Exploring Types of Acceleration in Rotational Movement of Rigid Bodies

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Discussion Overview

The discussion revolves around the types of acceleration in the rotational movement of rigid bodies. Participants explore various forms of acceleration, including translational and rotational, and seek to clarify the relationships and equations governing these movements.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants categorize movements into translational and rotational, with rotational movements further divided based on whether they occur around the center of mass or an external point.
  • There is a discussion about the equation for rotational acceleration, with some stating it as a=ra and others clarifying it as a=r*alpha.
  • Participants debate the correct expression for acceleration in circular motion, with conflicting views on whether it should be expressed as a=ω²·r or simply a=ω.
  • Some participants express confusion regarding the definitions of angular velocity (ω) and angular acceleration (α), and their relationships to linear acceleration.
  • There are mentions of the need for clarity on different types of acceleration, including centripetal acceleration and tangential acceleration, as well as their corresponding formulas.
  • One participant emphasizes the importance of understanding the derivation of these equations rather than just accepting definitions.
  • There is a challenge regarding the validity of equating angular acceleration to the square of angular velocity, which some participants argue is incorrect.
  • Participants introduce equations for circular motion, including the coordinates and acceleration components, but express uncertainty about the terminology and concepts involved.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the definitions and relationships between different types of acceleration in rotational movement. Multiple competing views remain, particularly regarding the correct equations and interpretations of angular velocity and acceleration.

Contextual Notes

Some participants express confusion over the terminology and relationships between variables, indicating a potential lack of clarity in foundational concepts. The discussion includes references to specific equations and their derivations, but these are not universally accepted or understood among participants.

physea
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Hello,

I am confused about the types of acceleration in rotational movement of rigid bodies.

I am quite clear about the various types of movement of rigid bodies. The body can have translational movement where acceleration is dV/dt. But what are the other types of acceleration that the body may have?

I think we can categorise the other types of movements into rotational through the centre of mass and rotational through a centre outside the centre of mass.

Can you tell me please the equations that describe these? It is not clear and I see confusing things on the web, for example that a=ra.

Thanks!
 
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physea said:
I am quite clear about the various types of movement of rigid bodies. The body can have translational movement where acceleration is dV/dt. But what are the other types of acceleration that the body may have?

I think we can categorise the other types of movements into rotational through the centre of mass and rotational through a centre outside the centre of mass.
Any rigid motion can be characterized as a translation plus a rotation. You can choose any point you like to describe the rotation. Depending on the point you choose, the corresponding translation may be different.

For instance, a rolling wheel can be described as a translation of the axle and a rotation about the axle. Or it can be described (momentarily at least) as a rotation about the instantaneous point of contact with the road.
 
a=ra is the equation for rotational acceleration. It is usually written as a=r*alpha
 
osilmag said:
a=ra is the equation for rotational acceleration. It is usually written as a=r*alpha

Can anyone explain what is a and what alpha?
 
osilmag said:
a=ra is the equation for rotational acceleration. It is usually written as a=r*alpha
acceleration in circular movement is ##a=\omega^2\cdot r##
  • a is acceleration.
  • ##\omega## is angular velocity.
  • r is radius of trajectory.
 
olgerm said:
acceleration in circular movement is ##a=\omega^2\cdot r##
  • a is acceleration.
  • ##\omega## is angular velocity.
  • r is radius of trajectory.

Ok, but you say it's omega squared, while @https://www.physicsforums.com/members/osilmag.640068/ said it's simply omega!
 
physea said:
Ok, but you say it's omega squared, while @https://www.physicsforums.com/members/osilmag.640068/ said it's simply omega!
Omega squared is the correct one.
 
sophiecentaur said:
Omega squared is the correct one.

Are you sure?
It's x = rθ
So derivative of x = r times derivative of θ
So second derivative of x = r times second derivative of θ which is linear acceleration = r times angular acceleration

How can angular velocity (ω) be the square of angular acceleration?
 
physea said:
Are you sure?
If there is a misunderstanding here, then why not just look it up? Afaiac acceleration under circular motion is ω2r. Can you find a source that says otherwise.
This stuff is not really a matter of discussion. It's all written down and the definitions are accepted.
 
  • #10
sophiecentaur said:
If there is a misunderstanding here, then why not just look it up? Afaiac acceleration under circular motion is ω2r. Can you find a source that says otherwise.
This stuff is not really a matter of discussion. It's all written down and the definitions are accepted.

I don't want to just look it up, if I wanted to do that I would do it and wouldn't come here, but I suppose this is not the intention always as this forum would have no meaning.

I want to know how these are derived and related together.

So, I know that x=rθ.
From that, don't we derive that V=rω and γ=rα ? Aren't these correct so far?

How can α=rω^2 ?

By the way:
α = angular acceleration
γ = linear acceleration
 
  • #11
physea said:
How can α=rω^2 ?
Where did you get that from?
 
  • #12
A.T. said:
Where did you get that from?

olgerm said:
acceleration in circular movement is ##a=\omega^2\cdot r##
  • a is acceleration.
  • ##\omega## is angular velocity.
  • r is radius of trajectory.
 
  • #13
olgerm said:
a is acceleration.
physea said:
α = angular acceleration
 
  • #14
A.T. said:
...

