Descending mass on rope attached to wheel

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Homework Help Overview

The problem involves a physics student descending from a height of 12.0 m using a rope attached to a wheel, with considerations of forces, energy, and rotational dynamics. The subject area includes mechanics, specifically kinematics and dynamics related to rotational motion.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss applying Newton's second law to both the student and the wheel, exploring the relationship between linear and angular motion. There are attempts to use energy conservation principles, with questions about the correct expressions for velocity and angular velocity.

Discussion Status

Participants are actively engaging with the problem, providing guidance on applying different physical laws and clarifying concepts. There is a focus on ensuring the relationships between linear and angular quantities are correctly understood, with some participants expressing uncertainty about certain concepts.

Contextual Notes

One participant notes that they have not been taught about torque, which may limit their approach to the problem. There is also mention of previous attempts yielding incorrect answers, prompting further exploration of the energy conservation method.

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Homework Statement


A physics student of mass 57.0 kg is standing at the edge of the flat roof of a building, 12.0 m above the sidewalk. An unfriendly dog is running across the roof toward her. Next to her is a large wheel mounted on a horizontal axle at its center. The wheel, used to lift objects from the ground to the roof, has a light crank attached to it and a light rope wrapped around it; the free end of the rope hangs over the edge of the roof. The student grabs the end of the rope and steps off the roof.

a) If the wheel has radius 0.300 m and a moment of inertia of 9.60 kg⋅m2 for rotation about the axle, how long does it take her to reach the sidewalk? Ignore friction.

b) How fast will she be moving just before she lands? (I have not done anything for part b yet)

Homework Equations


I don't know if these are relevant, and I am sure I am missing some.

F=ma

ω=θ/t

v=ωr

θ=h/r

The Attempt at a Solution


As the person descends, there is a constant tension in the rope so the force acting on the person is
ΣF=ma=T-mg (Taking up as positive)

The height of the building is equal to the amount of rope required to descend, so the angle that the wheel must rotate through is
θ=h/r

and so the angular velocity of the wheel is
ω=h/(rt)

But this is where is cannot figure out where to go from here.
I did try to solve this with energy, but it kept giving me an incorrect answer.
The moment of inertia does suggest energy method though, but I cannot get it to work properly.
 
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ConorDMK said:
As the person descends, there is a constant tension in the rope so the force acting on the person is
ΣF=ma=T-mg (Taking up as positive)
OK, you've applied Newton's 2nd law to the person. Good!

Now do the same thing for the wheel. Then you'll be able to solve for the acceleration.
 
Doc Al said:
OK, you've applied Newton's 2nd law to the person. Good!

Now do the same thing for the wheel. Then you'll be able to solve for the acceleration.

Do you mean apply the rotational form of Newton's 2nd law? τ=Iα
 
ConorDMK said:
Do you mean apply the rotational form of Newton's 2nd law? τ=Iα
Absolutely.
 
Doc Al said:
Absolutely.

But we haven't been taught that yet, so I wouldn't know how torque works.
 
ConorDMK said:
But we haven't been taught that yet, so I wouldn't know how torque works.
No problem. Use conservation of energy.

You tried it and got the wrong answer, so show what you did. (One key is to properly relate the linear speed of the falling person to the angular speed of the turning wheel.)
 
Doc Al said:
No problem. Use conservation of energy.

You tried it and got the wrong answer, so show what you did. (One key is to properly relate the linear speed of the falling person to the angular speed of the turning wheel.)

Energy before:
Etotal=mgh

Energy after:
Etotal=0.5mv2+0.5Iω2

using ω=h/(rt) and v=2h/t

mgh=0.5m(2h/t)2+0.5I(h/(rt))2

t2=(2mh2+0.5I(h/r)2)/(mgh)

t=√[(2mh2+0.5I(h/r)2)/(mgh)]

Putting in the values

t=√[(2(57kg)(12m)2+0.5I(12m/0.3m)2)/((57kg)(9.8N/kg)(12m))]

t=1.90s to 2 decimal places (1.89596... s)

I don't know if this would be the answer if I had of used τ=Iα.
 
ConorDMK said:
Energy before:
Etotal=mgh

Energy after:
Etotal=0.5mv2+0.5Iω2
This is good.

ConorDMK said:
using ω=h/(rt) and v=2h/t
Why is there a factor of 2 in the expression for v, but not in the expression for ω?
 
Doc Al said:
This is good.Why is there a factor of 2 in the expression for v, but not in the expression for ω?

suvat: s=t(v+u)/2 as u=0 for both
v=2s/t

so v=2h/t and ω=2h/(rt)

Correct? or should they be without the 2?
 
  • #10
ConorDMK said:
suvat: s=t(v+u)/2 as u=0 for both
v=2s/t

so v=2h/t and ω=2h/(rt)

Correct?
Correct!

ConorDMK said:
or should they be without the 2?
Nope, the 2 is correct.
 
  • #11
Doc Al said:
Correct!Nope, the 2 is correct.

so if I continue with mgh=0.5m(2h/t)2+0.5I(2h/(rt))2 I should get the correct answer?
 
  • #12
ConorDMK said:
so if I continue with mgh=0.5m(2h/t)2+0.5I(2h/(rt))2 I should get the correct answer?
Yes. Just solve for t.
 
  • #13
Doc Al said:
Yes. Just solve for t.
t=√[(2(57kg)(12m)+2(9.6kgm2)(12m/0.3m)2)/((57kg)(9.8N/kg)(12m))]

t=2.65s
 
  • #14
ConorDMK said:
t=√[(2(57kg)(12m)+2(9.6kgm2)(12m/0.3m)2)/((57kg)(9.8N/kg)(12m))]

t=2.65s
Looks good.
 

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