Using Energy Conservation to Find Height in Pulley System

In summary, the block's acceleration is 2.0m/s when it reaches its final speed. The block has dropped 1.5m from its initial height.
  • #1
candyq27
71
0
This is a multiple part problem but I'd like to have some help on one part at a time. Here is the general question:

A pulley with a radius of R=0.50m and a mass of M=4.0kg is mounted on a frictionless axle. The pulley is a uniform solid disk with a rotational inertia of I=1/2MR^2. A block with a mass m=2.0kg hangs from a string wrapped around the pulley. When the system is released from rest the block accelerates down. Use g=10m/s^2.
a) After dropping through a height h, the block's speed is 2.0m/s. Use energy conservation to find h.
b)Apply Newton's Second Law, and Newton's Second Law for Rotation. Solve your equations to find the acceleration of the block.
c)Use your value from (b) and one or more constant acceleration equations to find h, the distance the block has dropped when its speed reaches 2.0m/s. Does it agree with your answer from (a)?

So for part (a)...
the energy is KE + PE so it is 1/2Iw^2 + mgh which is...1/2(1/2(4.0kg)(0.50m)^2)0^2 + (2.0kg)(10m/s^2)h
the final energy is 1/2(2.0kg)(2.0m/s)^2 + (2.0kg)(10m/s^2)(0m)
so setting them equal to each other you get...
20h=4 so h=4/20, simplified is h=1/5
Is that right? If not please give me some hints, and I will work on part (b). Thanks!
 
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  • #2
candyq27 said:
This is a multiple part problem but I'd like to have some help on one part at a time. Here is the general question:

A pulley with a radius of R=0.50m and a mass of M=4.0kg is mounted on a frictionless axle. The pulley is a uniform solid disk with a rotational inertia of I=1/2MR^2. A block with a mass m=2.0kg hangs from a string wrapped around the pulley. When the system is released from rest the block accelerates down. Use g=10m/s^2.
a) After dropping through a height h, the block's speed is 2.0m/s. Use energy conservation to find h.
b)Apply Newton's Second Law, and Newton's Second Law for Rotation. Solve your equations to find the acceleration of the block.
c)Use your value from (b) and one or more constant acceleration equations to find h, the distance the block has dropped when its speed reaches 2.0m/s. Does it agree with your answer from (a)?

So for part (a)...
the energy is KE + PE so it is 1/2Iw^2 + mgh which is...1/2(1/2(4.0kg)(0.50m)^2)0^2 + (2.0kg)(10m/s^2)h
the final energy is 1/2(2.0kg)(2.0m/s)^2 + (2.0kg)(10m/s^2)(0m)
so setting them equal to each other you get...
20h=4 so h=4/20, simplified is h=1/5
Is that right? If not please give me some hints, and I will work on part (b). Thanks!
What did you do with the kinetic energy of rotation of the pulley at the final position? It is not zero! You seem to do it as if you must include the kinetic energy of rotation of the pulley at the initial position only and the kinetic energy of translation of the falling mass at the end only. Actually, both must be included at the initial AND at the final positions. So the full equation is really
[tex] {1 \over 2} I \omega_i^2 + {1 \over 2} m v_i^2 + m g y_i = {1 \over 2} I \omega_f^2 + {1 \over 2} m v_f^2 + m g y_f [/tex]
In your case, both the pulley and the mass are initial at rest. But they are both in motion at the end. If you set the origin of the y-axis to be at the final position, you get [itex] y_f=0 [/itex] and [itex] y_i = h [/itex]. So you have
[tex] mg h = {1 \over 2} I \omega_f^2 + {1 \over 2} m v_f^2 [/tex]

Hope this helps.

Patrick
 
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  • #3
how do i figure out the wf of the pulley? I think that's where I'm getting confused. Thanks!
 
  • #4
Is the wf of the pulley v/r? so is it (2m/s)/(0.50m)=4.0rad/s
...
which makes the equation...
(this is going to look messy sorry)
(2.0kg)(10m/s^2)h = [1/2(1/2(4.0kg)(0.50m)^2](4.0rad/s)^2 + [1/2(2.0kg)(2.0m/s)^2]
20h = (4) + (4)
h= 8/20
h = 0.40m
 
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  • #5
Now for part (b)...
Newton's Second Law is F=ma, and Newton's Second Law for Rotation is T=I@ (torque=moment of inertia*alpha)
I know that I=mr^2 and alpha=a/r so...torque=mra
But then if F=ma and torque=mra, I'm not sure where to go with it..?
If a=F/m and a=torque/mr then ??
 
