Angular Acceleration of a Fixed Rod

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Homework Help Overview

The discussion revolves around the angular acceleration of a fixed rod with a spherical object attached to its end. The problem involves calculating the angular acceleration after the system is released from a specific angle, incorporating concepts of torque and moment of inertia.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the calculation of torque and moment of inertia for both the rod and the attached sphere, questioning the use of the parallel-axis theorem and the correct distances for the center of mass.

Discussion Status

There is ongoing exploration of the correct approach to calculating the moments of inertia and torques. Some participants have provided guidance on the application of the parallel-axis theorem and the need to consider individual components of the system. Multiple interpretations of the problem setup are being discussed.

Contextual Notes

Participants express uncertainty regarding the mass of the rod and the distribution of mass in the system. There are also concerns about the assumptions made in the calculations and the applicability of certain equations under the conditions described.

Schulze
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Homework Statement


Consider a thin 14 m rod pivoted at one end. A uniform density spherical object (whose mass is 9 kg and radius is 3.2 m) is attached to the free end of the rod and the moment of inertia of the rod about an end is Irod =1/3mL^2 and the moment of inertia of the sphere about its center of mass is Isphere =2/5mr^2 . What is the angular acceleration of the rod immediately after it is released from its initial position of 35◦ from the vertical? The acceleration of gravity g = 9.8 m/s^2

If needed a graphical representation of the question can be found at the following link:
http://i1221.photobucket.com/albums/dd470/jokerg908/435.jpg

Homework Equations


τ = Iα
I = (1/3)MR2
τ = FRsin(Θ)

The Attempt at a Solution


Finding the position of the center of mass (x meters from pivot):
(x-7) = (14+3.2-x)
x=12.1 meters

Using xcm = 12.1 m, we can solve for α:
I = (1/3)(18 kg)(12.1 m)2 ≈ 878.46 kg·m2
τ = (18 kg)(9.8 m/s2)(12.1 m)sin(35°) ≈ 1224.264489 N·m
α = τ/I ≈ 1.39361 rad/s2

This answer is taken as incorrect by my online program. Any suggestions or assumptions that I have made in my calculations would be helpful. Thanks. One thing that I was worried about was that this method didn't use the moments of inertia that I was given.
 
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Did you try working out the torque due to each mass separately?
How did you combine the moments of inertia for the two parts of the rig? I'd have expected a sum in there somewhere.
 
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Moment of Inertia

Should I have used the parallel-axis theorem (I think it's called):

I = Icm + Md2

Then I wouldn't know what I should take as my value of M due to the mass distribution of the object?

My attempt to find I:

I = (Isphere + Md2) + (Irod + Md2)
I = (2/5 (9 kg)(3.2 m)2) + (3.2 kg)((D?)2) + ((1/3)(9 kg)(14 m)2) + (9 kg)((12.1 m)2)

I don't know how to find D? = the distance between the sphere and the center of mass, because D would be greater than the radius of the sphere. So I feel that D > r would cause me to make an assumption that the sphere is greater than it actually is?
 
Individual torques

I quite honestly have no clue how to find, individual torques on a system composed of multiple parts.
 
Should I have used the parallel-axis theorem (I think it's called):
Yes, you should have.
I think you have misunderstood the formula though - check that.
the term "d" refers to the distance between the center of mass of the object going in a circle and the rotation axis. The "Icm" refers to the moment of inertia for the same object rotating about it's center of mass.

I quite honestly have no clue how to find, individual torques on a system composed of multiple parts.
Gravity acts on the com of each individual component separately.
But I think you should concentrate on your understanding of moment of inertia first.
 
d is the distance between the two parallel axes of rotation (aka the distance between the axis of rotation Icm (of that object) and the moment of inertia I about a parallel axis through some other point).

In this case, we choose that other point to be the center of mass of the two combined objects in order to find the sum of their moments of inertia.

Now that I am thinking about the problem a bit more, I think that one should take (D?) to be 17.2 meters. Because this is the distance between the sphere's center of mass, and the pivot point. Therefore you would be finding the moment of inertia about the pivot point for the sphere.
 
In this case, we choose that other point to be the center of mass of the two combined objects in order to find the sum of their moments of inertia.
You need to rethink this.
The axis of rotation of the composite object is not at it's center of mass.
Now that I am thinking about the problem a bit more, I think that one should take (D?) to be 17.2 meters. Because this is the distance between the sphere's center of mass, and the pivot point. Therefore you would be finding the moment of inertia about the pivot point for the sphere.
Now you've got it.
 
Think i figured it out.

Correct I:

I = (Isphere + Md2) + (Irod) (Note: Irod needs no adjustment because we are rotating about a perpendicular axis through the end of the rod.)
I = (2/5 (9 kg)(3.2 m)2) + (9 kg)((17.2 kg)2) + (1/3)(9 kg)(14 m)2
I≈3287.424 kgm2

Xcm= 12.1 m

PEi = KEf, rotational
(18kg)(9.8 m/s2)(12.1*sin(90-35) m) = 0.5(3287.424 kgm2)(w2)
ωfinal2 = 1.063708782 (rad/s)2
ωfinal≈1.0313626 (rad/s)Applying analog to kinematics equations to find the solution:
2α(Δθ) = ωf2 - ωi2
where Δθ = (0-55)/2π, ωi2 = 0 rad/s

α≈0.0607589035 rad/s2 (Edit: sign should be positive, however, I tried this answer. It's not correct! I am about to rip my hair out) I don't know what I am doing wrong.

Any suggestions would be helpful, thanks. Do I have a large gap in my understanding of the concepts?
 
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@Tanya Sharma

@Tanya Sharma

To find the center of mass, you take the individual masses as point masses, and then calculate the center of mass between these two point masses.

Xcm = [(m1)(x1)) + (m2)(x2)]/Total mass of the two objects

Xcm = [(9 kg)(7 m) + (9kg)(17.2 m)] / (18 kg)

Xcm = 12.1 m, where this distance is along the length of the rod.
 
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  • #10
Hello Schulze

Schulze said:
I = (1/3)(18 kg)(12.1 m)2 ≈ 878.46 kg·m2

The mass of the rod is not given in the question and from the OP I got the impression that mass of the rod was 18 kg .

Anyways,if the mass of rod is 9 kg then you have correctly calculated the location of CM.

Schulze said:
Applying analog to kinematics equations to find the solution:
2α(Δθ) = ωf2 - ωi2
where Δθ = (0-55)/2π, ωi2 = 0 rad/s

This equation is applicable when angular acceleration α is constant. ‘α’ is variable in this problem.

Schulze said:
τ = (18 kg)(9.8 m/s2)(12.1 m)sin(35°) ≈ 1224.264489 N·m

Schulze said:
I = (2/5 (9 kg)(3.2 m)2) + (9 kg)((17.2 kg)2) + (1/3)(9 kg)(14 m)2
I≈3287.424 kgm2

You have correctly calculated both the net torque on the system about the pivot , and the MI of the system .

Now just apply τnet = Iα and get the value of α.

Hopefully you should get the correct answer .
 
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  • #11
Thanks for helping me out to understand the pieces of information that could be used to arrive at this answer.
I did find out how to do the problem, and got the right answer!

Is there any way that I mark this thread as solved?
 
  • #12
You just did. Well done.
 
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