Conservation of Energy Tutor | Physics Problem | x162,x163

In summary, the conversation discusses a problem in a high school physics textbook where the conservation of mechanical energy is applied to a spring-mass system. The solution provided in the textbook is questioned by the participants, who believe that the spring constant may be incorrect. It is also noted that the problem is not a conservation problem, but rather aims to teach students how to calculate elastic potential energy. The participants also discuss the effects of dissipative forces and the theoretical behavior of the system if no friction is present.
  • #1
ham
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I am a tutor. I ran across this problem is a high school physics textbook. See attachment x162, my solution is on x163. I thought that mechancical energy is conserved and that loss of potential energy should be equal to gain in elastic (stored) energy. Ithink the spring constant must be wrong?
 

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  • #2
Note the phrase "allowed to come to rest". If the weight were just dropped, there would be both spring PE and kinetic energy. That extra kinetic has been dissipated somehow. (The mass may have been lowered gently to the equilibrium position, or just allowed to oscillate until the kinetic energy was "lost" to internal friction or air resistance.)
 
  • #3
I think that although not specifically said, there is no wind or other resistance here. If the mass were dropped, it would oscillate as the potential energy in the spring would be transferred between kinetic energy and gravitational potential energy. At rest, there would be no kinetic energy so I would think all of the PE would be transwferred to stored elastic energy. I still think the book answer is wrong.
 
  • #4
This problem is not a conservation problem. It is just trying to teach the student how to calculate the elastic potential energy.
 
  • #5
Dale, Regardless of the objective of the problem, I think there is an error here. Please check my calculations and tell me whee I am wrong.
 
  • #6
my bet is that the problem wants you to apply the following equation:

[tex]U= \frac{1}{2}kx^{2}[/tex]

since Force is related to Potential Energy by the following relation

[tex] F= -\frac{dU}{dx} [/tex]

and the force of a spring is [tex]F= -kx[/tex]

the negative integral with respect to x would give

[tex]U= \frac{1}{2}kx^{2}[/tex]

and x is the change from the relaxed point with 0 mass(really just the spring mass)
 
  • #7
Smash, I agree that that equation e = (1/2) kd^2 should be used. This is not the issue. I think the k value, or something else, is wrong in order to conserv energy.
 
  • #8
ham said:
Dale, Regardless of the objective of the problem, I think there is an error here. Please check my calculations and tell me whee I am wrong.
You just didn't need to calculate the mass of the weight nor the change in gravitational potential energy. Your calculations for the elastic potential energy are correct.

ham said:
I think the k value, or something else, is wrong in order to conserv energy.
The k value is fine. This is not an energy conservation problem.
 
  • #9
ham said:
I think that although not specifically said, there is no wind or other resistance here. If the mass were dropped, it would oscillate as the potential energy in the spring would be transferred between kinetic energy and gravitational potential energy. At rest, there would be no kinetic energy so I would think all of the PE would be transwferred to stored elastic energy. I still think the book answer is wrong.
If dropped without any dissipative forces, it would oscillate. It would not come to rest at the equilibrium position, but (momentarily) at the bottom of the oscillation. The book's answer is correct, given the stipulation "allowed to come to rest". That stipulation implies that all kinetic energy has been dissipated. (Otherwise it just bounces up and down, with maximum kinetic energy at the equilibrium position.)

Mechanical energy of the spring-mass system is not conserved here.
 
  • #10
my mistake i failed to see what you were really asking here.

Doc Al got it though. Spring systems that come to rest are nonconservative. that is where your loss in energy is
 
  • #11
Wow, pretty impressive. Three replies in the same minute! My kids would say "Jinks, you owe me a coke"
 
  • #12
Doc Al. Theoritically, energy in a sping is stored and not used, like energy in a capacitor and inductor. If the mass was dropped, it should oscillate indifinately. Let's asume we don't drop the mass but lower it slowly. The change in PE would be 6.52, and the stored energy, per calculation would be 3.26. Where did the PE go? I agree that at the equiliberium point of the spring, the KE would me at max. If we plotted the energy and displacements of this problem, we would have a sinusoid going forever (with no friction) ?

Agree?
 
  • #13
ham said:
Theoritically, energy in a sping is stored and not used
But the problem specifies that the energy is taken out of the system (used) by the satement "allowed to come to rest".
 
  • #14
ham said:
Doc Al. Theoritically, energy in a sping is stored and not used, like energy in a capacitor and inductor. If the mass was dropped, it should oscillate indifinately.
Right.
Lets asume we don't drop the mass but lower it slowly. The change in PE would be 6.52, and the stored energy, per calculation would be 3.26. Where did the PE go?
The energy was dissipated in whatever mechanism lowered the mass. If you lower it with your hand, your internal energy will increase as you absorb that energy. (Think about walking downstairs. You start at rest at the top of the steps and end up at rest at the bottom. Where does the energy go?)
I agree that at the equiliberium point of the spring, the KE would me at max. If we plotted the energy and displacements of this problem, we would have a sinusoid going forever (with no friction) ?
Sure.
 
