Second order Autonomous Differential Equations

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The discussion revolves around solving the second-order autonomous differential equation d²R/dt² = W²R, where R represents radial position and W is a constant angular velocity. A participant suggests using the substitution v = dR/dt to convert the equation into a first-order separable form, leading to the integration of both sides. The solution is derived as R = a sinh(Wt + arcsinh(R0/a)), with a defined in terms of initial conditions. Another method is proposed, assuming R = e^(kt), which simplifies the problem and yields the same result. The conversation highlights the importance of recognizing different approaches to solving differential equations.
roamer
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Hi All,
I have a differntial equation that I came up with on a little engineering problem posted here https://www.physicsforums.com/showthread.php?t=129247 that I can't solve. It is d^2R/dt^2=W^2*R where R is radial position and W is angular velocity and t is time. I think it is an autonomous diff eq. but don't know, its been a while since math class. Any ideas?? Thanks
 
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W is a constant?

if so we can solve it relatively easy.

Introduce v = dR/dt. Then the differential equation is
v dv/dR = W^2 R.

Integrating once gives
v^2 - v0^2 = W^2 R^2 - W^2 R0^2
Where i have assumed v(t=0) = v0 and R(t=0) = R0.

a quick arrangement
v = +/- sqrt( v0^2 - W^2 R0^2 + W^2 R^2 )

and thus dR/dt = +/- sqrt( v0^2 - W^2 R0^2 + W^2 R^2 )

This is a seperable first order ODE

define a such that W^2 a^2 = v0^2 - W^2 R0^2

Then
dR/dt = +/- sqrt(W^2 a^2 + W^2 R^2)

dR/sqrt(a^2 + R^2) = +/- W dt

The right hand side is +/- Wt.
To integrate the left hand side Put R = a*sinh(x) so that
dR = a cosh(x) dx then
sqrt( a^2 + R^2 ) = sqrt(a^2 + a^2 sinh^2(x)) = a sqrt(1 + sinh(x)^2)
= a sqrt(cosh^2(x)) = a*cosh(x).

This dR/sqrt(a^2 + R^2) -> dx
The integral is thus

arcsinh(R/a) - arcsinh(R0 / a) = +/- Wt
and therefore

R = a sinh( +/- Wt + arcsinh(R0 / a))
and a = sqrt(V0^2/W^2 - R0^2).

Plugging this in and checking shows us that the
- sign gives the v(0) = - v0

Therefore

R = a sinh( Wt + arcsinh(R0 / a))
 
Last edited:
just shows to go you, when your tool is a hammer...
i was thinking about the trick v =dR/dt so that was the
first way i did this problem.

ergh! the easier (more standard way) assume
R = e^kt then the differential equation gives
k^2 = W^2 so that

R = A exp(Wt) + B exp(-Wt)

introducing the initial values you get the same
answer as above but easier.
 
qbert,
Thanks for the answers. I know exactly what you mean about going about problems with the wrong tool, still it is at least good to know you can grind out answers in more than one way even if your first choice isn't the easiest.
 
"autonomous" equations are those in which the independent variable does not appear explicitly. Second order autonomous equations are those of the form \frac{d^2y}{dx^2}= f(y,y') and, as qbert said, letting v= y' is a standard method (its' called "quadrature"). If v= y', then
\frac{d^2y}{dx^2}= \frac{dv}{dt}= \frac{dv}{dy}\frac{dy}{dt}= v\frac{dv}{dy}
so that the second order equation reduces to a first order equation
v\frac{dv}{dy}= f(y,v)[/itex]. After you have solved for v, integrate to find y.
 

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