Conservation of energy -- Using a spring to launch a ball up an incline

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Homework Help Overview

The discussion revolves around the conservation of energy in a system involving a spring launching a ball up an incline. The original poster presents calculations for the initial and final energy states, but expresses frustration over repeated incorrect results.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the relationship between the spring constant and energy calculations, questioning the conversion of units from N/cm to N/m. There are discussions about the relevance of the incline angle and the energy lost to gravity as the ball ascends.

Discussion Status

Participants are actively engaging with the problem, offering insights about unit conversions and the implications of the incline on energy calculations. Some suggest re-evaluating the calculations and assumptions made regarding the spring's behavior and the forces acting on the ball.

Contextual Notes

There is mention of potential errors in the calculation of initial energy and the need for clarity on the incline's impact. The original poster indicates a lack of progress despite multiple attempts, highlighting the challenge of reconciling the theoretical and practical aspects of the problem.

tootired
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Homework Statement
Launcher has a spring force constant of 1.52N/cm. The surface is at an incline of 8.3 degrees.
The Spring is initially compressed 3.75 cm. Find the launching speed of the .164 kg ball when the plunger is released. A due to G is 9.8m/s^2. Friction and the plunger are negligible
Relevant Equations
Ei=Ef
Ei = 1/2 K (x)^ 2
K = .0152N/m
x = .0375 m
Ei = 1.06x10^-5

Ef= 1/2mv2 + mgh
m = .164kg, v is unknown, h is .0375sin(8.3)=.00541, Ef set equal to Ei
1.06x10^-5=1/2(.164kg)(v^2)+ (.164kg)(9.8)(.00541)
v = .3254m/s

I have gotten this answer multiple times but it is not correct. I am going a bit crazy, someone please give me clue here
 
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tootired said:
Homework Statement:: Launcher has a spring force constant of 1.52N/cm. The surface is at an incline of 8.3 degrees.
The Spring is initially compressed 3.75 cm. Find the launching speed of the .164 kg ball when the plunger is released. A due to G is 9.8m/s^2. Friction and the plunger are negligible
Relevant Equations:: Ei=Ef

Ei = 1/2 K (x)^ 2
K = .0152N/m
x = .0375 m
Ei = 1.06x10^-5

Ef= 1/2mv2 + mgh
m = .164kg, v is unknown, h is .0375sin(8.3)=.00541, Ef set equal to Ei
1.06x10^-5=1/2(.164kg)(v^2)+ (.164kg)(9.8)(.00541)
v = .3254m/s

I have gotten this answer multiple times but it is not correct. I am going a bit crazy, someone please give me clue here
Hi @tootired and welcome to PF.

You are given that k = 1.52 N/cm. This means that when you stretch the spring by 1 cm it pulls back with a force of 1.52 Newtons.

You say that k = .0152 N/m. This means that when you stretch the spring 100 times as much as before, it pulls back with a force that is 100 times less. Huh?

You need some rest because it seems you are too tired.:oldsmile:
 
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kuruman said:
Hi @tootired and welcome to PF.

You are given that k = 1.52 N/cm. This means that when you stretch the spring by 1 cm it pulls back with a force of 1.52 Newtons.

You say that k = .0152 N/m. This means that when you stretch the spring 100 times as much as before, it pulls back with a force that is 100 times less. Huh?

You need some rest because it seems you are too tired.:oldsmile:
I would agree on the rest, but not an option lately. If I do not convert N/cm to N/m the answer is still not correct. I'm all out of attempts on this one. Thank you for the insight
 
Welcome! :cool:

How is the "incline of 8.3 degrees" relevant in this problem?
Uphill, I assume.
Could you show us a diagram?

Please, read this guide about working with symbolic variables as far as possible in the calculation process:
https://www.physicsforums.com/insights/frequently-made-errors-equation-handling/

It seems that the calculated value of Ei is incorrect, but units are not shown.
Energy of the compressed spring is 10.69 N-cm.
Why don't you work with N and cm and convert at the end to m/s?
 
Last edited:
tootired said:
If I do not convert N/cm to N/m the answer is still not correct.
Not sure what you mean by that. You do need to convert at some point, but to do so correctly. You should have noticed that the expression you got for ##v^2## was negative.
In case you are still getting the conversion wrong, here's the safest way to do it. There are 100 cm per metre, so ##1.52N/cm\times 100cm/m=152N/m##. This should yield an answer about 1.09m/s.
Lnewqban said:
How is the "incline of 8.3 degrees" relevant in this problem?
Because as post #1 working shows, some energy is used in raising the ball to the point where it leaves the spring. The angle is needed to find the height gain.
 
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The ball will lose contact at a point where its acceleration is zero. That point is the equilibrium position of the inclined spring-mass system which occurs where the spring is compressed by ##x_{\text{eq}}=mg\sin\!\theta/k##. If we assume that the given ##x_0=3.75## cm is the compression from the relaxed length of the spring, the energy conservation equation in the form ##\Delta U+\Delta K=0## would be $$\frac{1}{2}k\left(x_{\text{eq}}^2-x_0^2 \right)+mg\sin\!\theta(x_{\text{eq}}-x_0)+\frac{1}{2}m\left(v^2-0\right)=0.$$In this case, the incline angle is small and ##x_{\text{eq}}=0.15## cm or 4% of ##x_0##. This may or may not be sufficient to push the approximate solution with ##x_{\text{eq}}=0## beyond the tolerance of the scoring algorithm.
 
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kuruman said:
The ball will lose contact at a point where its acceleration is zero.
No, the spring, being ideal, will expand as fast as necessary to maintain contact until it reaches its relaxed length. At some point before that the force it exerts on the ball will be insufficient to overcome gravity, so the ball reaches its maximum speed there, but that does not alter the correctness of the energy calculation for the speed at the moment contact is lost.
 
haruspex said:
No, the spring, being ideal, will expand as fast as necessary to maintain contact until it reaches its relaxed length.
Indeed. I was thinking of the other problem with two separate masses one of which is attached to the spring and the other buting against the first mass.
 

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