Power given to particle by centripetal forces

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Homework Help Overview

The problem involves a particle of mass m moving in a circular path with a constant radius r, while its centripetal acceleration a varies with time as a = k2rt2. Participants are tasked with understanding the implications of changing centripetal acceleration on the motion of the particle.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between centripetal acceleration and tangential velocity, questioning how a changing centripetal acceleration can coexist with a constant radius. Some suggest that tangential acceleration is not restricted by the problem statement.

Discussion Status

The discussion is active, with participants offering various interpretations of the problem setup. Some have provided examples to illustrate the concepts, while others are clarifying the independence of centripetal and tangential components of motion.

Contextual Notes

There is an ongoing exploration of assumptions regarding tangential acceleration and its relationship to centripetal acceleration, as well as the implications of the problem's constraints.

Ghost Repeater
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Homework Statement



A particle of mass m is moving in a circular path of constant radius r such that its centripetal acceleration a varies with time t as a = k2rt2, where k is a constant. Show that the power delivered to the particle by the forces acting on it is mk4r2t5/3. [/B]

I have solved this problem, but I am still confused about it conceptually. If a particle's centripetal acceleration is changing with time, how can it continue to travel on a circular path of constant radius?
 
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Ghost Repeater said:
If a particle's centripetal acceleration is changing with time, how can it continue to travel on a circular path of constant radius?
It can speed up and slow down. I see no language in the problem statement restricting its tangential acceleration.

Clearly, knowing the centripetal acceleration as a function of time gives tangential velocity as a function of time and, accordingly, the tangential acceleration as a function of time.
 
It may be moving along a circular track of some sort (think bead on a wire), or perhaps it's fixed to the end of a light rod that pivots about the center. Or, perhaps it is kept on trajectory by tiny rockets :smile:
 
Ok, so centripetal and tangential vectors are independent of one another, analogous to the way that horizontal and vertical components of motion are independent in projectile problems?

But in that case how can a centripetal acceleration change the tangential velocity?
 
Ghost Repeater said:
Ok, so centripetal and tangential vectors are independent of one another, analogous to the way that horizontal and vertical components of motion are independent in projectile problems?

But in that case how can a centripetal acceleration change the tangential velocity?
There is no reason for it to need to. We are told how the centripetal acceleration changes with time. We are told that the object follows a circular path. We are not told that this causes the tangential acceleration. We merely infer the tangential acceleration because it is required to make the givens of the problem possible.
 
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An example would be the pendulum in a clock. As it swings back and forth the velocity and centripetal acceleration changes but the radius remains constant.
 

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