Solving for Rotational Kinetic Energy with Angular Speed and Masses

In summary: To find this, you need to calculate the linear velocity of the angular speed (using the work-energy theorem). r = distance from axis * tangential velocity.
  • #1
M98Ranger
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I have a question about this question that I hope someone can answer.

QUESTION: "A student on a piano stool rotates freely with an angular speed of 29.5rps. The student holds a 1.25 kg mass in each outstretched arm, .759m from the axis of rotation. The combined moment of Inertia of the student and the stool (ignoring the two masses) is 5.430kg.m^2 (a value that remains constant).

a.) As the student's arm are pull inward the angular speed is 3.54 rps. Determine the distance the masses are from the axis of rotation at this time (consider the masses to be modeled a mass-points).<I KNOW THE ENGLISH IS CHOPPED UP, BUT THIS IS HOW IT WAS WRITTEN ON THE PAPER.>

b.)Calculate KEfinal\KEINITIAL

MY THOUGHT PROCESS: This seems to me that the answers lie in utilizing the work-energy theorem which says that the net work done by external forces in a rotating rigid object about a fixed axis equals the change in the object's rotational energy. ie

(.5*IW^2)final-.5*IW^2)initial=Sum of Work
Where I=moment of inertia of an extended rigid object and W=instantaneous angular speed

To get radius (r) we know that W*r=tangential Velocity
we also know that I=m*r^2

MY questions:
-I don't understand how you can "ignore the two masses" in the calculation of I to get 5.430kg.m^2.
-How do I find the I of the whole system if the 2 masses are ignored
-Do I need to find the tangential velocity value of angular speed in order to find the R?
-If so, how would I go about doing it?

Thanks for reading this. Hopefully somebody can make sense of all this.
 
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  • #2
The PERSON's I is 5.43 [kgm^2] ... the TOTAL I is I_person + I_masses .
I_masses will depend on their distance from the rotation axis.

the person is on a "piano stool" so that the EXTERNAL torque is small.
That is, Angular momentum is conserved while the masses move inward.

Find the initial angular momentum, then the final angular speed ...
KE = 1/2 L omega ... (just like KE = 1/2 p v for linear motion).
 
  • #3
You said find the initial angular momentum and then find the final angular speed, but I thought that it gives you the final angular speed of 3.54rps. Maybe I am totally confused though.

here is what I did, but my answer is all messed up. I got 13.73 meters as my radius for my masses. Here goes...
Ip+Imasses= Itotal(initial)--->5.430[kg.m^2]+2*(1.25kg)*(.759m)^2=6.8702[kg.m^2] then, (IF X = the final I of the masses as they are brought in)
(.5*LW)initial=(.5*LW)final--->
(.5)*(6.87[kg.m^2])*(29.5rps)^2=(.5)(5.430+X[kg.m^2])(3.54rps)^2-->
X=471.667[kg.m^2] then, (IF 2mr^2 = X)
2*m*r^2=471.667[kg.m^2] | m=1.25kg
r=13.736meters...Pretty LONG arms, so where did I go wrong.
I am not understanding what you mean obviously when you said "find the initial angular momentum, then the final angular speed"

Thanks for the explanation thus far. It helped me tremendously.
 
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  • #4
M98Ranger said:
I have a question about this question that I hope someone can answer.

QUESTION: "A student on a piano stool rotates freely with an angular speed of 29.5rps.
Wow, he/she must be dizzy!
The student holds a 1.25 kg mass in each outstretched arm, .759m from the axis of rotation. The combined moment of Inertia of the student and the stool (ignoring the two masses) is 5.430kg.m^2 (a value that remains constant).

a.) As the student's arm are pull inward the angular speed is 3.54 rps.
there is something fishy. The number of rotation per second should *increase* as the mass are pulled inward.
Determine the distance the masses are from the axis of rotation at this time (consider the masses to be modeled a mass-points).<I KNOW THE ENGLISH IS CHOPPED UP, BUT THIS IS HOW IT WAS WRITTEN ON THE PAPER.>

b.)Calculate KEfinal\KEINITIAL

MY THOUGHT PROCESS: This seems to me that the answers lie in utilizing the work-energy theorem which says that the net work done by external forces in a rotating rigid object about a fixed axis equals the change in the object's rotational energy. ie

