Transverse Oscillation of horizontal Mass-Springs system

In summary: Thank you both for your help, in combination I believe I understand this much better now but I'll continue to ponder this idea of approximations (in terms of power series) over. Much appreciated!
  • #1
omegasquared
13
0

Homework Statement



Mass M is supported by a smooth table and connected by two light horizontal springs to two fixed blocks. Each spring is of natural length L. Both springs are initially extended by L to get a total width between blocks of 4L. The spring constant of both springs is k.

When the mass is given a small transverse displacement, y, show that the restoring force is approximately ky.

See photo below:

Photo on 11-11-2015 at 15.54.jpg


Homework Equations



F = kx
sinθ = o/h[/B]

The Attempt at a Solution



Restoring force, Fr = 2kxsinθ
sinθ = y / (2L + x)
x = (y / sinθ) - 2L
 
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  • #2
First you should draw a diagram showing a small transverse displacement y of the ball, and draw a coordinate system. Then write your equations. For example, I don't understand why there is an x in your equations at all.
 
  • #3
Chandra Prayaga said:
First you should draw a diagram showing a small transverse displacement y of the ball, and draw a coordinate system. Then write your equations. For example, I don't understand why there is an x in your equations at all.

The x is to do with the extension of the spring which will occur when you displace the ball by y upwards.
 
  • #4
omegasquared said:
Restoring force, Fr = 2kxsinθ
sinθ = y / (2L + x)
Are you being consistent about the meaning of x? Is it the total extension of the spring, or the additional extension beyond its extension when y=0?
 
  • #5
haruspex said:
Are you being consistent about the meaning of x? Is it the total extension of the spring, or the additional extension beyond its extension when y=0?

Additional extension beyond what it was (L) at y=0.
 
  • #6
omegasquared said:
Additional extension beyond what it was (L) at y=0.
Then reconsider your equation for Fr.
 
  • #7
haruspex said:
Then reconsider your equation for Fr.

Ah, good point.

So it should be: Fr = 2k(L+x)sinθ

Which would then be: = 2ky(L+x) / (2L+x)

Agreed?
 
  • #8
omegasquared said:
Ah, good point.

So it should be: Fr = 2k(L+x)sinθ

Which would then be: = 2ky(L+x) / (2L+x)

Agreed?
Yes.
 
  • #9
haruspex said:
Yes.

I'm still unsure how to get from there to simply ky however.
 
  • #10
omegasquared said:
I'm still unsure how to get from there to simply ky however.
It says small displacements. If y is small, x is very small. What approximations does that allow you to make?
 
  • #11
haruspex said:
It says small displacements. If y is small, x is very small. What approximations does that allow you to make?

Expanding previously, Fr = (2kL+2kx)y / (2L+x), so if x is small then 2kx ≈ 0 and 2L + x ≈ 2L? Which would leave 2kLy/2L = ky but then surely the y on the top would make the whole thing ≈ 0?
 
  • #12
omegasquared said:
Expanding previously, Fr = (2kL+2kx)y / (2L+x), so if x is small then 2kx ≈ 0 and 2L + x ≈ 2L? Which would leave 2kLy/2L = ky but then surely the y on the top would make the whole thing ≈ 0?
What we're doing here is finding the first order approximation. You can think of it as writing the full form as the sum of a series of terms in which, as the displacement tends to zero, each term tends to zero faster than the one before it: a power series, say. The first order approximation throws away all except the first term.
 
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  • #13
Well, certainly, if you put y = 0, then you don't have to do anything. There are no oscillations! You are making an approximation, where y, and x are small compared to L. So expressions like L + x, where L is large, and x is small, are nearly equal to L. e.g., 1000 + 1 ~ 1000. If you look at the y on top, you cannot neglect it because you don't have anything to compare it with. After all, while 1 << 1000, 1 is not small compared to 0.
 
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  • #14
haruspex said:
What we're doing here is finding the first order approximation. You can think of it as writing the full form as the sum of a series of terms in which, as the displacement tends to zero, each term tends to zero faster than the one before it: a power series, say. The first order approximation throws away all except the first term.

Chandra Prayaga said:
Well, certainly, if you put y = 0, then you don't have to do anything. There are no oscillations! You are making an approximation, where y, and x are small compared to L. So expressions like L + x, where L is large, and x is small, are nearly equal to L. e.g., 1000 + 1 ~ 1000. If you look at the y on top, you cannot neglect it because you don't have anything to compare it with. After all, while 1 << 1000, 1 is not small compared to 0.

Thank you both for your help, in combination I believe I understand this much better now but I'll continue to ponder this idea of approximations (in terms of power series) over. Much appreciated!
 

FAQ: Transverse Oscillation of horizontal Mass-Springs system

1. What is a transverse oscillation in a horizontal mass-spring system?

A transverse oscillation refers to the movement of a mass-spring system in a direction perpendicular to the direction of the applied force. In a horizontal mass-spring system, this would be side-to-side movement as opposed to up-and-down movement.

2. How does a horizontal mass-spring system oscillate?

A horizontal mass-spring system oscillates due to the interplay of two main forces: the force of gravity and the spring force. When the system is displaced from its equilibrium position, the spring force pulls it back towards equilibrium, but the force of gravity causes the system to overshoot and thus oscillate back and forth.

3. What factors affect the frequency of transverse oscillations in a horizontal mass-spring system?

The frequency of transverse oscillations in a horizontal mass-spring system is affected by the mass of the object, the stiffness of the spring, and the force of gravity. The larger the mass or the stiffer the spring, the lower the frequency will be. Similarly, a stronger force of gravity will result in a lower frequency.

4. How does damping impact transverse oscillations in a horizontal mass-spring system?

Damping is the resistance to motion in a system, and it can impact the amplitude and frequency of transverse oscillations in a horizontal mass-spring system. Damping can decrease the amplitude of oscillations over time, resulting in a smaller range of motion. It can also change the frequency of oscillations, making them slower and more regular.

5. How is the behavior of a horizontal mass-spring system affected by different initial conditions?

The behavior of a horizontal mass-spring system is highly dependent on its initial conditions, such as the initial displacement and velocity. These initial conditions determine the amplitude, frequency, and overall movement of the system. Changing the initial conditions can result in different patterns of oscillation or even different types of motion, such as chaotic or periodic behavior.

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