Angular velocity and rotational motion

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Discussion Overview

The discussion revolves around the concepts of angular velocity and acceleration in the context of rotational motion. Participants explore the relationship between angular velocity, linear velocity, and acceleration, addressing both theoretical and conceptual aspects of these topics.

Discussion Character

  • Conceptual clarification
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants express confusion about why angular velocity is the same for all points on a rotating object, questioning how this relates to acceleration.
  • Others clarify that while angular velocity is uniform for rigid bodies, linear velocity varies with distance from the axis of rotation.
  • It is noted that angular acceleration implies a change in angular velocity, but this does not contradict the uniformity of angular velocity in rigid objects.
  • Some participants argue that the concept of angular velocity being the same applies only to rigid bodies, while fluid dynamics would not support this uniformity.
  • There is a discussion about the implications of angular acceleration on the angular velocity of all points in a rigid object, suggesting that all points experience the same change over time.
  • Participants reference the mathematical relationships between angular and linear velocities, including the formulas that govern these concepts.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of angular velocity and acceleration, with multiple competing views on how these concepts interact, particularly in rigid versus non-rigid bodies.

Contextual Notes

Some participants highlight the distinction between angular and linear velocities, noting that linear velocity changes with radius while angular velocity remains constant for rigid bodies. The discussion also touches on the mathematical definitions and units of angular quantities, which may not be fully resolved.

MIA6
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For the rotational motion, on my book, it says "Since w (angular velocity) is the same for all points of a rotating object, a (alpha) also will be the same for all points.w and a are properties of the rotating object as a whole." The thing that I don't get is that why velocity is the same at all points no matter if there is an acceleration? Its speed is supposed to increase at each point? Hope you can explain, thank you.
 
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Remember that velocity is a vector. A vector has a magnitude and a direction. Speed is the magnitude of the velocity vector. So a velocity can change direction without changing speed. This is still a change in velocity and therefore an acceleration.

Uniform circular motion is a special case of continuous acceleration without a change in speed. Only the direction changes.
 
No, velocity is not the same for all points !
It differs from point to point, if not in value then in its direction.
Yet, the angular velocity associated with any point of the rotating
object is the same, direction - and value-wise.
Acceleration has nothing to do with this property.
 
DaleSpam said:
Remember that velocity is a vector. A vector has a magnitude and a direction. Speed is the magnitude of the velocity vector. So a velocity can change direction without changing speed. This is still a change in velocity and therefore an acceleration.

Uniform circular motion is a special case of continuous acceleration without a change in speed. Only the direction changes.

You just said that there is a change in velocity no matter its speed or direction. But why it stated that w (angular velocity) is the same for all points of a rotating object? It implies no change?
 
ln motion, on my book, it says "Since w (angular velocity) is the same for all points of a rotating object, a (alpha) also will be the same for all points.w and a are properties of the rotating object as a whole."
I believe that the inference is that the object is 'solid' or more precisely 'rigid', i.e. the points in the object are fixed within the object, in which case if all objects have the same angular velocity, then all points would have the same angular acceleration, i.e. the rate of change of angular velocity would the same for all points in the object.

Do not confuse angular velocity with linear velocity, since the linear velocity is constantly changes (direction) and the magnitude depends on r, the distance from axis of rotation.

The same angular velocity means the radius to a point sweeps the same angle (angular displacement) during a given time period (same length of time).
 
Astronuc said:
I believe that the inference is that the object is 'solid' or more precisely 'rigid', i.e. the points in the object are fixed within the object, in which case if all objects have the same angular velocity, then all points would have the same angular acceleration, i.e. the rate of change of angular velocity would the same for all points in the object.

Do not confuse angular velocity with linear velocity, since the linear velocity is constantly changes (direction) and the magnitude depends on r, the distance from axis of rotation.

The same angular velocity means the radius to a point sweeps the same angle (angular displacement) during a given time period (same length of time).

but wouldn't the angular velocity change any direction or increase speed when there is an acceleration since I was thinking about the same concept as linear velocity.
 
MIA6 said:
but wouldn't the angular velocity change any direction or increase speed when there is an acceleration since I was thinking about the same concept as linear velocity.
Yes, an angular acceleration implies a change in angular velocity, but that is not what the statement is addressing.

In a rotating object, the only way that every point can have the same angular velocity \omega is for the object to be rigid, and that rigidity also means that at a given instant, each point has the same angular acceleration \alpha if a torque is applied to the object. That would not be the case for a fluid (liquid or gas).
 
