Loop-the-loop on frictionless track, spring-powered

In summary, the toy car is shot out of a compressed horizontal spring and then travels around a loop-the-loop on a frictionless track. The energy stored in the spring is used to propel the car around the track. The car's speed is highest at point B, and it stops at point C. The energy lost to friction is determined by how much energy is stored in the spring and the friction coefficient of the track.
  • #1
fysics4liefe
3
0

Homework Statement


A toy car of mass 0.300 kg is shot out of a compressed horizontal spring (A), and then travels around a loop-the-loop along a frictionless track. The spring has a spring constant k = 900 N/m, and 3.50 J of energy was stored in the spring by compressing it.

(1) How far was the spring compressed to store 3.5 J of energy in it?
(2) What is the speed of the car as it passes point B, which is 0.400 m above point A?
(3) How high above the original position does the car go before stopping (point C)?
(4) Suppose now that the track has some friction, and that it is observed that the car's height at point C is only 80% of the height it would reach in the absence of friction (i.e. in Question #3). How much energy did friction remove on the trip from A to C?


Homework Equations


KE = (1/2)mv2
PE = mgh
PES = (1/2)kx2


The Attempt at a Solution


(1) PE = (1/2)kx2, so 3.5 = (0.5)(900)x2. Solving for x, x = 0.088. So this is the distance the spring was compressed in order to store 3.5 J.
(2) To be honest, I have attempted this about 10 different ways, none of which were correct. I believe that mgh = (1/2)mv2 could be used in some way, but am not sure of how to use this, because I don't know what the maximum height would be. (1/2)mv12 = (1/2)mv22 + mgh could be useful as well, if either velocity was known. Perhaps the velocity can be figured from the amount of energy that was stored in the spring.
(3) & (4) Without knowing the answer to #2, it is difficult/impossible to even get started on these ones. Please advise. Thank you all in advance.
 
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  • #2
(2) Another attempt... PE(spring) = PE = (1/2)mx2 ==> (1/2)(900)(0.088^2) = 3.4848. Plugging this value of PE into PE = (1/2)mv2, I get V(initial) = 4.82. Plugging this into (1/2)mV^2 = (1/2)mV^2 + mgh, I get that the velocity at the top of the ramp = 3.92 m/s. Is this sensible?
 
  • #3
fysics4liefe said:
(2) Another attempt... PE(spring) = PE = (1/2)[strike]m[/strike]kx2 ==> (1/2)(900)(0.088^2) = 3.4848. Plugging this value of PE into PE = (1/2)mv2, I get V(initial) = 4.82.
yes, this is good
Plugging this into (1/2)mVinitial^2 = (1/2)mVfinal^2 + mgh, I get that the velocity at the top of the ramp = 3.92 m/s. Is this sensible?
using h = 0.4 m, you get the velocity at that point B. To get the max height when the car stops, what is v_final and what is h at that point C?
 
  • #4
PhanthomJay said:
yes, this is good using h = 0.4 m, you get the velocity at that point B. To get the max height when the car stops, what is v_final and what is h at that point C?

Okay, got it now, thank you. So the energy at the highest point is the sum of KE + PE, which is (1/2)mv2 + mgh. Since v = 0 at the highest point, (1/2)mv^2 = 0. So kinetic energy is zero (obviously, since we aren't moving). So the total energy (which is conserved on frictionless track) is equal to the PE, mgh. (0.3 kg)(9.8 m/s^2)(h) = 3.4848. Solving for h at v=0, we get h = 1.185 meters, which is the max height (correct significant figures notwithstanding).

Which enables us to solve question 4. 80% of previous max. height is 0.952 meters, since (0.8)(1.185) = 0.952. Plugging this into mgh, we get a total PE of 2.7988 J. On frictionless track, this number was 3.4848. So, 3.488 J (frictionless energy) - 2.7988 J (energy after friction) = 0.69 J.

Does that all look sound? Thank you, PhanthomJay. It is much appreciated.
 
  • #5
Yes, looks very good!:approve:
 

1. How does a loop-the-loop on a frictionless track work?

A loop-the-loop on a frictionless track works by utilizing the principles of centripetal force and potential energy. The track is designed with a gradual slope leading into a loop, and the spring is wound up to create potential energy. This potential energy is converted into kinetic energy as the spring is released, propelling the object forward and upwards. The centripetal force from the circular motion keeps the object moving in a circular path, allowing it to complete the loop.

2. What is the purpose of a frictionless track in a loop-the-loop?

The purpose of a frictionless track in a loop-the-loop is to eliminate any external forces that could slow down or stop the object's motion. Friction is a force that opposes motion, so by removing it from the equation, the object can maintain its speed and complete the loop without any external interference.

3. How does the spring provide the necessary energy for the loop-the-loop?

The spring in a loop-the-loop is wound up, creating potential energy due to its compression. As the spring is released, this potential energy is converted into kinetic energy, which propels the object forward and upwards. This kinetic energy is what allows the object to have enough speed and momentum to complete the loop.

4. Can a loop-the-loop on a frictionless track be performed with any object?

No, not all objects can successfully complete a loop-the-loop on a frictionless track. This type of experiment requires a precise balance of forces and energy, so the object must have enough mass and speed to overcome the forces of gravity and centripetal force. Objects that are too heavy or too light may not be able to complete the loop.

5. What are the safety precautions when conducting a loop-the-loop on a frictionless track?

When conducting a loop-the-loop on a frictionless track, it is important to ensure that the track is securely anchored and that the object being used is appropriate for the experiment. Eye protection should also be worn in case of any unexpected mishaps. Additionally, the experiment should be conducted in a controlled environment with proper supervision to minimize any potential risks.

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