  • #6
candyq27 said:
Now for part (b)...
Newton's Second Law is F=ma, and Newton's Second Law for Rotation is T=I@ (torque=moment of inertia*alpha)
I know that I=mr^2 and alpha=a/r so...torque=mra
But then if F=ma and torque=mra, I'm not sure where to go with it..?
If a=F/m and a=torque/mr then ??

The torque on the pulley comes from the tension in the string, and the tension is part of the force acting on the mass. Write the equations for each object in terms of the unknown tension and acceleration. Solve the two equations for the two unknowns.
 
  • #7
So I need to figure out the torque and the tension? I'm confused. Do I need to figure out what's acting on the pulley and the block? If so how do I put those together?
 
  • #8
candyq27 said:
So I need to figure out the torque and the tension? I'm confused. Do I need to figure out what's acting on the pulley and the block? If so how do I put those together?
Draw a FBD for the mass. The forces acting are gravity and tension. Apply Newton's second law. Draw a FBD for the disk. There is a torque related to the tension. Apply the rotational analog of Newton's second law. You now have two equations involving the tension, the linear acceleration of the mass, and the angular acceleration of the disk. You already know how to replace one of the accelerations with the other. Whichever way you choose to do that you are left with two equations and two unknowns. Solve them.
 
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  • #9
Ok so for the block i got a=F/m and for the pulley i did torque=I*alpha and torque=tension*r so alpha=Tr/I
But I'm still not understanding where to go with it...?sorry
Is the F the tension on the block? is that (mv^2)/r?
Or do I do the block is a=T/m and alpha=Tr/I but isn't alpha just a/r?
 
  • #10
Or do i do a=T/m and alpha=Tr/I so then i plug in the T=ma to get alpha=(mar)/(1/2mr^2) = (2a)/r

so the acceleration of the block is a=(alpha*r)/2
 
  • #11
candyq27 said:
Ok so for the block i got a=F/m and for the pulley i did torque=I*alpha and torque=tension*r so alpha=Tr/I
But I'm still not understanding where to go with it...?sorry
Is the F the tension on the block? is that (mv^2)/r?
Or do I do the block is a=T/m and alpha=Tr/I but isn't alpha just a/r?
F is the sum of two forces acting on the block, gravity and tension. There is no mv²/r in this problem. We do not care about the forces that are holding the disk together.

candyq27 said:
Now for part (b)...
Newton's Second Law is F=ma, and Newton's Second Law for Rotation is T=I@ (torque=moment of inertia*alpha)
I know that I=mr^2 and alpha=a/r . . . . . . .
You were good up to the point where I ended the quote, except that is not the correct moment of inertia of a disk.
 
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  • #12
Isn't the problem with a solid disk? Thats why I used the inertia I=1/2mr^2

For the block, is the F=-mg+T?
and for the pulley disk is it torque=I(a/r)= (1/2mr^2)(a/r) = 1/2mra?

And then would the net forces acting on the block equal the torque of the pulley?
So it would be -mg+T = 1/2mra and solve for a to get a=2(-mg+T)/mr
 
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  • #13
candyq27 said:
Isn't the problem with a solid disk? Thats why I used the inertia I=1/2mr^2

For the block, is the F=-mg+T?
and for the pulley disk is it torque=I(a/r)= (1/2mr^2)(a/r) = 1/2mra?

And then would the net forces acting on the block equal the torque of the pulley?
So it would be -mg+T = 1/2mra and solve for a to get a=2(-mg+T)/mr
½mr² is good. You wrote mv²/r before. Maybe you did not mean that. Yes, the force on the block is T - mg or mg - T if you take downward as the positive direction, but by Newton's second law the force is ma. Why do you have the ½mr in your block equation? Taking downward positive is convenient becasue you expect downward acceleration. Your torgue equation is fine.
 
  • #14
Sorry I've been looking at this problem for so long I'm confusing myself. Thanks for being patient.
Ok so the force on the block is T-mg and that is equal to ma? so then a of the block is a= (T/m)-g

But then do i set that equal to 1/2mra and solve for ...what?
 
  • #15
and then what?
 
