Changing the mass of a simple harmonic oscillator

In summary, I find the homework statement difficult to understand because first of all when adding more mass, wouldn't that change the acceleration, according to F=ma? And in that case the velocity should also change when adding more mass, shouldn't it? That would then also change the amplitude and angular frequency. I don't understand how to think about the physical concepts in this example.
  • #1
Maxo
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1

Homework Statement


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Homework Equations



The Attempt at a Solution


I find this task very hard to understand. First of all, when adding more mass, wouldn't that change the acceleration, according to F=ma? And in that case the velocity should also change when adding more mass, shouldn't it? That would then also change the amplitude and angular frequency. When I think of it intuitively, I think that adding more mass will increase the inertia, and hence make the amplitude less and also the frequency. Why is this wrong?

I don't understand how to think about the physical concepts in this example. If you understand it, please explain how you reason about it!
 
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  • #2
When the second box is "attached to" the first box, you can think of it as a "collision" between the masses. Can you think of a physical quantity that is conserved during the "collision"?
 
  • #3
Hm first of all I don't see what makes the second box stick together with the first box, but maybe that doesn't matter. So let's think of it as a collision. Is it then correct to see this situation as equivalent to the second box was put in front of the first box, and then the first box collides with the second box and "drags with" the second box? In that case we have a completely inelastic collision, and kinetic energy is preserved.

KEf = KE0, that is

m1*vf1^2 + m2*vf2^2 = m1*v01^2 + m2*v02^2

The initial velocity of the mass on the spring (m1) is vmax and for the mass being attached (m2) is 0, and after the collision the two masses will have the same velocity. So we can simplify to:

(m1+m2)*vf^2 = m1*vmax^2

m1=m2=m so we get 2*m*vf^2 = m*vmax^2 <=> 2*vf^2 = vmax^2 <=> vf = √2*vmax.

This is unfortunately not correct. What is wrong in my reasoning?
 
  • #4
Maxo said:
In that case we have a completely inelastic collision, ..

Yes, good. You can think of it as a completely inelastic collision.

and kinetic energy is preserved.

What is meant by the term inelastic? Is KE conserved in such a collision? If not, what is conserved?
 
  • #5
In any collision, nothing but the total energy and linear momentum is conserved. Check your calculations accordingly.
Mass doubles, Energy is conserved, Find out what decreases and what increases from
F=ma. or F=m.(Second derivative of position wrt time)... you have the additional relations to assist you, which are
F=-kx and a=-(w^2).x and w(angular freq)=root(k/m) if you require them. :) all this keeping in mind the relationship between force and work(Total Energy) in a conservative process... I'm sure you can solve this problem, this isn't the toughest.. :)
 
  • #6
SohamSen said:
In any collision, nothing but the total energy and linear momentum is conserved.

Hello, SohamSen. Welcome to PF!

You are right that total energy is conserved. But total energy includes all forms of energy, such as "heat" stored internally within the objects. Maxo will need to decide if KE alone is conserved in this type of collision.
 
  • #7
TSny said:
What is meant by the term inelastic? Is KE conserved in such a collision? If not, what is conserved?
Right. The linear momentum is conserved. The equations that I did for KE will almost be the same for linear momentum:

pf = p0

m1*vf + m2*vf2 = m1*v01 + m2*v02

The initial velocity of the mass on the spring (m1) is vmax and for the mass being attached (m2) is 0, and after the collision the two masses will have the same velocity. So we can simplify to:

(m1+m2)*vf = m1*vmax

m1=m2=m so we get 2*m*vf = m*vmax <=> 2*vf = vmax <=> vf = 1/2*vmax.

But it's still not correct.

I also still don't know what makes the second box stick to the first one? Maybe that doesn't matter, but why not? I also wonder, if we see this as an inelastic collision, is it then correct to see this situation as equivalent to a situation where the second box was put in front of the first box, and then the first box collides with the second box and "drags with" the second box? Please help to clarify so I can understand this.
 
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  • #8
Maxo said:
Right. The linear momentum is conserved. The equations that I did for KE will almost be the same for linear momentum:

pf = p0

m1*vf + m2*vf2 = m1*v01 + m2*v02

The initial velocity of the mass on the spring (m1) is vmax and for the mass being attached (m2) is 0, and after the collision the two masses will have the same velocity. So we can simplify to:

(m1+m2)*vf = m1*vmax

m1=m2=m so we get 2*m*vf = m*vmax <=> 2*vf = vmax <=> vf = 1/2*vmax.

But it's still not correct.

That all looks right to me. The wording of part (a) is a little vague. They ask "what happens" to vmax. I think you are right that it is reduced by a factor of 1/2. How do you know it's not the right answer?

I also still don't know what makes the second box stick to the first one? Maybe that doesn't matter, but why not?