(.5*IW^2)final-.5*IW^2)initial=Sum of Work
Where I=moment of inertia of an extended rigid object and W=instantaneous angular speed

To get radius (r) we know that W*r=tangential Velocity
we also know that I=m*r^2

MY questions:
-I don't understand how you can "ignore the two masses" in the calculation of I to get 5.430kg.m^2.
-How do I find the I of the whole system if the 2 masses are ignored
-Do I need to find the tangential velocity value of angular speed in order to find the R?
-If so, how would I go about doing it?

Thanks for reading this. Hopefully somebody can make sense of all this.
there is no work done (no extrenal force acts on the system assuming that the friction force on the stool is negligibe.

Just calculate the initial K energy (using I_total = I_stool+student + I_masses) (the I of the two masses is just m* distance from the axis of rotation). This is a number you know.

Now, the final KE will contain one unknown: the distance at which the masses are. You can solve for this
 
  • #5
M98Ranger said:
You said find the initial angular momentum and then find the final angular speed, but I thought that it gives you the final angular speed of 3.54rps. Maybe I am totally confused though.

here is what I did, but my answer is all messed up. I got 13.73 meters as my radius for my masses. Here goes...
Ip+Imasses= Itotal(initial)--->5.430[kg.m^2]+2*(1.25kg)*(.759m)^2=6.8702[kg.m^2] then, (IF X = the final I of the masses as they are brought in)
(.5*LW)initial=(.5*LW)final--->
(.5)*(6.87[kg.m^2])*(29.5rps)^2=(.5)(5.430+X[kg.m^2])(3.54rps)^2-->
X=471.667[kg.m^2] then, (IF 2mr^2 = X)
2*m*r^2=471.667[kg.m^2] | m=1.25kg
r=13.736meters...obviously not possible so where did I go wrong.
I am not understanding what you mean obviously when you said "find the initial angular momentum, then the final angular speed"

Thanks for the explanation thus far. It helped me tremendously.
looks like you did it right (normally, omega should be put in radians per second not left in rps...here by luck it does not matter since it cancels out..but watch out for this in general).

The reason you get a larger value is that the values given in the initial question don't make sense. It would make much more sense if the initial value was 2.95 rps, not 29.5.
 
  • #6
EXACTLY WHAT I WAS THINKING... now I feel better that somebody else was thinking that it didn't make sense. I wish my teacher would proof homework before he gives it out to students.
Thanks for all your help.
 
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FAQ: Solving for Rotational Kinetic Energy with Angular Speed and Masses

What is rotational kinetic energy?

Rotational kinetic energy is the energy an object possesses due to its rotation around an axis. It is a form of kinetic energy that is associated with the motion of an object around a fixed point.

How is rotational kinetic energy calculated?

The formula for calculating rotational kinetic energy is 1/2 * I * ω^2, where I is the moment of inertia and ω is the angular velocity of the object. The moment of inertia is a measure of an object's resistance to rotational motion and depends on the object's mass and shape.

What factors affect rotational kinetic energy?

The amount of rotational kinetic energy an object has depends on its mass, moment of inertia, and angular velocity. The greater the mass and moment of inertia, the more rotational kinetic energy the object will have. Additionally, the faster an object rotates, the more rotational kinetic energy it will have.

How is rotational kinetic energy different from linear kinetic energy?

Rotational kinetic energy is the energy associated with an object's rotation, while linear kinetic energy is the energy associated with an object's linear motion. Rotational kinetic energy depends on an object's moment of inertia, while linear kinetic energy depends on an object's mass and velocity.

What are some real-life examples of rotational kinetic energy?

A spinning top, a rotating fan, a spinning wheel on a bicycle, or a spinning Earth are all examples of objects with rotational kinetic energy. Additionally, objects such as gears, wheels, and turbines also have rotational kinetic energy as they rotate around an axis.

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