Conservation of Energy and Non-Conservative Forces

In summary, the conversation discusses various concepts related to potential and kinetic energy, centripetal force, and the Law of Conservation of Energy. The main takeaway is that in a conservative field, potential energy is determined by location alone and external work is not a factor. The role of the new force in determining the total energy of an object is also discussed.
  • #1
Devilwhy
6
0

Homework Statement



o33557RWi163.png

Homework Equations

The Attempt at a Solution


4a at x=-2 F=0N
Potential energy=integration of F(-2)=Integration of 0=0 so it will reach minimum at x=-2?
b. integration of F(-2)-integration of F(-2-h)=m(v-0)^2/2
am i right?

5 Centripetal force=mv^2/r=mgsinθ-Fn(normal force)
will the block fall leave surface when Fn=0?

so i can represent the velocity as v=(mgrsinθ)^1/2=((m)(9.8)(15)sinθ)^1/2?
 
Physics news on Phys.org
  • #2
Force F is the gradient of the potential energy U.
A function has an extremum when its gradient is zero.
Therefore U has a minumum at some position where F=0

Integrate F(x) to get the PE function U(x), then put in x=-2 to find U(-2) ##\neq## 0

Also... what is U(x0 - h)?

How do changes in kinetic energy relate to changes in potential energy?
 
  • #3
Your attempt at the first question [4(a)] looks correct. As F=0 at x= (-2), it is the co-ordinate where U is minimum.

There are complications in 4(b) though. the work done by the new force cannot be determined from given data. It renders the Law of Conservation of Energy useless. How then do we proceed?

For 5, use the Law of Conservation of Energy. That should give you the required answer.
 
  • #4
There are complications in 4(b) though. the work done by the new force cannot be determined from given data.
I can do it from the data supplied, using conservation of energy.
Remember the relationship between kinetic and potential energy.
 
  • #5
The new force is not given to be conservative. Hence the work it does requires the path too, of which nothing is mentioned. Nor is the equation governing the magnitude.
 
  • #6
CrazyNinja said:
The new force is not given to be conservative. Hence the work it does requires the path too, of which nothing is mentioned. Nor is the equation governing the magnitude.
The new force is not acting when the object is released. The new force only served to move the block to its new location and plays no role in the work done by the conservative force when it is released from rest from that location.
 
  • Like
Likes Simon Bridge
  • #7
gneill said:
The new force is not acting when the object is released. The new force only served to move the block to its new location and plays no role in the work done by the conservative force when it is released from rest from that location.

What you have said is indeed correct. But in order to determine the initial "total" energy of the object, we require the work done by the new force. I am talking about the process in which the new force moves the particle form x0 to x0-h. KE is zero in both the cases. Initial PE is U(x0). Final PE is U(x0-h). In addition to this, there is additional work done by the new force. Thus, U(x0-h) = U(x0) + W

If this work done is known, then we know the total energy of the particle at x= x0-h. Only then can we proceed with its release and use this to calculate max KE which, interestingly, will be equal to the work done by the new force.
 
  • #8
CrazyNinja said:
What you have said is indeed correct. But in order to determine the initial "total" energy of the object, we require the work done by the new force. I am talking about the process in which the new force moves the particle form x0 to x0-h. KE is zero in both the cases. Initial PE is U(x0). Final PE is U(x0-h). In addition to this, there is additional work done by the new force. Thus, U(x0-h) = U(x0) + W
No. The history of the object is totally irrelevant. Additional work would show up as KE, but the object is at rest at the new location. Whatever work was done to move the object left no evidence of the process. In a conservative field PE is determined by location alone.


If this work done is known, then we know the total energy of the particle at x= x0-h. Only then can we proceed with its release and use this to calculate max KE which, interestingly, will be equal to the work done by the new force.
No, no, no. The only incarnations of energy in this system are KE expressed as motion and PE as a result of location in the field. Objects don't otherwise "remember" their history. Once an object is brought to rest there's no inherent evidence that the object experienced any particular process or path.
 
  • #9
gneill said:
No. The history of the object is totally irrelevant. Additional work would show up as KE, but the object is at rest at the new location. Whatever work was done to move the object left no evidence of the process. In a conservative field PE is determined by location alone.

And what you have said is again true, though in this case there are a few additional points. PE is determined by location alone in a conservative field, but external work is not. The Law of Conservation of Energy states- " E(final)= E(initial) + W(external)", where I have included PE in E() and W(external) implies work done by non-conservative forces, which I have excluded from my system. In this context, the object remains at rest because the external work done (by the new force) is equal in magnitude to the change in PE and opposite in sign, which is what U(x0-h)= U(x0) + W means.

gneill said:
No, no, no. The only incarnations of energy in this system are KE expressed as motion and PE as a result of location in the field. Objects don't otherwise "remember" their history. Once an object is brought to rest there's no inherent evidence that the object experienced any particular process or path.