  • #16
candyq27 said:
Sorry I've been looking at this problem for so long I'm confusing myself. Thanks for being patient.
Ok so the force on the block is T-mg and that is equal to ma? so then a of the block is a= (T/m)-g

But then do i set that equal to 1/2mra and solve for ...what?
You need to be consistent with the sign convention. When you wrote torque = I(a/r) = ½mr²(a/r) = ½mra you were assuming a was positve downward. When you write T - mg = ma, you are assuming a is positve upward. You need a to be positive in only one direction, or you need to have two different a where one is the negative of the other (not recommended). So let's write your last equation as

mg - T = ma
g - T/M = a

Now substitute this expression for a into the other equation you have relating T and a, namely torque = Tr (you wrote that several posts back) and Tr = ½Mra or T = ½Ma. Alternatively, you can solve the equation above for T instead of a, and substitute T into the Tr = ½mra. So either you have

T = ½M(g - T/M)

OR

T = mg - ma
mg - ma = ½Ma

You can solve these equations for T and a. Usually one just writes one of these equations, solves it, and then goes back to either of the two original equations and plugs in the now-known value to solve for the other variable. That is exactly equivalent to doing the algebra I did to get these two equations. It's just doing things in a little different order.

Be careful to keep the M and m distinct. Somewhere you merged them into the one symbol, m, but the mass of the disk is not the same as the mass of the block.
 
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  • #17
so then you should get a = (2mg)/(M+2m) and when you solve for a you get 5m/s^2, right?
 
  • #18
ok so part (d): Use your value from (c) and one or more constant-acceleration equations to find h,
the distance the block has dropped when its speed reaches 2.0 m/s. Does it agree with your answer from (a)?

so i used w = wi + alpha*t
t = w/alpha
t = 4/5 = 0.8 sec

then i plugged that into x = xi + (wi)t = 1/2*alpha*t^2
xi = 0
wi = 0
so, = 1/2(5)(.8)^2

but my answer comes out to 1.6m

are (a) and (c) suppsed to have the same answers? Am i doing something wrong?

Thanks so much!
 
  • #19
jalpabhav said:
so then you should get a = (2mg)/(M+2m) and when you solve for a you get 5m/s^2, right?

M = 2m, so a = 2mg/4m = g/2 = 5m/s²

Looks good!
 
  • #20
For the last part I used the equation v=vo +at and solved for t=(v-vo)/a = (2m/s-0m/s)/(5m/s^2) = 0.40s
Then I plugged that into the equation h=ho+vot+1/2at^2 to get h=0+0+1/2(5m/s^2)(0.40s)^2 = 0.40m and that is the same as I got in part (a) YAY! Thank you!
 
  • #21
yea i got 0.40 m for both a and c too...awesome!
 

What is pulley energy conservation?

Pulley energy conservation is the principle that states energy cannot be created or destroyed, only transferred or converted from one form to another. In the case of pulleys, the energy put into the system by an input force is conserved and transferred to the output force.

How does a pulley system conserve energy?

A pulley system consists of a rope or belt wrapped around a wheel or axle, with one end attached to a fixed point and the other end attached to a moveable object. As the input force is applied to the rope, it is transferred to the load being lifted, allowing it to be moved with less effort. This transfer of energy from the input force to the output force is what allows for energy conservation in a pulley system.

What are the types of energy involved in pulley energy conservation?

The types of energy involved in pulley energy conservation include potential energy, kinetic energy, and mechanical energy. Potential energy is stored energy that is dependent on the position or configuration of an object, such as the load being lifted by a pulley. Kinetic energy is the energy of motion, which is transferred from the input force to the output force in a pulley system. Mechanical energy is the sum of potential and kinetic energy and is conserved in a pulley system.

What are some real-life examples of pulley energy conservation?

Pulley energy conservation is utilized in various real-life applications. One common example is in elevators, where a motor applies an input force to lift the elevator car and its passengers, conserving energy as it transfers it to the pulley system. Another example is in exercise equipment, such as weight machines, where pulleys are used to lift weights and conserve energy for the user. Pulley systems are also used in cranes and construction equipment to lift heavy loads with less effort.

How is pulley energy conservation important in everyday life?

Pulley energy conservation is important in everyday life as it allows us to use less energy to perform tasks that would otherwise require a greater amount of effort. This is especially beneficial in activities that involve lifting or moving heavy objects. In addition, understanding the principles of pulley energy conservation can help us design more efficient machines and systems that conserve energy and reduce waste.

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