Calculate the angular velocity for each case

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Homework Help Overview

The discussion revolves around calculating the angular velocity of a wheel in two different scenarios involving gravitational potential energy and kinetic energy. The scenarios include a mass descending with the wheel and a mass in free fall impacting the wheel. The problem involves concepts from mechanics, particularly energy conservation and momentum.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the conversion of gravitational potential energy to kinetic energy in both cases, questioning the clarity of the problem statement regarding energy equivalence. Some participants discuss the implications of the moment of inertia and the impact of the mass on the wheel's motion.

Discussion Status

The discussion is ongoing, with participants providing insights into the calculations and questioning assumptions about energy distribution and momentum. There are suggestions to consider conservation laws, and some participants express uncertainty about the treatment of kinetic energy in relation to the mass and wheel.

Contextual Notes

Participants note the importance of including units in calculations and the potential confusion arising from the problem statement. There is a mention of the large moment of inertia of the wheel and its effect on the final kinetic energy of the mass.

leafy
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Homework Statement
Consider a wheel of large moment of inertia and radius. A mass is first allowed to descend with the wheel for a short distance as shown. It is then compared to the second case where it is free fall dropped for the same distance and make inelastic impact. The energy is the same for both cases.

Moment of inertia I = 10,000
Radius of the wheel r = 1000
Mass m = 2
Drop height h = 3
Relevant Equations
Mgh = .5mv^2
Mgh = .5(I)(w^2)
Ft = mv
Ftr = Iw
First case, descends with the wheel:
mgh = .5(I)(w^2) ———- GPE converted to wheel energy
w = .1095. ———- rotation result is .1095

Second case, allow to free fall and impulse:
mgh = .5(m)(v^2). ———- GPE converted to kinetic energy
v = 7.746 ———- result in speed of 7.746
Ft = mv ———— impulse when hit the wheel
Ftr = I(w) ———— impulse converted to angular momentum
w = 1.5491. ———— rotation result is 1.5491

is this correct?
 

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leafy said:
Homework Statement:: Consider a wheel of large moment of inertia and radius. A mass is first allowed to descend with the wheel for a short distance as shown. It is then compared to the second case where it is free fall dropped for the same distance and make inelastic impact. The energy is the same for both cases.
Have you quoted the problem statement exactly as given to you? As stated, it is not clear. For example, it says the energy is the same in both cases. But it's not clear what particular energy is the same.

leafy said:
Moment of inertia I = 10,000
Radius of the wheel r = 1000
Mass m = 2
Drop height h = 3
Always include the units when giving numerical values of physical quantities.

leafy said:
First case, descends with the wheel:
mgh = .5(I)(w^2) ———- GPE converted to wheel energy
w = .1095. ———- rotation result is .1095
The final KE is not just the KE of the wheel. There is also the final KE of the mass m. The GPE is converted into the final total KE of the wheel and mass m.

Include units.

leafy said:
Second case, allow to free fall and impulse:
mgh = .5(m)(v^2). ———- GPE converted to kinetic energy
v = 7.746 ———- result in speed of 7.746
Ft = mv ———— impulse when hit the wheel
The impulse experienced by the mass m equals the change in momentum of m. The change in momentum is not equal to mv because m does not come to rest when it sticks to the wheel. Just after the collision, m will be moving with the wheel. If you take this into account, then your approach should yield the correct answer. However, a nice way to approach this problem is to use a conservation law. Then you do not need to consider the impulse.
 
Last edited:
The gravitational potential energy is mgh is the same for both cases

The units are standard metric

Since the wheel is made with so much intertia, final KE of the mass can be ignored or 0.

Again, the intertia of the wheel so big, the change of the mass momentum could consider be mv.

Of course if you approach this problem with energy conservation, I believe the energy of the wheel is halves for the impusle case. But the impulse approach is many times greater energy that overwhelm the error margin.
 
Actually I think you're right, because the radius is also large that we can't ignored the final KE of the mass. Thanks
 
leafy said:
The gravitational potential energy is mgh is the same for both cases
OK. But did you quote the problem statement exactly as given to you?

leafy said:
The units are standard metric
So, the radius of the wheel is 1000 meters. That's big :wideeyed:

It is a good idea to include units in your calculations. Checking the consistency of units during a calculation is a good way to catch careless errors.

leafy said:
Actually I think you're right, because the radius is also large that we can't ignored the final KE of the mass. Thanks
Right. The rotational inertia of the particle, mr2, is much larger than the moment of inertia of the wheel. For the second part, I find that the particle m loses very little speed when it collides with the wheel.
 
Last edited:
leafy said:
Of course if you approach this problem with energy conservation, ...
For part 2, I was thinking of a different conservation law than energy. Conservation of energy is not very useful for this part, since there is some internal energy ("heat") created in the collision.
 

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