Observer A & B's Views on Work Done to Book in Elevator

  • Thread starter Thread starter Arman777
  • Start date Start date
  • Tags Tags
    Work
AI Thread Summary
In the discussion about the work done on a book in an elevator, observer A inside the elevator perceives the total work done on the book as zero, as it remains still in their frame. In contrast, observer B on Earth sees the situation differently, leading to confusion about whether the work done is non-zero. The key point is that work is frame-dependent; while A sees no work done, B considers the forces acting on the book, including gravity and the normal force, which can yield a non-zero calculation depending on the perspective taken. The conversation highlights the importance of defining which forces are considered and how they relate to the work-energy theorem. Ultimately, both observers can arrive at different conclusions based on their frames of reference.
Arman777
Insights Author
Gold Member
Messages
2,163
Reaction score
191
Think, there's an elevator going upward with constant velocity.Theres two observers, one of them is in the elevator , the other one is on Earth observing the elevator.
The observer in the elevator A carries a book and holds it still.And B is outside

A will think that the total work done to the book is zero.

I am confused here about B.Does B also see the total net work done to the book is zero ?
 
Physics news on Phys.org
No. Work is frame variant, so it can be 0 in A's frame and nonzero in B's frame. This is not a relativistic effect, it is true in normal Newtonian physics.
 
Dale said:
No. Work is frame variant, so it can be 0 in A's frame and nonzero in B's frame. This is not a relativistic effect, it is true in normal Newtonian physics.

I know that work is frame variant.In this special case what will be the total work done for B ? If its nonzero how ?

Can someone help pls why its non-zero ??
 
Last edited:
Arman777 said:
I know that work is frame variant.In this special case what will be the total work done for B ? If its nonzero how ?

Can someone help pls why its non-zero ??
As I understand the question, you are asking about the total (by all forces) work done on the book according to observer B.
Dale has answered about the work (by the supporting force alone) done on the book according to observer B.

In this scenario and if we consider gravity as an external force, the total work done by all forces is zero for both observers. One can see this as an immediate consequence of the work-energy theorem. Both observers see the kinetic energy of the book to be unchanged. Accordingly, both observers must compute the total work done to be zero.
 
jbriggs444 said:
As I understand the question, you are asking about the total (by all forces) work done on the book according to observer B.
Dale has answered about the work (by the supporting force alone) done on the book according to observer B.

In this scenario and if we consider gravity as an external force, the total work done by all forces is zero for both observers. One can see this as an immediate consequence of the work-energy theorem. Both observers see the kinetic energy of the book to be unchanged. Accordingly, both observers must compute the total work done to be zero.

Thanks for confirming.My Professor said that's its non-zero.Thats why I am confused
 
Arman777 said:
Thanks for confirming.My Professor said that's its non-zero.Thats why I am confused
If one regards gravity as a potential field (putting it over on the energy side of the work-energy relation) and not as an external force (which would put it over on the work side) then the professor's answer becomes correct.

According to B, the total mechanical energy of the system has increased and positive work has been done by the single external force.

According to A, the total mechanical energy of the system has remained unchanged and no work has been done by the single external force.

Edit: First draft of this had reversed A and B. I think I have it right now.
 
I don't still know the exteral force idea
 
jbriggs444 said:
According to B, the total mechanical energy of the system has increased and positive work has been done by the single external force.

.

ohh you are talking about mgh...no I don't think he included that
 
Arman777 said:
I know that work is frame variant.In this special case what will be the total work done for B ? If its nonzero how ?

Can someone help pls why its non-zero ??
The work is ##f\cdot d##. The force is the same in both frames but d is 0 for A and non zero for B. So the work is 0 for A and non zero for B. Both use the same law, ## f \cdot d## , to determine the answer, even though the answers are different.
 
  • #10
For B F total is zero ?
 
  • #11
Arman777 said:
For B F total is zero ?
If you count gravity as one of the forces acting on the book, yes. If not, no.
 
  • #12
A holds a book in hand there's gravity acting on it and there's normal force.They cancel out.And for B the book velocity didnt changed.Cause the elevator goes with constant velocity.
 
  • #13
Arman777 said:
A holds a book in hand there's gravity acting on it and there's normal force.They cancel out.And for B the book velocity didnt changed.Cause the elevator goes with constant velocity.

Calculate the work done by both forces individually on the book from each observer's perspective. Assume that the elevator travels at a constant velocity for 10 meters.
 
  • #14
Drakkith said:
Calculate the work done by both forces individually on the book from each observer's perspective. Assume that the elevator travels at a constant velocity for 10 meters.

For A its obvious zero.For B there's no other force then G and N.This is not homework question..
 
  • #15
So your description of the problem is slightly ambiguous. The general principle is that ##W=f\cdot d##. You may be interested in the work done only by the force holding the book (my response), or you may be interested in the work done by the force holding the book plus the force of gravity, which is also called the net force (@jbriggs444 responses).

You can apply the work formula for any single force to get the work done by that single force, or you can apply it for the net force to get the net work.

Your professor seems to be taking my approach and talking about just the force holding the book.
 
  • Like
Likes jbriggs444
  • #16
Dale said:
So your description of the problem is slightly ambiguous. The general principle is that ##W=f\cdot d##. You may be interested in the work done only by the force holding the book (my response), or you may be interested in the work done by the force holding the book plus the force of gravity, which is also called the net force (@jbriggs444 responses).

You can apply the work formula for any single force to get the work done by that single force, or you can apply it for the net force to get the net work.

Your professor seems to be taking my approach and talking about just the force holding the book.

I see there's also gravity acts to the book
 
  • #17
Actually he added gravity.I ll send the link of the lecture
 
  • #18
Arman777 said:
I see there's also gravity acts to the book
So the reason that your professor is confusing you is that you may be thinking about the net work and he is talking about the normal force work only.
 
  • #19


14:20
 
  • #20
Arman777 said:
For A its obvious zero.For B there's no other force then G and N.This is not homework question..

Perhaps, but it is often helpful to do a quick calculation. If you calculate the work done by each force from B's perspective, would that not answer your question about what observer B sees?
 

Similar threads

Back
Top