Analyzing Angular Acceleration and Particle Motion in Rotating Spheres

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Homework Help Overview

The problem involves a solid sphere rotating with constant angular acceleration about a fixed axis, focusing on the linear acceleration of a particle within the sphere. The scenario includes analyzing the relationship between tangential and centripetal acceleration and determining the total angle the sphere has turned at a specific instant.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the implications of constant angular acceleration on tangential and centripetal acceleration, questioning how these accelerations change over time. There is an exploration of vector representations of acceleration and the direction of overall linear acceleration.

Discussion Status

The discussion is active, with participants offering insights into the nature of tangential and radial accelerations. Some participants are attempting to express angular velocity in terms of time and are considering the implications of starting from rest. There is a recognition of the need to clarify initial conditions and the relationship between forces acting on the particle.

Contextual Notes

Participants note the importance of understanding the initial angle and the definitions of acceleration in the context of the problem. There is an acknowledgment of the need for a force diagram to analyze the resultant force direction.

Jamest39
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Homework Statement


A solid sphere, starting from rest, rotates with constant angular acceleration α about a fixed axis passing through its center. Consider a particle within this sphere that lies at a perpendicular distance r from this axis. If, at some instant, the linear acceleration of this particle makes an angle of 50° with respect to the direction of its tangential acceleration, what is the total angle that the sphere has turned through up until that instant?

Homework Equations


tangential acceleration = αr
centripetal acceleration = ω^2r

The Attempt at a Solution


Since the angular acceleration is constant, the tangential acceleration would also remain constant and I don't see how the angle could be changing.
 
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Jamest39 said:
Since the angular acceleration is constant, the tangential acceleration would also remain constant and I don't see how the angle could be changing.
Definition of acceleration.
Note: angular acceleration is constant but not zero... who says the centripetal acceleration is constant?
You are given the final angle... to make sense of the problem statement you need to make a decision about the initial angle and maybe other things too. You'll need to look through your notes for the right context.
 
Last edited:
Jamest39 said:
tangential acceleration = αr
It would be well to consider that as a vector equation. In that view, what varies?
 
haruspex said:
It would be well to consider that as a vector equation. In that view, what varies?
The angular velocity would be changing. But considering those as vectors, the direction would be constantly changing.
 
Jamest39 said:
considering those as vectors, the direction would be constantly changing.
Exactly so. Therefore the tangential acceleration is changing (in direction).
Starting from rest at t=0, what is its tangential acceleration at time t, and what is its radial acceleration at that time?
 
haruspex said:
Exactly so. Therefore the tangential acceleration is changing (in direction).
Starting from rest at t=0, what is its tangential acceleration at time t, and what is its radial acceleration at that time?
Since its starting from rest, it would be zero at t=0. Then after that, the tangential acceleration is given by rα or (Δω)/(Δt) and the centripetal acceleration is given by (ω^2)r
 
Jamest39 said:
Since its starting from rest, it would be zero at t=0. Then after that, the tangential acceleration is given by rα or (Δω)/(Δt) and the centripetal acceleration is given by (ω^2)r
Yes, but express ω in terms of t.
 
haruspex said:
Yes, but express ω in terms of t.
ω in terms of t, so (Δθ)/(Δt)
 
Jamest39 said:
ω in terms of t, so (Δθ)/(Δt)
Use the fact that α is constant.
 
  • #10
haruspex said:
Use the fact that α is constant.
right, so that allows us to use the equation ω=ω(initial) + αt, and since its staring from rest, the ω(initial is zero).
 
  • #11
Jamest39 said:
right, so that allows us to use the equation ω=ω(initial) + αt, and since its staring from rest, the ω(initial is zero).
Right. So you know the tangential acceleration at time t and the radial acceleration at time t. So in what direction is the overall linear acceleration at time t?
 
  • #12
haruspex said:
Right. So you know the tangential acceleration at time t and the radial acceleration at time t. So in what direction is the overall linear acceleration at time t?
In the direction of the rotation, between the tangential and centripetal acceleration vectors
 
  • #13
Jamest39 said:
In the direction of the rotation, between the tangential and centripetal acceleration vectors
You can write it as an explicit formula, in terms of r, t and alpha.
It might help if I ask you this first: if there is a vertically upward force U acting on a body and a force R acting horizontally to the right, at what angle to the horizontal is the net force?
 
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  • #14
haruspex said:
You can write it as an explicit formula, in terms of r, t and alpha.
It might help if I ask you this first: if there is a vertically upward force U acting on a body and a force R acting horizontally to the right, at what angle to the horizontal is the net force?
A 45 degree angle?
 
  • #15
i have the same problem and have no clue how to start
 
  • #16
Jamest39 said:
A 45 degree angle?
No, it depends on R and U. Do you know how to draw a force diagram, with two forces at right angles, the lengths of the lines representing the magnitudes of the forces? What line represents the resultant? What angle does it make to the other lines?
 

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