Torque & Force: Exploring Physics Problems

In summary: 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.OK.
  • #1
Ibraheem
51
2
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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  • #2
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.
 
  • #3
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?)
 
  • #4
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
 
  • #5
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.
 
  • #6
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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  • #7
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?
 
  • #8
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.
 
  • #9
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 ?
 
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  • #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
 

FAQ: Torque & Force: Exploring Physics Problems

What is torque and how is it related to force?

Torque is a measure of the rotational force applied to an object. It is defined as the product of the force and the distance from the point of rotation to the point where the force is applied. In other words, torque is the force that causes an object to rotate around a fixed point.

What are some real-world examples of torque and force?

Some common examples of torque and force include opening a door, tightening a bolt with a wrench, and throwing a baseball. In each of these scenarios, a force is applied at a distance from the point of rotation, causing a rotational motion.

How is torque and force related to the concept of equilibrium?

In physics, equilibrium refers to a state where all forces acting on an object balance out, resulting in no net force and no acceleration. Torque and force play a crucial role in equilibrium, as a force applied at a distance can create a torque that balances out other torques acting on an object.

How can torque and force be calculated mathematically?

To calculate torque, you need to know the magnitude of the force applied and the distance from the point of rotation. The formula for torque is T = F * d * sinθ, where T is torque, F is force, d is distance, and θ is the angle between the force and the lever arm. Force can be calculated using Newton's second law, F = m * a, where m is mass and a is acceleration.

How can torque and force be applied in everyday life?

Torque and force have many applications in everyday life, including in machines and tools, sports, and even cooking. For example, understanding torque can help in using tools such as wrenches and screwdrivers more effectively, and in sports such as golf and baseball, where rotational motion is essential. In cooking, torque and force are used when stirring or whisking ingredients to create a smooth mixture.

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