Unfortunately, the problem statement is not very clear on the meaning of "attached to". But I don't see any other way to interpret the problem except to assume that it's equivalent to a totally inelastic collision.

I also wonder, if we see this as an inelastic collision, is it then correct to see this situation as equivalent to a situation where the second box was put in front of the first box, and then the first box collides with the second box and "drags with" the second box? Please help to clarify so I can understand this.

Yes, that's right.
 
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  • #9
TSny said:
That all looks right to me. The wording of part (a) is a little vague. They ask "what happens" to vmax. I think you are right that it is reduced by a factor of 1/2. How do you know it's not the right answer?
In my book the answer is given as that the speed remains the same. It seems they assume that the second box attached will already have an initial speed equal to the first box. But it's not said clear in the task. I'm glad I'm not the only one who interpreted it this way anyway. :)

What about the other questions, b) and c)? In b) they ask if the amplitude changes. I find this quite hard to solve also. I know the force of the spring relates to the amplitude like F=-k*A. Does this help finding out how the amplitude will change? How can we find that out?
 
  • #10
Maxo said:
In my book the answer is given as that the speed remains the same. It seems they assume that the second box attached will already have an initial speed equal to the first box. But it's not said clear in the task. I'm glad I'm not the only one who interpreted it this way anyway. :)

OK. With that interpretation, then the diagram in the text makes more sense to me now. Sorry for misleading you.

What about the other questions, b) and c)? In b) they ask if the amplitude changes. I find this quite hard to solve also. I know the force of the spring relates to the amplitude like F=-k*A. Does this help finding out how the amplitude will change? How can we find that out?

You might want to consider energy here. Can you describe what type of energy the system has at x = 0? At x = Anew? Are these two energies related? Can you use this to relate Anew to vmax? How is Aold related to vmax?
 
  • #11
TSny said:
You might want to consider energy here. Can you describe what type of energy the system has at x = 0? At x = Anew? Are these two energies related? Can you use this to relate Anew to vmax? How is Aold related to vmax?

At x=0 the system has kinetic energy only. At Anew it is potential elastic energy. Yes they are related somehow. I know they can't both be max at the same time. So when PE=max KE=0 and vice versa. I also know that if there is no non conservative forces doing work, then KEf+PEf = KE0 + PE0. Here PE0=0 and KEf=0, so we get PEf = KE0 or

1/2*k*A^2 = 1/2*m*vmax^2

Am I on the right track? How can we continue from here?
 
  • #12
Maxo said:
I also know that if there is no non conservative forces doing work, then KEf+PEf = KE0 + PE0. Here PE0=0 and KEf=0, so we get PEf = KE0 or

1/2*k*A^2 = 1/2*m*vmax^2

Am I on the right track?

Yes, you're on the right track!

But, be careful with the interpretation of the mass m. Apply this equation to two cases: (i) before the second mass is added (ii) after the second mass is added.
 
  • #13
TSny said:
Yes, you're on the right track!

But, be careful with the interpretation of the mass m. Apply this equation to two cases: (i) before the second mass is added (ii) after the second mass is added.

Ah, I see now. Anew = √2*Aold. Great.

Now I have another question, which I would also very much like explained. What would happen (concerning maximum speed, amplitude and angular frequency) if the second box was attached at the one extreme end of the oscillation cycle?

I don't see how that would be different from when the second box is attached in the middle position, but apparently it is different. Can someone please explain why it is different?
 
  • #14
If you add the second mass to the first mass when x = A, have you added any energy to the system?

What about when you add the second mass at x = 0?
 
  • #15
TSny said:
If you add the second mass to the first mass when x = A, have you added any energy to the system?
Well, the mass is increased but since the velocity at this point is 0 I guess there can't be any kinetic energy involved? Also the linear momentum must be zero for the same reason. And the elastic potential energy is unchanged since there is no displacement of the spring when the second box is added.

Can this really be correct? According to my book the maximum velocity is actually decreased when the second box is added at one extreme end. But I don't understand why? How can we get to this conclusion?

TSny said:
What about when you add the second mass at x = 0?
Then kinetic energy is added (like in the previous task).
 
  • #16
Maxo said:
Well, the mass is increased but since the velocity at this point is 0 I guess there can't be any kinetic energy involved? Also the linear momentum must be zero for the same reason. And the elastic potential energy is unchanged since there is no displacement of the spring when the second box is added.

Can this really be correct?

Yes, that's right. Adding the second mass to the first mass at x = A does not change the energy of the system.

According to my book the maximum velocity is actually decreased when the second box is added at one extreme end. But I don't understand why? How can we get to this conclusion?

The energy of the system does not change when adding the second box at x = A.
What does that tell you about the KE at x = 0? Is the total KE at x = 0 for the two boxes the same as it was for the one box at x = 0?

Think about how the mass of the system affects the relationship between KE and speed.
 
  • #17
TSny said:
Yes, that's right. Adding the second mass to the first mass at x = A does not change the energy of the system.