  • #15
Dale, I see your point. However, given that this is a high school physics problem, I don't think the intent of the problem was to consider damping where I would agree some energy would go into the damping medium such as air friction. If we asume there is no friction, and we lowered the mass gradually so it would not oscillate but rather hang there, would you agree that there is a problem?

I have to leave for 1 hour and will return. I hope you guys will still be online.
 
  • #16
DaleSpam said:
But the problem specifies that the energy is taken out of the system (used) by the satement "allowed to come to rest".

after thinking for a minute, I came to an answer, but Dale beat me to it.

Lets think about it:

Originally, spring is at equilibrium. When you add the mass, the spring oscillates, the height changes. This change in gravitational energy is split up; half goes into Kinetic Energy, half goes to Elastic Energy in the spring. If you let the spring come to rest, the only way to do this is to take energy OUT of the system. The only energy you can take out here is the kinetic. So that's what happens to the energy you're missing
 
  • #17
ham said:
If we asume there is no friction, and we lowered the mass gradually so it would not oscillate but rather hang there, would you agree that there is a problem?
No, there's no problem (as I have attempted to explain).

To "answer the question" all one need do is plug into the formula for spring PE. But I applaud your efforts to understand why this doesn't fit with your assumption that mechanical energy is conserved. (The answer is that mechanical energy is not conserved. There are additional dissipative forces at work.)
 
  • #18
ham said:
Dale, I see your point. However, given that this is a high school physics problem, I don't think the intent of the problem was to consider damping where I would agree some energy would go into the damping medium such as air friction. If we asume there is no friction, and we lowered the mass gradually so it would not oscillate but rather hang there, would you agree that there is a problem?

I have to leave for 1 hour and will return. I hope you guys will still be online.

when you lower the mass gradually, what you are doing is applying an upward force so that the acceleration of the mass is very small, so that at the bottom there is no motion. Therefore, you are applying a force, over a distance, which is Work. Work= change in Kinetic Energy. Normally the Kinetic energy, if you allow the spring to oscillate, would be the same 3.26 value at the bottom point of oscillation. Therefore, for there to be no kinetic energy, you have to apply an equal amount of work to the system, which takes the energy out.

Efinal= Einitial - Work
 
  • #19
If you compare the spring and weight, to the bounce of a basket ball, you have the same manor of energy dissipation, however the spring allows a smooth change of direction and a much longer oscillation period.
 
  • #20
ham said:
However, given that this is a high school physics problem, I don't think the intent of the problem was to consider damping where I would agree some energy would go into the damping medium such as air friction. If we asume there is no friction, and we lowered the mass gradually so it would not oscillate but rather hang there, would you agree that there is a problem?
Just go to your answer, use the first and the fourth line, delete the second and third lines. That is all that this question is asking. It is definitely a high-school level problem.

It does not matter how it comes to rest at the stretched length, whether it is through friction or gradually lowering the mass. All that the question is asking for is what is the elastic potential energy at that stretched length. It is completely independent of any specific mechanism for removing the energy.

The "allowed to come to rest" specifies that energy is removed but does not give details of how it is removed since the details are irrelevant for the problem. You can prescribe many different mechanisms for removing the energy, all will result in the conservation of energy (i.e. the work done on the mechanism will exactly equal the change in PE) but none are relevant for the problem since it is not a conservation problem.
 
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  • #21
I am now convinced I am wrong. However, I must go and work a few more problems like this to totally understand what is going on.

Thanks to all of you.

Ham
 

FAQ: Conservation of Energy Tutor | Physics Problem | x162,x163

What is conservation of energy?

The conservation of energy is a fundamental principle in physics that states that energy cannot be created or destroyed, but can only be transformed from one form to another.

How is the conservation of energy applied in real-life situations?

The conservation of energy is applicable in various real-life situations, such as the operation of machines, the movement of objects, and the generation of electricity. It is also a crucial concept in understanding natural phenomena, such as the motion of planets, the flow of water, and the behavior of living organisms.

What is the role of the conservation of energy in solving physics problems?

The conservation of energy is a fundamental principle that is used in solving many physics problems. It allows us to analyze and understand the behavior of objects and systems without having to consider every individual force acting on them. By applying this principle, we can predict the outcome of various physical processes and phenomena.

What are some common examples of the conservation of energy in action?

Some common examples of the conservation of energy include a pendulum swinging back and forth, a roller coaster moving along its track, a car accelerating from rest, and a light bulb producing light. In all of these examples, the total amount of energy remains constant, but it is constantly being transformed from one form to another.

Is the conservation of energy always true?

Yes, the conservation of energy is a universal principle that applies to all physical systems. However, it is important to note that this principle is only valid in isolated systems, where no external forces are acting on the system. In real-life situations, energy can be lost due to various factors such as friction or air resistance, but the total amount of energy in the universe always remains constant.

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