Problem - Lagrange function for mass on springs attached on a frame

In summary, the mass is on a rod attached to a frame with two springs. The mass is trying to move to a stationary position, but the springs are preventing it. The equations of motion for the mass are T=1/2mω2 and V=kx2*2. The system has two degrees of freedom, and the kinetic and potential energies can be expressed in coordinates that are convenient for the problem.
  • #1
asynja
16
0
Hello! I have a problem in classical mechanics that I'm unable to solve. Any help would be much appreciated since we have a partial exam tomorrow. :(

Homework Statement



There's a picture of the problem in the attachment

A mass m, which is on a light rod (lenght d), is attached to a square frame with sides 2d and to two springs with coefficient k, as shown on the picture. The length of unstreched springs is d. We put the frame on the surface and spin it around the point s with angular speed ω. We assume that there is no friction between mass and the surface and that springs can slide up and down the frame (they are not fixated).
Find the Lagrange function and the equation of motion for the mass.
Where are the stationary positions? For which coefficients k is the stationary position stable when the springs are the least streched?


Homework Equations



Lagrange's formalism

The Attempt at a Solution



T=1/2mω2 , V=kx2*2 , but then I don't know how to take into the account the effect that rod with length d has on the springs (it contributes that they are stretched more, right?)
 

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  • #2
I think it only acts as a constraint to keep the mass on a semi-circle.
 
  • #3
The d's make me think you need to take into account GPE. The way I was taught to setup a lagrangian is to NOT start in polar, but to start in cartesian and work you're way over to polar (for the position of the mass and thus velocities). There are "mysterious" cross-terms that pop up when you do it that way. Maybe there won't be in this system, but I don't know without actually setting it up.
Also, ##V_{spring}=\frac{1}{2}k\Delta x^2## and 2 springs gives you ##k\Delta x^2##, not ##2k\Delta x^2##

paisiello is correct, since the rod wasn't given a mass, you can simply act as though it's an imaginary rod, but I'm not even sure that you need to account for it in your constraints. You just need d for you moment of inertia.
 
  • #4
How many degrees of freedom does the system have? What sort of coordinates can describe those degrees of freedom conveniently? Can you express the kinetic and the potential energies of the system in those coordinates?
 
  • #5


Hi there,

Thank you for reaching out for help with your classical mechanics problem. It sounds like you are working on a problem involving a mass attached to springs on a rotating frame, which is a common problem in introductory mechanics courses. Based on the information provided, it seems like you have a good understanding of the problem and have correctly identified the relevant equations (kinetic and potential energy) to use in finding the Lagrange function.

To incorporate the effect of the rod with length d on the springs, you will need to consider the potential energy contribution from the rod as well. This can be done by breaking up the potential energy into two components - one from the springs and one from the rod. The potential energy from the rod can be calculated using the formula for gravitational potential energy, since the rod is acting as a pivot point for the mass. You can then add this potential energy to the potential energy from the springs to get the total potential energy of the system.

Once you have the Lagrange function, you can use the Euler-Lagrange equations to find the equations of motion for the mass. These equations will tell you how the position of the mass changes with time, taking into account the effects of the rotating frame and the springs. To find the stationary positions of the mass, you will need to set the equations of motion equal to zero and solve for the position of the mass. These positions will correspond to points where the mass is not moving, or is moving with a constant velocity.

To determine the stability of these stationary positions, you can use the second derivative test. This involves taking the second derivative of the potential energy with respect to the position of the mass and evaluating it at the stationary points. If the second derivative is positive, the stationary point is stable, and if it is negative, the stationary point is unstable.

I hope this helps you in solving your problem. Good luck on your exam tomorrow!
 

1. What is the Lagrange function for a mass on springs attached to a frame?

The Lagrange function, also known as the Lagrangian, is a mathematical function used in physics to describe the dynamics of a system. For a mass on springs attached to a frame, the Lagrange function is given by L = T - V, where T represents the kinetic energy of the system and V represents the potential energy of the springs.

2. How is the Lagrange function derived for this problem?

The Lagrange function is derived using the principle of least action, which states that the path taken by a system is the one that minimizes the action (the integral of the Lagrangian) between two points in time. By applying this principle to the system of a mass on springs attached to a frame, we can obtain the equations of motion for the system.

3. What are the equations of motion derived from the Lagrange function?

The equations of motion for a mass on springs attached to a frame can be obtained by taking the partial derivatives of the Lagrange function with respect to the position and velocity of the mass. This results in two second-order differential equations that describe the motion of the mass in the system.

4. How does the Lagrange function account for the constraints in this system?

The Lagrange function takes into account the constraints of the system by incorporating them into the equations of motion. These constraints, such as the fixed positions of the springs and the mass, are used to eliminate certain variables from the equations and simplify the calculations.

5. Can the Lagrange function be used for systems with multiple masses and springs?

Yes, the Lagrange function can be extended to systems with multiple masses and springs by incorporating the kinetic and potential energies of each individual mass and spring into the function. This allows for a more comprehensive analysis of the dynamics of the system and can be applied to a wide range of physical problems.

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