Solving a coupled nonhomegenoues ode

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Homework Help Overview

The discussion revolves around solving a coupled system of nonhomogeneous ordinary differential equations (ODEs) involving two variables, ω₁ and ω₂, with real, positive constants λ and μ. The participants are exploring the implications of the nonhomogeneous term μ and how it affects the solution structure.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the general form of the solution and the role of the nonhomogeneous term μ. There are attempts to derive the equations by taking derivatives and substituting variables, with some uncertainty about how to handle the constant term. Questions arise regarding the validity of initial guesses for the solution and the impact of the constants λ and μ on the final expressions.

Discussion Status

The discussion is active, with participants providing guidance on how to approach the problem. There is recognition of incorrect solutions and an emphasis on showing work to clarify reasoning. Some participants suggest checking derived expressions against the original equations to validate the approach.

Contextual Notes

Participants are working under the constraints of initial conditions for ω₁ and ω₂, and there is an ongoing debate about the treatment of the nonhomogeneous term μ in the context of the differential equations.

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Homework Statement



[itex]\dot{ω_{1}}[/itex] = λ[itex]ω_{2}[/itex] +μ
[itex]\dot{ω_{2}}[/itex] = -λ[itex]ω_{1}[/itex]

Homework Equations



λ and μ are real, positive constants
[itex]ω_{1}[/itex](0) ≠ 0
[itex]ω_{2}[/itex](0) ≠ 0

The Attempt at a Solution



I know that the general solution will be in the form
ω1(t) = A sin ωt + B cos ωt + C
ω2(t) = D sin ωt + E cos ωt
but I'm not sure how to solve it

Eqn 2 becomes:
[itex]\ddot{ω_{2}}[/itex] = -λ[itex]\dot{ω_{1}}[/itex]
Substituting equation 1:
[itex]\ddot{ω_{2}}[/itex] = -λ[itex]^{2}[/itex][itex]ω_{2}[/itex] +λμ

I'm really just unsure of how to handle the constant when you solve it as a nonhomegenous equation.
 
Last edited:
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dawgs1236 said:

Homework Statement



[itex]\dot{ω_{1}}[/itex] = λ[itex]ω_{2}[/itex] +μ
[itex]\dot{ω_{2}}[/itex] = -λ[itex]ω_{1}[/itex]

Homework Equations



λ and μ are real, positive constants
[itex]ω_{1}[/itex](0) ≠ 0
[itex]ω_{2}[/itex](0) ≠ 0

The Attempt at a Solution



I know that the general solution will be in the form
ω1(t) = A sin ωt + B cos ωt + C
ω2(t) = D sin ωt + E cos ωt
but I'm not sure how to solve it

Take another derivative of the first equation and substitute the second one into it.
 
Yeah I know how to do that part. I'm really just not sure what to do about the μ on the end. When I take the derivative it should disappear but I don't think it should.
 
Well, if it's a constant, then it should...

You can of course take the derivative of the second equation and use the first.
 
So does μ affect this problem?

the answers I came up with were

[itex]ω_{1}[/itex](t) = [itex]ω_{2}[/itex](0) sin ωt + [itex]ω_{1}[/itex](0) cos ωt
[itex]ω_{2}[/itex](t) = [itex]ω_{1}[/itex](0) sin ωt + [itex]ω_{2}[/itex](0) cos ωt

but these were wrong
 
Of course they're wrong, there's no evidence of mu and lambda.
 
dawgs1236 said:
Yeah I know how to do that part. I'm really just not sure what to do about the μ on the end. When I take the derivative it should disappear but I don't think it should.

I think the μ will disappear when you take the derivative. That's ok. Just keep working. It will come back into the solution later. Show your work.
 
dextercioby said:
Of course they're wrong, there's no evidence of mu and lambda.

Obviously I know they're wrong. Why else would I post this here? I posted it here looking for help with the solution not conformation that I was incorrect.
 
dawgs1236 said:
Obviously I know they're wrong. Why else would I post this here? I posted it here looking for help with the solution not conformation that I was incorrect.

Can't say why you got incorrect solutions until you show how you got them.
 
  • #10
Would it be a good idea to take the second derivative of :
ω2(t) = D sin ωt + E cos ωt
and plug them them into:
ω2¨ = -λ^2ω2 +λμ
and then use the initial conditions?
 
  • #11
dawgs1236 said:
Would it be a good idea to take the second derivative of :
ω2(t) = D sin ωt + E cos ωt
and plug them them into:
ω2¨ = -λ^2ω2 +λμ
and then use the initial conditions?

It would be a good idea to say how you got ω2(t) = D sin ωt + E cos ωt. It looks like you are just plugging in a guess for the answer. And the guess is wrong. Why don't you start with the part we agreed on? Solve (ω1)''=(-λ^2ω1).
 
  • #12
I did just guess at that.

okay so I set up the characteristic equation and got sqrt(λ) as the answer. would that make it:
ω1(t) = A sin sqrt(λ)t + B cos sqrt(λ)t + C ?
 
  • #13
dawgs1236 said:
I did just guess at that.

okay so I set up the characteristic equation and got sqrt(λ) as the answer. would that make it:
ω1(t) = A sin sqrt(λ)t + B cos sqrt(λ)t + C ?

Good, you're getting started. Try to check that, plug it into (ω1)''=(-λ^2ω1). You should realize the the sqrt(λ) isn't quite right. I get a characteristic equation of x+λ^2=0. And does the C really belong there?
 
Last edited:
  • #14
Okay so ω=-λ
working that out I came up with:

ω1(t) = w1(0) cos -λt - [w2(0) + μ/λ] sin -λt
ω2(t) = w1(0) sin -λt + [w2(0) + μ/λ] cos (-λt) - μ/λ
 
  • #15
dawgs1236 said:
Okay so ω=-λ
working that out I came up with:

ω1(t) = w1(0) cos -λt - [w2(0) + μ/λ] sin -λt
ω2(t) = w1(0) sin -λt + [w2(0) + μ/λ] cos (-λt) - μ/λ

That works. It would maybe look a little nicer if you would get rid of the signs on λ using trig, but it works. You've certainly gotten a lot better at this since your last post.
 
Last edited:

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