The energy of the system does not change when adding the second box at x = A.
What does that tell you about the KE at x = 0? Is the total KE at x = 0 for the two boxes the same as it was for the one box at x = 0?

Think about how the mass of the system affects the relationship between KE and speed.

I think I understand. The only thing that matters it what happens to the total energy (TE) at the instant of changing some variable (in this case doubling mass when v=0). In this case the TE is unchanged because the box being added has no energy to add to the system. And since the TE is unchanged at this point, it's also unchanged at the point x=0, even though the KE is larger at x=0 compared to at x=A. Is that correct? But how does that go together with the fact that this is again equivalent to a inellastic collision, which by definition means KE is NOT preserved?

I'm then wondering what happens to the PE(elastic), which leads us to the second question, which is what happens to the amplitude. In the first task the doubling of maximum KE also meant doubling of maximum PE. In this case the KE is unchanged, so the same reasoning should mean that PE must here also be unchanged. PE relates to the amplitude as PE=1/2*k*A^2. So if PE is the same, and k is the same, then A must also be the same? Again this is incorrect though. How can we solve this?
 
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  • #18
Maxo said:
I think I understand. The only thing that matters it what happens to the total energy (TE) at the instant of changing some variable (in this case doubling mass when v=0). In this case the TE is unchanged because the box being added has no energy to add to the system. And since the TE is unchanged at this point, it's also unchanged at the point x=0, even though the KE is larger at x=0 compared to at x=A. Is that correct?

Yes, that is correct.

But how does that go together with the fact that this is again equivalent to a inellastic collision, which by definition means KE is NOT preserved?

There is no collision. When the second box is added to the first box at x = A, both boxes are at rest. There is no loss of KE. Both boxes have zero KE just before they are attached and also zero KE just after they are attached. The energy of the simple harmonic motion does not change when the second box is added.

In the first case where the second box was added at x = 0, there was also no collision. The second box had the same speed as the first box when the second box was added. Nevertheless, in this case energy was added to the simple harmonic motion because the second mass already had KE when it was added to the simple harmonic motion.

I'm then wondering what happens to the PE(elastic), which leads us to the second question, which is what happens to the amplitude. In the first task the doubling of maximum KE also meant doubling of maximum PE. In this case the KE is unchanged, so the same reasoning should mean that PE must here also be unchanged. PE relates to the amplitude as PE=1/2*k*A^2. So if PE is the same, and k is the same, then A must also be the same? Again this is incorrect though. How can we solve this?

I agree with you that for the case where the second box is added to the first box at x = A, the amplitude should not change. As you say, there is no change in total energy in this case. So the PE at x = A doesn’t change. Therefore the amplitude doesn’t change. I don’t understand why this isn’t the correct answer.

[In the first case where the second box was added at x = 0, there is a change in amplitude.]
 
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  • #19
TSny said:
I agree with you that for the case where the second box is added to the first box at x = A, the amplitude should not change. As you say, there is no change in total energy in this case. So the PE at x = A doesn’t change. Therefore the amplitude doesn’t change. I don’t understand why this isn’t the correct answer.

Sorry I made a misstake, it actually does say the amplitude doesn't change. I mixed it up, it's the angular frequency that changes.

I think I understand everything now. For some reason this physical example was one of the most unintuitive I've encountered in all of mechanics. But now it makes much more sense. Thanks TSny for clarifying so much, you've been very helpful. :)
 

FAQ: Changing the mass of a simple harmonic oscillator

1. How does changing the mass affect the period of a simple harmonic oscillator?

Changing the mass of a simple harmonic oscillator does not affect its period. The period of a simple harmonic oscillator is solely determined by the stiffness of the spring and the mass does not have any influence on it.

2. Does changing the mass of a simple harmonic oscillator affect its amplitude?

Yes, changing the mass of a simple harmonic oscillator will affect its amplitude. As the mass increases, the amplitude of the oscillator will decrease, and vice versa. This is because the mass affects the restoring force of the oscillator.

3. How does changing the mass affect the energy of a simple harmonic oscillator?

Changing the mass of a simple harmonic oscillator does not affect its energy. The energy of a simple harmonic oscillator is determined by its amplitude and does not depend on the mass.

4. Does changing the mass of a simple harmonic oscillator affect its frequency?

Yes, changing the mass of a simple harmonic oscillator will affect its frequency. As the mass increases, the frequency of the oscillator will decrease, and vice versa. This is because the mass affects the stiffness of the spring and thus the frequency of the oscillator.

5. Can changing the mass of a simple harmonic oscillator cause it to stop oscillating?

No, changing the mass of a simple harmonic oscillator will not cause it to stop oscillating. As long as there is a restoring force acting on the oscillator, it will continue to oscillate. However, changing the mass may affect the amplitude and frequency of the oscillations.

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