Is a shorter lever arm more effective in generating angular acceleration?

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Discussion Overview

The discussion revolves around the relationship between lever arm length, torque, moment of inertia, and angular acceleration in the context of two physics problems involving uniform bodies subjected to a force. Participants explore whether a shorter lever arm is more effective in generating angular acceleration and how this relates to the moment of inertia.

Discussion Character

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

Main Points Raised

  • One participant proposes that a shorter lever arm results in higher angular acceleration, questioning if this is correct.
  • Another participant emphasizes that angular acceleration cannot be determined without knowing the moment of inertia.
  • Discussions arise about the calculation of moment of inertia, with participants providing formulas based on different lever arm lengths.
  • Some participants clarify that the moment of inertia changes with the distance of the mass from the axis, while the lever arm is related to the point of force application.
  • There is confusion expressed about the distinction between the distance of the mass from the axis and the lever arm, with participants seeking clarification on how these concepts interact.
  • One participant suggests using a thin rod as an example to illustrate the differences in moment of inertia and torque based on where the force is applied.
  • Another participant acknowledges the distinction between moment of inertia and lever arm, stating that the moment of inertia is constant for a rigid object.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the effectiveness of shorter lever arms in generating angular acceleration. There are competing views regarding the relationship between lever arm length, moment of inertia, and angular acceleration, leading to ongoing debate and clarification.

Contextual Notes

Participants express uncertainty about the definitions and relationships between lever arm, moment of inertia, and torque, indicating that further exploration of these concepts is needed. The discussion highlights the complexity of these relationships in physics problems.

Ibraheem
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Hello,
I've recently tried to come up with my own physics problems to clarify the torque equation(T=αI). I've made up two problems with the same force magnitude and mass but different lever length.It turned out to me that the shorter the lever the higher the angular acceleration. Is that possible? or have I done it wrong? and does that mean the closer the force to the axis the more effective it is ?!

all the bodies in the two problems are uniformed and the forces are perpendicular to the lever r
Problem one: problem two:
givens: givens:
F=5N F=5N
m=0.3kg m=0.3kg
r=0.2m r= 0.8m
results: results :
α=83.3 rad/s^2 α=20.83 rad/s^2
T=1 N.m T=4 N.m



I would be grateful if someone could help me with this.

 
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Your expressions for torque are fine, but you cannot determine angular acceleration without the moment of inertia which is not shown nor described in a way that would allow its calculation.
 
Ibraheem said:
I assumed that the moment of inertia is I=MR^2 = (0.3)(2)^2=1.2
That expression gives the moment of inertia of a point mass a distance R from the axis. (What value of R are you using?)
 
Ignore my last comment I have mistaken the values of r with a different question I'm working on, sorry about that.
the values of moment of inertia are as following:

Problem 1: I=mr^2=0.3*0.2^2= 0.012
problem2 : I=mr^2=0.3*0.8^2=0.192

Again, sorry about the mistake
 
Ibraheem said:
the values of moment of inertia are as following:

Problem 1: I=mr^2=0.3*0.2^2= 0.012
problem2 : I=mr^2=0.3*0.8^2=0.192
OK.

Ibraheem said:
It turned out to me that the shorter the lever the higher the angular acceleration. Is that possible?
Only because you are changing the moment of inertia when you change the lever, since your masses are at that distance from the axis. If you kept the masses in the same place, thus keeping the moment of inertia the same, you'd find that shortening the lever reduces the angular acceleration.

Ibraheem said:
and does that mean the closer the force to the axis the more effective it is ?!
No.
 
Key point: Don't confuse the distance the mass is from the axis, which determines the moment of inertia, with the lever arm, which determines the torque from the applied force.

Also realize that the moment of inertia of a point mass is a special case, not a general result for an arbitrary object.
 
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Doc Al said:
OK.Only because you are changing the moment of inertia when you change the lever, since your masses are at that distance from the axis. If you kept the masses in the same place, thus keeping the moment of inertia the same, you'd find that shortening the lever reduces the angular acceleration.

In both of the problems, I assumed that the forces are all perpendicular to R which makes the lever= R, T=F.r sin90 . So how can I shorten the lever without changing the moment of inertia?
 
Ibraheem said:
In both of the problems, I assumed that the forces are all perpendicular to R which makes the lever= R, T=F.r sin90 . So how can I shorten the lever without changing the moment of inertia?
Realize that the lever arm has nothing to do with the distance the mass is from the axis. Unless you choose to use the same distance for both, which is what you did.

If you want to keep using a point mass, just fix its distance from the axis. Keep it the same for both calculations, so they have the same moment of inertia. Then, when finding the torque, use a different lever arm for each calculation.
 
I still don't get the difference between the distance and the lever arm.I know that the lever arm is a vector, but wouldn't the lever arm have a magnitude equal to the distance if the force is perpendicular (sin(90)) ? Also, I wanted to note that I have used different distances for each problem.
 
  • #10
Ibraheem said:
I still don't get the difference between the distance and the lever arm.
There are two distances involved here. One is the distance the mass is from the axis. That distance is used to calculate the moment of inertia.

The other distance is the lever arm, the distance from the point of application of the force and the axis. Two very different things.

I think you are confusing yourself by using a point mass. Try this: Imagine a thin rod of mass M and length L. What's the moment of inertia of that rod, assuming the axis of rotation is at one end and perpendicular to the rod? Then apply the force at two points: At the middle of the rod (lever arm = L/2) and at the end of the rod (lever arm = L). Compare the torque and resulting angular accelerations for both cases.
 
  • #11
Would changing the point of application of the force change the distance of mass?

So if the lever arm= L/2 will the moment of inertia be I=M(L/2)^2 or if the lever arm= L will the moment of inertia be I=ML^2 ?
 
Last edited:
  • #12
Ibraheem said:
Would changing the point of application of the force change the distance of mass?

So if the lever arm= L/2 will the moment of inertia be I=M(L/2)^2 or if the lever arm= L will the moment of inertia be I=ML^2 ?
Once again, the lever arm has nothing to do with the moment of inertia. The lever arm just describes where you are applying the force and thus determines the resulting torque created by that force.

The moment of inertia depends on how the mass is distributed, not where the force is applied.

Look up the moment of inertia of a thin rod.
 
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  • #13
Oh I see the difference now.The moment of inertia is constant for a rigid object so the moment of inertia of a rigid object is the proportionality constant
of T/α , and the lever arm is the line from the axis to point where the force applied and has nothing to do with the lever arm.

Thank you sir for the help
 

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