Understanding the Power of Elevator Lift Systems

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Homework Help Overview

The discussion revolves around understanding the power dynamics in elevator lift systems, specifically focusing on the relationship between the elevator's weight, the counterweight, and the power exerted by the motor during steady motion.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the implications of the elevator's steady speed on tension and power, questioning how the counterweight affects the overall power of the system. They discuss energy differences and the role of forces involved in the system.

Discussion Status

Several participants have provided insights into the energy and power relationships, with some clarifying the need to consider velocity in conjunction with force to determine power. There is an ongoing exploration of the signs associated with work and forces, indicating a productive dialogue without explicit consensus.

Contextual Notes

Participants are navigating the complexities of the problem, including the definitions of work and power, and the assumptions regarding the direction of forces and motion. The discussion reflects a mix of interpretations and clarifications regarding the physical principles involved.

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Homework Statement


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Homework Equations


P=Fv

The Attempt at a Solution


Since the elevator is rising at a steady speed, a=0, thus, the tension on the string equals to the weight of the elevator. I chose C as I thought just for the elevator case, it would be m1gv, but how does m2 affects the power of the system?
 
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Answer C is not correct.

Imagine the movement within a finite time Δt (and therefore a change of position of Δh for both m1 and m2). What is the energy difference of the whole system during Δt?
 
Janiceleong26 said:
Since the elevator is rising at a steady speed, a=0, thus, the tension on the string equals to the weight of the elevator. I chose C as I thought just for the elevator case, it would be m1gv, but how does m2 affects the power of the system?
Yes, the motor is working at that rate in raising the elevator, but what is happening on the other side? How much power is being transferred, and which way, between the counterweight and the motor?
 
stockzahn said:
Answer C is not correct.

Imagine the movement within a finite time Δt (and therefore a change of position of Δh for both m1 and m2). What is the energy difference of the whole system during Δt?
Energy difference would be (m1-m2)gΔh ?
 
haruspex said:
Yes, the motor is working at that rate in raising the elevator, but what is happening on the other side? How much power is being transferred, and which way, between the counterweight and the motor?
m2gv, and anti-clockwise? But I thought power is scalar? Does the minus sign comes from the velocity?
 
Janiceleong26 said:
Energy difference would be (m1-m2)gΔh ?
Correct. And instead of distance and energy you need velocity and power - so what to do?
 
stockzahn said:
Correct. And instead of distance and energy you need velocity and power - so what to do?
Divide it by Δt and you will get velocity and (m1-m2)g is the force, so force times velocity gives power. I got it! Thanks!
 
Janiceleong26 said:
m2gv, and anti-clockwise? But I thought power is scalar? Does the minus sign comes from the velocity?
Even scalar values can have sign. If A does positive work on B then B does negative work on A.
If you take up as positive and gravity as -g then the motor does work at rate -m1(-g)v on the elevator and at rate -m2(-g)(-v) on m2.
 
haruspex said:
Even scalar values can have sign. If A does positive work on B then B does negative work on A.
If you take up as positive and gravity as -g then the motor does work at rate -m1(-g)v on the elevator and at rate -m2(-g)(-v) on m2.
Oh I see, thanks. But why is there a negative sign before the mass?
 
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Janiceleong26 said:
Oh I see, thanks. But why is there a negative sign before the mass?
Because m(-g) is the force from gravity. The motor has to supply an equal and opposite force, -m(-g).
 
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