Yeah, α = angular acceleration. I wrote the same.
α=rω^2
 
  • #15
physea said:
I wrote the same.
If you think you wrote the same as olgerm, then you need to use a bigger font, or better glasses.
 
  • #16
A.T. said:
If you think you wrote the same as olgerm, then you need to use a bigger font, or better glasses.

OK so you mean that γ=rω^2 then.
And we know that γ=rα
So α=ω^2. Is this true? The angular acceleration is the square of the angular velocity?
 
  • #17
physea said:
And we know that γ=rα
Where did you get that from?
 
  • #18
A.T. said:
Where did you get that from?
We know that x=rθ
Then x'=rθ'
So x''=rθ'' which is γ=rα.
 
  • #19
@physea What source are you using for your opinions and statements? I have a feeling that you are trying to self-drive through this topic and that you are trying to use Q and A to learn the stuff. This is not a good way (as you are demonstrating with many of your posts). You seem to be mixing up ideas and symbols, which may be why you arrive at things like "α=ω^2.", which is a nonsense statement where an acceleration is equated to a velocity squared. You would, I'm sure, never do that for linear motion.
You need a half decent mechanics book.
 
  • #20
  • #21
physea said:
So, I know that x=rθ
What's x, what's r, what's theta and what's the situation?

The horizontal acceleration of the axle on a car moving down the highway where theta is the accumulated angle turned by the wheel is different from the centripetal acceleration of a bug on a tire that is rotating in place.
 
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  • #22
jbriggs444 said:
What's x, what's r, what's theta and what's the situation?

The horizontal acceleration of the axle on a car moving down the highway where theta is the accumulated angle turned by the wheel is different from the centripetal acceleration of a bug on a tire that is rotating in place.

OMG, that's what I am trying to clarify with this thread but no-one answers properly.

So, again, I am asking, in rotational movement, what are the different types of acceleration and their formulas?

Will someone eventually post a 'comprehensive' reply instead of posting bits?
 
  • #23
What you mean by type of acceleration? If one pointmass is in circular movement then its coordinates are:
##
x=r\cdot sin(t\cdot\omega+\alpha)\\
y=r\cdot cos(t\cdot\omega+\alpha)
##
acceleration is:
##
a_x(t)=-r\cdot\omega^2\cdot sin(t\cdot \omega+\alpha)\\
a_y(t)=-r\cdot\omega^2\cdot cos(t\cdot \omega+\alpha)
##

If by rotational movement you that the body is spinning, then different parts of the body have different accelerations.
 
  • #24
olgerm said:
What you mean by type of acceleration? If one pointmass is in circular movement then its coordinates are:
##
x=r\cdot sin(t\cdot\omega+\alpha)\\
y=r\cdot cos(t\cdot\omega+\alpha)
##
acceleration is:
##
a_x(t)=-r\cdot\omega^2\cdot sin(t\cdot \omega+\alpha)\\
a_y(t)=-r\cdot\omega^2\cdot cos(t\cdot \omega+\alpha)
##

If by rotational movement you that the body is spinning, then different parts of the body have different accelerations.

You introduce terms that I don't understand.
If v=rω, what is α?

Also, from what I have gathered, there are two types of acceleration. The centripetal acceleration and the ... not sure how it is called, the acceleration that is tangent to the trace of the point/particle.

What are these accelerations equal to? Is there any other type of acceleration in circular/rotational motions?
 
Last edited:
  • #25
physea said:
You introduce terms that I don't understand.
If v=rω, what is α?
if ##x(0)=0## and ##y(0)=r##, then ##\alpha=0##.
It is hard to explain. If you understand what other variables mean and, what circular orbit is, then you should understand what ##\alpha## means.
 
  • #26
physea said:
The centripetal acceleration and the ... not sure how it is called, the acceleration that is tangent to the trace of the point/particle.
These equations assume constant angular speed therefore tangential acceleraition is 0.
 
  • #27
physea said:
So, again, I am asking, in rotational movement, what are the different types of acceleration and their formulas?

Will someone eventually post a 'comprehensive' reply instead of posting bits?
This is actually quite unreasonable. You are not asking one question or introducing a point for discussion. What you need is a whole Dynamics Course, which is not the brief of PF.
If it's too hard for you to find a suitable course then I suggest some on line course like the Kahn Academy.
 
  • #28
##a_{tangential}=r \cdot \frac{\partial \omega}{\partial t}##
 
  • #29
olgerm said:
##a_{tangential}=r \cdot \frac{\partial \omega}{\partial t}##
That's fine but he is demanding a "Comprehensive reply". There is no end to what that could entail.
 
  • #30
physea said:
OMG, that's what I am trying to clarify with this thread but no-one answers properly.

So, again, I am asking, in rotational movement, what are the different types of acceleration and their formulas?

Linear acceleration and angular acceleration.

Linear acceleration ##\vec{a}=\frac{d \vec{v}}{dt}## and angular acceleration ##\alpha=\frac{d \omega}{dt}##.

This article explains the meanings of the symbols in those equations, and provides an in-depth answer to your question: https://en.wikipedia.org/wiki/Rotation_around_a_fixed_axis
 

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