can tell me the equation or how to solve the Differential equation.
 
Physics news on Phys.org
"If I have a second order differential equation (like in SHM) ,ie, (d^2x)/(dt^2)=-kx, (1) the solution is of the form Acos(wt+B) (2). This is obviously true because by substituting i get the result. But the answer could very well have been [-(kx^3)/6 +AX^2+BX + C]. Why do we not take this answer to solve the SHM problems"
This is simply incorrect; where's your "t" dependence here, which is the one you differentiate with respect to?
 
OOPS! sorry i mean [-(kt^3)/6 +At^2+Bt + C].
 
Well, you could suggest that might be the answer, but if you put it into the equation, then it doesn't satisfy the differential equation.

We guess what the solution might be, because of experience, and then use some large result that states that this is the only answer.

d^2x/dt^2=-kx

tells us that the function x(t) is one that when differentiated twice gives us the negative of what we started with. Experience tells us that sin and cos are such functions, so we guess and answer, show it's ok, and then rely on the larger results to know these are the only ones.

writing L for the differential operator of diffin twice wrt to t

we solve Lx=-kx+C by solving the homogenous part


Lx+kx=0, and then by solving for the particular solution involving C.
 
Last edited:
Oh, i got it. I was just being plain stupid in the differentiation bit. But if I have
(d^2x)/(dt^2) + dx/dt = 0. Then I could have x(t) = A(e^Bt) + A1(e^b1t) + ...
such that B(B+1)=0 , B1(B1+1)=0, ...
So i would still have infinite soultions.
Solving Lx + kx =0 is fine. But if C is a constant, then how am I supposed to solve Lx=-kx+c?
Thanks for the help.
 
Last edited:
if the coefficients B and B1 etc all satisfy y(y+1)=0 then there are only two possibilities, 0 and -1.


As for solving the particular bit, I'd guess a polynomial in t, possibly of the form x(t)=C/k, or possilby -C/k, your minus signs are changing somewhat randomly.
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 16 ·
Replies
16
Views
3K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 19 ·
Replies
19
Views
5K
  • · Replies 8 ·
Replies
8
Views
2K