Last edited:
Astronuc said:
Yes, an angular acceleration implies a change in angular velocity, but that is not what the statement is addressing.

In a rotating object, the only way that every point can have the same angular velocity itex]\omega[/itex] is for the object to be rigid, and that rigidity also means that at a given instant, each point has the same angular acceleration \alpha if a torque is applied to the object. That would not be the case for a fluid (liquid or gas).

So if there is an acceleration, then the angular velocity would change, let say, from initial velocity 20m/s to 30m/s (maybe we can think of this as instantaneous velocity), then in every instant, it would be 30m/s? but wouldn't the speed keep increasing?from 20 -->25-->30-->35?
 
Well angular acceleration is measured in rad/s2, and angular velocity in rad/s, where rad means radians. One revolution represents an angular displacement of 2\pi radians. Radians are dimensionless, i.e. they don't have length.

The magnitude of linear (tangential) velocity of a point in a rotating object is given by v=\omegar, where r is the distance of said point from the axis of rotation.

So the linear (tangential) velocity varies with r.

See if this reference helps - http://hyperphysics.phy-astr.gsu.edu/hbase/rotq.html

http://hyperphysics.phy-astr.gsu.edu/hbase/mi.html

Note the equation \omega\,=\,\omega_0\,+\,\alpha{t}, where \omega\,=\,\omega(t)
 
  • #10
Astronuc said:
Well angular acceleration is measured in rad/s2, and angular velocity in rad/s, where rad means radians. One revolution represents an angular displacement of 2\pi radians. Radians are dimensionless, i.e. they don't have length.

The magnitude of linear (tangential) velocity of a point in a rotating object is given by v=\omegar, where r is the distance of said point from the axis of rotation.

So the linear (tangential) velocity varies with r.

See if this reference helps - http://hyperphysics.phy-astr.gsu.edu/hbase/rotq.html

http://hyperphysics.phy-astr.gsu.edu/hbase/mi.html

Note the equation \omega\,=\,\omega_0\,+\,\alpha{t}, where \omega\,=\,\omega(t)


RIght, I forgot it should be radian/second. According to the formula, average alpha=delta w/ delta t, can we know that at every point, or every instant, the average velocity is increasing or remains at a new velocity at every point? let's say, if the original is w=24 rad/s, then the new w is 30rad/s, and will it remain at every point or it will accelerate so will have bigger and bigger speed at each point.
 
  • #11
If every point has angular velocity 24 rad/s, then some time later, every point has angular velocity of 30 rad/s, then every point accelerated at the same angular acceleration, since every point had the same change in angular velocity over the same period of time.
 
  • #12
Astronuc said:
If every point has angular velocity 24 rad/s, then some time later, every point has angular velocity of 30 rad/s, then every point accelerated at the same angular acceleration, since every point had the same change in angular velocity over the same period of time.

Oh, so what you said was, suppose the angular acceleration is 5 rad/s^2, then every point or every instant will increase the same amount 5 rad/s^2 at one second, and then the next second, it will still increase 5 rad/s^2, so that their velocity at every instant is the same, which is unlike translational motion that each point has different/increasing velocity when it undergoes acceleration?
 
  • #13
MIA6 said:
Oh, so what you said was, suppose the angular acceleration is 5 rad/s^2, then every point or every instant will increase the same amount 5 rad/s^2 at one second, and then the next second, it will still increase 5 rad/s^2, so that their velocity at every instant is the same, which is unlike translational motion that each point has different/increasing velocity when it undergoes acceleration?
Close.

If angular acceleration is 5 rad/s^2, then in one second, the angular velocity increases by 5 rad/s (i.e. \Delta\omega\,=\,\alpha*\Delta{t} => 5 rad/s = 5 rad/s2 * 1 s), and if the angular acceleration remains constant, then after another second the angular velocity increases by 5 rad/s.

Acceleration implies a change in velocity with time, whether it's linear or angular.

The point of the comment "Since w (angular velocity) is the same for all points of a rotating object, a (alpha) also will be the same for all points.w and a are properties of the rotating object as a whole." is that if all points of a rotating body rotate simultaneously at the same angular velocity, then the body is rigid, and this then implies that all points in a rigid body will experience that same angular acceleration simultaneously. The key is RIGID body.
 

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