I disagree with you. The work done by the new force will also manifest as a form of energy and will play a role in the "energy" equation.
 
  • #10
Okay. I just realized something.

I mentioned the answer in my own post and was arguing about it.

CrazyNinja said:
Thus, U(x0-h) = U(x0) + W

If this work done is known, then we know the total energy of the particle at x= x0-h. Only then can we proceed with its release and use this to calculate max KE which, interestingly, will be equal to the work done by the new force.

This basically implies that change in PE is the max KE. I am sorry for the inconvenience caused.

This brings a question to my head: Was I right all this while, or were you guys right all the time, or were both of us right and arguing for the same thing (which I don't know why happens a lot with physics -_- )??
 
  • #11
CrazyNinja said:
I disagree with you. The work done by the new force will also manifest as a form of energy and will play a role in the "energy" equation.
Does this energy show up as KE? Does it show up as PE? Something else? Will two objects brought to rest at the same location by different means or routes have different energies? What test could be performed on such objects to tell them apart?
 
  • #12
gneill said:
Does this energy show up as KE? Does it show up as PE? Something else? Will two objects brought to rest at the same location by different means or routes have different energies? What test could be performed on such objects to tell them apart?

I guess your post answers this the best. Which means I was wrong.
gneill said:
Additional work would show up as KE

I still do not understand where I went wrong though. The equations I wrote look consistent. In addition to that, they tell me that the new force is one with similar characteristics to the conservative force whose field we are working in.
 
  • #13
CrazyNinja said:
I guess your post answers this the best. Which means I was wrong.
No worries. What's important is that you're thinking about the physics and working your way to understanding. One aha! is worth a week of memorization :smile:
I still do not understand where I went wrong though. The equations I wrote look consistent. In addition to that, they tell me that the new force is one with similar characteristics to the conservative force whose field we are working in.
What you wrote said that the total work done to move an object from one location to another in a conservative field is equal to the change in PE between those locations. That's fine! In fact it's the definition of PE for a conservative field. Where things went awry was in deducing or perhaps implying that the method or route taken would leave an "imprint" on the result. It is a common misconception that crops up when conservative forces and fields are first introduced.
 
  • Like
Likes CrazyNinja
  • #14
The trick is to think about what sort of energy other than PE or KE could be involved ... how would that energy, under the condition of free motion in the PE field, affect the resulting kinetic energy? The extra W in your equation - by what mechanism would it turn into KE?

##U(x_0-h) + W = K_{max} + Q## ... by what mechanism would ##W \neq Q## that is consistent with the description and context?
(The object is held at rest and then released.)

In short - it is not so much that you were wrong exactly, but that you were over-thinking the problem.
Implicit in any physics problem is that the problem should be solvable, in a sensible way, by the average student having completed and understood the coursework ... physics problems never have all the information included explicitly or they would be very long-winded. Part of doing the problem is making a value judgement about what information is sensible to be included.. part of learning physics is learning to make that judgement.

In this case, unless the student has other information, we can consider that everything we need to know about the effect of the additional non-conservative force has been provided: that it's result is to place the object, initially stationary, other than at the PE=0 point.
Other possible effects depend on information not supplied and not relevant to the lesson - so: it's a red herring.
 

FAQ: Conservation of Energy and Non-Conservative Forces

What is conservation of energy?

Conservation of energy is a fundamental principle in physics that states that energy cannot be created or destroyed, it can only be transformed from one form to another. This means that the total amount of energy in a closed system remains constant over time.

Why is conservation of energy important?

Conservation of energy is important because it helps us understand and predict the behavior of physical systems. It allows us to calculate the amount of energy that will be present in a system at any given time and to determine how that energy will be distributed and transformed.

How does conservation of energy apply to real-life situations?

Conservation of energy applies to real-life situations in many ways. For example, when we turn on a light, electrical energy is converted into light energy. When we ride a bike, our muscles convert chemical energy into kinetic energy. In all of these cases, the total amount of energy remains the same.

Can energy be lost or wasted?

No, energy cannot be lost or wasted. It can only be converted into other forms of energy. However, some forms of energy are more useful to us than others. For example, when we drive a car, the chemical energy in the gasoline is mostly converted into heat, which is not very useful for moving the car forward. This is why cars are not very efficient.

Are there any exceptions to the conservation of energy?

No, there are no known exceptions to the conservation of energy. This principle has been extensively tested and has been found to hold true in all physical systems. However, in some situations, it may appear that energy is being lost, but in reality, it is just being converted into a form that is not easily measurable or useful.

Back
Top