Conservation of Energy - Elevator Problem.

In summary, the cable of the elevator cab snaps at the first floor, causing it to fall 3.7 meters onto a cushioning spring with a spring constant of 0.15 MN/m. The cab is also slowed down by a frictional force of 4.4 kN. The speed of the cab right before it hits the spring is 7.4 m/s and the maximum distance the spring is compressed is 0.90 m. The cab will bounce back up the shaft to a height of 2.8 m above the point of maximum compression. Using conservation of energy, the approximate total distance the cab will move before coming to rest is 15 m.
  • #1
dhchemistry
Alright, so I'm a little stuck on the last bit of this problem:

The cable of the 1,800 kg elevator cab snaps when the cab is at rest at the first floor, where the cab bottom is a distance d = 3.7 m above a cushioning spring whose spring constant is k = 0.15 MN/m. A safety device clamps the cab against guide rails so that a constant frictional force of 4.4 kN opposes the cab's motion. (a) Find the speed of the cab just before it hits the spring. (b) Find the maximum distance x that the spring is compressed (the frictional force still acts during this compression). (c) Find the distance (above the point of maximum compression) that the cab will bounce back up the shaft. (d) Using conservation of energy, find the approximate total distance that the cab will move before coming to rest. (Assume that the frictional force on the cab is negligible when the cab is stationary.)I was able to solve parts a-c without too much of a problem. I just can't get part 3.

Here are my solutions:
a) [tex]
\Sigma F=mg-F_{k}=ma[/tex]
[tex]a=g-\frac{F_{k}}{m}[/tex]
[tex]a=7.4m/s^{2}[/tex]
[tex]v_{f}^{2}=v_{i}^{2}+2as[/tex]
[tex]v_{f}=\sqrt{2(7.4m/s^{s})(3.7m)}[/tex]

so
[tex]
v_{f}=7.4m/s
[/tex]

b) [tex]\frac{1}{2}mv^{2}-(mg-F_{k})x-\frac{1}{2}kx^{2}=0[/tex]

Then I solved the quadratic equation and found
x=.90m

c) [tex]\frac{1}{2}kx^{2}=mgh+F_{k}h[/tex]
[tex]\frac{1}{2}kx^{2}=h(mg+F_{k})[/tex]
[tex]h=\frac{\frac{1}{2}kx^{2}}{mg+F_{k}}[/tex]
[tex]h=2.8m[/tex]

Now for d, I tried:
[tex]K=F_{k}x[/tex]
[tex]\frac{1}{2}mv^{2}=F_{k}x,
[/tex]

Since the only slowing force doing work on the elevator is friction. If I use the v from part a and solve for x, however, I get 11.2m. The solution in the back of the book is 15m. Any ideas?
 
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  • #2
dhchemistry said:
b) [tex]\frac{1}{2}mv^{2}-(mg-F_{k})-\frac{1}{2}kx^{2}=0[/tex]

This can't be right. The first term has units of energy while the second term has units of force. Second term should be mgx - Fx.
 
  • #3
Delphi51 said:
This can't be right. The first term has units of energy while the second term has units of force. Second term should be mgx - Fx.

You're right. That's a typo. Sorry!
 
  • #4
So, for part (b) x = 0.783 ?
In part (c), I think you need an additional term on the right for the spring energy after it goes up h and is stretched away from equilibrium: 1/2*k*(x-h)^2.
But I'm getting a final answer of 1.86 for h.
Seems to me 15 m is unreasonable - it would bounce only to 3.7 + .783 m if there was no friction.
 
  • #5
Delphi51 said:
So, for part (b) x = 0.783 ?
In part (c), I think you need an additional term on the right for the spring energy after it goes up h and is stretched away from equilibrium: 1/2*k*(x-h)^2.
But I'm getting a final answer of 1.86 for h.
Seems to me 15 m is unreasonable - it would bounce only to 3.7 + .783 m if there was no friction.

The answers to a, b, and c I have are the correct answers. 15m is also correct, I confirmed this with my professor.

As far as c goes, that term is unnecessary because the spring is not both giving and taking energy. It's only releasing its stored energy as it expands back to its original position.
 
  • #6
Doesn't make sense to me. You have an elevator that falls 3.7 meters and then bounces back up 15 meters?

that term is unnecessary because the spring is not both giving and taking energy.
Yes it is. It takes in energy when it is being compressed, releases it when it springs back to the equilibrium point, then takes in some more as it is stretched beyond the equilibrium point.

If it stretched 15 m, it would break!
 
  • #7
Delphi51 said:
Doesn't make sense to me. You have an elevator that falls 3.7 meters and then bounces back up 15 meters?


Yes it is. It takes in energy when it is being compressed, releases it when it springs back to the equilibrium point, then takes in some more as it is stretched beyond the equilibrium point.

If it stretched 15 m, it would break!

Not the spring, the elevator. How far total does the elevator travel until it comes to rest?
 
  • #8
Oh, do you mean 15 m is the answer to part D rather than C?
Certainly D could be 15 m because the elevator will go up and down quite a few times before it stops, and those up and down distances will add up.

Do you have answers for parts B and C?
 
  • #9
I guess I am wrong about that extra spring energy term. I was thinking the spring was attached to the elevator. Getting .783 for B and 2.08 for C now.
 
  • #10
B is .90 m and C is 2.8 m.
 
  • #11
Okay, found a mistake, now getting 0.898 for B and 2.74 for C.
I can rest now! Sorry if I wasted time for you.
 
  • #12
No, it's fine.
 
  • #13
Okay, I have the solution.
The two forces reducing the energy of the elevator are the spring force and the force of friction.
d) First, find the compression of the spring at which the cab is at equilibrium.
[tex]mg=kd_{eq}[/tex]
[tex]d_{eq}=\frac{mg}{k}[/tex]

So [tex]d_{eq}=[/tex] .12

Then,
[tex]mg(d+d_{eq})=\frac{1}{2}kd_{eq}^{2}+F_{k}d_{t}[/tex]
[tex] d_{t}=\frac{mg(d+d_{eq})-\frac{1}{2}kd_{eq}^{2}}{F_{k}}[/tex]
[tex] d_{t}=\frac{(1800kg)(9.8m/s^{2})(3.7m+.12m)-\frac{1}{2}(150000)(.12m)^{2}}{4400N\cdot m}[/tex]

So
[tex]d_{t}\approx 15m[/tex]
 
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Related to Conservation of Energy - Elevator Problem.

What is the concept of conservation of energy?

The concept of conservation of energy states that energy cannot be created or destroyed, but can only be transformed from one form to another. This means that the total amount of energy in a closed system remains constant.

How does the elevator problem relate to conservation of energy?

The elevator problem is a classic example used to illustrate the concept of conservation of energy. It demonstrates how energy is conserved as a person rides an elevator, as the potential energy gained by moving to a higher level is equal to the kinetic energy lost during the descent.

What are the different types of energy involved in the elevator problem?

The two main types of energy involved in the elevator problem are potential energy and kinetic energy. Potential energy is the energy an object has due to its position, while kinetic energy is the energy an object has due to its motion.

Can energy be lost in the elevator problem?

No, energy cannot be lost in the elevator problem. As the elevator moves, energy is constantly being converted from potential energy to kinetic energy and vice versa, but the total amount of energy remains constant.

How does friction affect the conservation of energy in the elevator problem?

Friction can cause some energy to be lost in the form of heat, but the total amount of energy in the system still remains constant. This means that the person in the elevator will still experience the same change in potential and kinetic energy, but some of it may be lost to friction.

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