What Is the Equation of Motion for a Pivoted Rod on an Accelerating Car?

AI Thread Summary
The discussion focuses on deriving the equation of motion for a pivoted rod on an accelerating car. The equilibrium angle between the rod and the car's top is determined using Newton's second law, resulting in the equation tan(equilibrium angle) = g/A. For small displacements from equilibrium, participants suggest using torque and moment of inertia to derive the motion equation, with simplifications for small angles. The stability of the equilibrium angle is debated, with indications that it may be stable based on the behavior of the second derivative at equilibrium. Overall, the conversation emphasizes the application of physics principles to solve the problem effectively.
matpo39
Messages
40
Reaction score
0
a uniform thin rod of length L and mass m is pivoted at one end the point is attached to the top of a car accelerating at a rate A.

a) what is the equilibrium angle between the rod and the top of the car?
b) suppose that the rod is displaced a small angle phi from the equilibrium derive the equation of motion for phi. Is the equilibrium angle stable or unstable?

I was able to get part a which using Newtons 2nd law for non inertial frames is
tan(equilibrium angle) = g/A.

but i am stuck on part b. I could use the lagrangian method to get phi(double dot) but that would be really messy, and was wondering if there would be a better way of getting it. oh and also he gave the hint to ignore air resistance and that torque= I*alpha.

thanks
 
Physics news on Phys.org
matpo39 said:
a uniform thin rod of length L and mass m is pivoted at one end the point is attached to the top of a car accelerating at a rate A.

a) what is the equilibrium angle between the rod and the top of the car?
b) suppose that the rod is displaced a small angle phi from the equilibrium derive the equation of motion for phi. Is the equilibrium angle stable or unstable?

I was able to get part a which using Newtons 2nd law for non inertial frames is
tan(equilibrium angle) = g/A.

but i am stuck on part b. I could use the lagrangian method to get phi(double dot) but that would be really messy, and was wondering if there would be a better way of getting it. oh and also he gave the hint to ignore air resistance and that torque= I*alpha.

thanks

Getting the equation isn't hard but solving it might be...

I'm going to take theta to be the total angle from the horizontal, and phi as the angle from the equilibrium point.

Calculate the torque acting on the rod... this is in terms of theta. Then write down I * alpha = torque.

Plug in the value of I in terms of m and L. Plug in \alpha=\frac{d^2\theta}{dt^2}

Then finally replace \theta with \phi + tan^{-1}(g/A)

That seems to give you the equation you need. It's a second order diff. equation... I'm not sure of the solution right now. But do you need the solution?
 
thanks for the help, it seems i forgot that alpha= phi(double dot), as soon i understood that the rest of the problem wasnt too hard.
 
The differential equation may be simplified for small \phi, since

\sin\phi = \phi and

\cos\phi = 1 (approximately).

I don't know how to write ~ in latex.
 
matpo39 said:
thanks for the help, it seems i forgot that alpha= phi(double dot), as soon i understood that the rest of the problem wasnt too hard.

I'm curious about the final solution to this problem... Did you have to solve the diff. eq? If you did, can you post it?

It seems stable to me because the second derivative of phi, is zero at the equilibrium point... but I'm not sure if this is the correct reasoning.
 
This what you're looking for?

\approx
 
Thank you Hurkyl, that's what I was looking for.
 
Back
Top