Mass of Backpack in Moving Elevator

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Discussion Overview

The discussion centers around the dynamics of a backpack attached to a spring scale in a downward-accelerating elevator. Participants explore the relationship between the forces acting on the backpack, the reading of the spring scale, and the implications of the elevator's acceleration on these forces.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions the interpretation of the spring scale reading, suggesting it should represent the net force due to the downward acceleration of the elevator.
  • Another participant argues that the spring scale reading is determined by the elastic force of the spring and is independent of gravitational effects, citing that in free fall, the scale would read zero.
  • A different viewpoint proposes a relationship involving the force of the scale in a non-moving elevator and the acceleration of the elevator, seeking clarification on its correctness.
  • Several participants emphasize the distinction between the forces acting on the backpack: the upward force from the spring scale and the downward gravitational force, asserting that the scale measures the force exerted by the rope rather than the net force.
  • One participant discusses the implications of removing the scale, suggesting that the backpack would free fall under gravity, leading to confusion about the forces in play when the elevator is accelerating downwards.
  • Another participant raises a question about the frame of reference in the elevator, pondering whether the forces balance out in that context.
  • There is a contention regarding the definition of net force, with some participants asserting that the term is being used incorrectly in the context of the discussion.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the interpretation of forces acting on the backpack and the reading of the spring scale. The discussion remains unresolved, with no consensus reached on the correct interpretation of the forces involved.

Contextual Notes

Limitations include potential misunderstandings of the definitions of forces and net force, as well as the implications of different frames of reference in the context of the elevator's motion.

annamal
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A backpack is attached to a spring scale which is attached to the ceiling of an elevator. The elevator is moving downwards with an acceleration of 3.8 m/s^2. The scale reads 60 N (Fscale). What is the mass of the backpack?
The solution to this problem says that Fscale - w (weight) = Fnet.
This confuses me because the elevator is causing a downward acceleration and so the spring scale reading should be the Fnet since it is the result of all the forces in play.
I think the answer should be Fscale (also known as Fnet now) = Fup (an upwards force on the spring produced by the moving elevator and the spring itself) - w (weight). Can someone explain how I am wrong?
 
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The spring sclae reding depends on the extension of the spring which is related to the elastic force. It has nothing to do with gravity or any other force. If the elevator is in free fall the scale will read zero even though the net force on the body is mg.
 
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I am thinking
Forig (force of scale with non moving elevator) + m*a (accceleration of elevator) = Fs ( resulting force of scale)

How is that wrong?
 
Think of the backpack hanging from a rope attached to the ceiling. Two forces are exerted on the backpack. There's the upward force exerted by the rope and the downward force exerted by gravity. The net force is the vector sum of these two forces.

In your scenario the scale reads the force exerted on the backpack by the rope. It does not read the net force.
 
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Mister T said:
Think of the backpack hanging from a rope attached to the ceiling. Two forces are exerted on the backpack. There's the upward force exerted by the rope and the downward force exerted by gravity. The net force is the vector sum of these two forces.

In your scenario the scale reads the force exerted on the backpack by the rope. It does not read the net force.
Yes, but doesn't Forig (force of scale with non moving elevator) + m*a (accceleration of elevator) = Fs ( resulting force of scale) --> that's what I mean by net force for Fs
 
annamal said:
... Can someone explain how I am wrong?
With the elevator fully stopped or moving at constant velocity, what would happen if you removed the scale (or Fs, or Fup or Fnet (the way you have re-define it)?
The only force acting on the backpack would be the weight (mg).
Then, the backpack would free fall at 9.81 m/s each second until hitting the elevator floor.
The backpack is falling down in an accelerated way, the elevator is not.

With the elevator moving down at constant acceleration of 9.81 m/s^2, what would happen if you removed the scale (or Fs, or Fup or Fnet)?
Then, both, the elevator and the backpack would free fall at 9.81 m/s each second, none of those two things moving respect to each other until the elevator reaches the ground.
Both, the elevator and the backpack are falling down in an accelerated way, and at the same rate.
Fs would be zero in the event that the scale remains in place rather than being removed.

"The elevator is moving downwards with an acceleration of 3.8 m/s^2" means that the elevator is not free falling, but that its fall is restricted to some degree by its motor or brake.

The scale is the solid link between elevator and backpack that is preventing the backpack from free falling onto the elevator floor.
That solid link happens to be elastic in this case, and its deformation is proportional to its internal tension (Fs).
 
Last edited:
annamal said:
I am thinking
Forig (force of scale with non moving elevator) + m*a (accceleration of elevator) = Fs ( resulting force of scale)

How is that wrong?
I process this better like this:
Forig + m*a - m*g = m*a --> Forig = m*g
 
Lnewqban said:
With the elevator fully stopped or moving at constant velocity, what would happen if you removed the scale (or Fs, or Fup or Fnet (the way you have re-define it)?
The only force acting on the backpack would be the weight (mg).
Then, the backpack would free fall at 9.81 m/s each second until hitting the elevator floor.
The backpack is falling down in an accelerated way, the elevator is not.

With the elevator moving down at constant acceleration of 9.81 m/s^2, what would happen if you removed the scale (or Fs, or Fup or Fnet)?
Then, both, the elevator and the backpack would free fall at 9.81 m/s each second, none of those two things moving respect to each other until the elevator reaches the ground.
Both, the elevator and the backpack are falling down in an accelerated way, and at the same rate.
Fs would be zero in the event that the scale remains in place rather than being removed.

"The elevator is moving downwards with an acceleration of 3.8 m/s^2" means that the elevator is not free falling, but that its fall is restricted to some degree by its motor or brake.

The scale is the solid link between elevator and backpack that is preventing the backpack from free falling onto the elevator floor.
That solid link happens to be elastic in this case, and its deformation is proportional to its internal tension (Fs).
Ok, for an elevator dropping downwards with acceleration 3.8 m/s^2, in the elevator's frame of reference would Fs-mg = 0? Because that would mean Fs = m*g which doesn't make sense esp if the elevator is accelerating downwards.
 
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annamal said:
that's what I mean by net force for Fs
That's not the standard meaning of net force.
 
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annamal said:
Ok, for an elevator dropping downwards with acceleration 3.8 m/s^2, in the elevator's frame of reference would Fs-mg = 0? Because that would mean Fs = m*g which doesn't make sense esp if the elevator is accelerating downwards.
Again, the backpack is linked to the ceiling of the elevator via a spring (scale).
What the acceleration of the backpack would be respect to the elevator (its frame of reference)?
9.81-3.80 ≠ 0
If you have acceleration and a mass, you have a force.
 
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