Resonance in a Mechanical System

In summary, the conversation discusses a problem involving a mass attached to a spring that is free to turn about a nail on a frictionless surface. The question asks for the length of the spring as a function of the angular frequency of revolution. The attempted solution involves equations for the elastic force and the force required for circular motion, but there is confusion about the use of "l" to designate the length of the spring and the unstretched length. The hint suggests considering the elastic force when the spring's length is the unstretched length.
  • #1
amk1995
4
0

Homework Statement


A mass m is attached to one end of a massless spring with a force constant k and an unstretched length l0. The other end of the spring is free to turn about a nail driven into a frictionless, horizontal surface. The mass is made to revolve in a circle with an angular frequency of revolution ω.
Question:
Calculate the length l of the spring as a function of ω.

Homework Equations


F = ω2*l*m
FSpring = k*l


The Attempt at a Solution


Fspring = Fcirc
-k*l = ω2*l*m

The issue I am having is how to get L by itself, or what I am supposed to do with l0. Can someone guide me on where I should head in order to solve this problem? The issue is l cancels when I divide, unless I am supposed to use l0 in place of l
Thanks!
 

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  • #2
You are using "l" to designate two different things.
If "l" in the first equation is the total length of the spring (radius of the circle), then the elastic force is not correct. The force does not depend on the total length.
What is the force when the length is lo?
 
  • #3
The force when length lo is just omega^2 *m*lo correct?
 
  • #4
No. What is the elastic force ("produced" by the spring) when the spring's length is lo?
Hint: at lo the spring is unstretched.
 
  • #5


I can guide you in solving this problem by providing you with the necessary steps and equations. First, let's define the variables involved in this problem:

m = mass attached to the spring
k = force constant of the spring
l0 = unstretched length of the spring
l = length of the spring when stretched
ω = angular frequency of revolution

Now, let's look at the forces acting on the mass:

1. Centripetal force (Fc): This is the force that keeps the mass moving in a circular motion and is given by Fc = mω2l.

2. Spring force (FSpring): This is the force exerted by the spring on the mass and is given by FSpring = k(l-l0).

Since the mass is in equilibrium, these two forces must be equal in magnitude and opposite in direction. Therefore, we can set them equal to each other:

Fc = FSpring
mω2l = k(l-l0)

Now, we can solve for l:

l = (mω2l + kl0)/k

This is the length of the spring as a function of ω. We can also simplify this equation by factoring out l:

l = (mω2 + k)l0/k

This equation shows that the length of the spring is directly proportional to the angular frequency ω. As ω increases, the length of the spring also increases. We can also see that the length of the spring is inversely proportional to the force constant k. As k increases, the length of the spring decreases.

I hope this helps you in solving the problem. Remember to always define your variables and use the appropriate equations to find the solution.
 

What is resonance in a mechanical system?

Resonance in a mechanical system refers to the phenomenon where the system vibrates at its natural frequency when subjected to external forces. This can cause the amplitude of the vibration to increase significantly.

What factors affect the resonance frequency of a mechanical system?

The resonance frequency of a mechanical system is affected by its mass, stiffness, and damping. A higher mass or stiffness will result in a lower resonance frequency, while a higher damping will decrease the resonance frequency.

How does resonance impact the performance of a mechanical system?

Resonance can have both positive and negative impacts on the performance of a mechanical system. It can be beneficial in applications such as musical instruments, where resonance is desired. However, in other systems, resonance can cause excessive vibrations and ultimately lead to mechanical failure.

How can resonance be prevented in a mechanical system?

Resonance can be prevented by avoiding the system's natural frequency or by changing the system's mass, stiffness, or damping. Damping can be increased by adding materials such as rubber or foam to absorb the vibrations.

What are some real-world examples of resonance in mechanical systems?

Some common examples of resonance in mechanical systems include tuning forks, bridges, and buildings. In these cases, resonance can be beneficial, such as in musical instruments, or detrimental, such as in the Tacoma Narrows Bridge collapse in 1940.

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