Ring attached to elastic and inextensible strings

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Homework Help Overview

The discussion revolves around a system involving a ring attached to elastic and inextensible strings, focusing on the forces acting on the ring and the conservation of energy principles. Participants explore the implications of tension forces and energy transformations within the system.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants examine the balance of forces acting on the ring, questioning the correctness of their calculations regarding tension and resultant forces. They also explore energy conservation, discussing the relationship between elastic potential energy and kinetic energy as the ring moves.

Discussion Status

Some participants have provided guidance on the need for clearer definitions of constants and the correct application of energy equations. Multiple interpretations of the energy conservation scenario are being explored, particularly regarding the maximum height the ring can reach and the implications of negative kinetic energy.

Contextual Notes

There are indications of confusion regarding the definitions of the spring constant and the extensions of the strings involved. Participants are also grappling with the implications of their calculations on the physical behavior of the system.

songoku
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Homework Statement
Two fixed points A and B are in the same vertical line with A at a distance 2L metres above B. Small smooth ring P of mass m kg is threaded on a light elastic string of modulus of elasticity 3 mg N and natural length L metres, and both ends of the string are fixed at A. The ring P is also attached to one end of another inextensible string of length L metres with the other end fixed at B.
a. Find the tension in the string PB when the system is in equilibrium with A, P and B in the same vertical line
b. The inextensible string is being cut while the system is in equilibrium. Find in terms of g and L the speed of P just before it hits A
Relevant Equations
F = k.x

k = λ / L

λ = modulus of elasticity
k = force constant
x = change in length
L = original length
I imagine the system where P is in the middle between A and B, and P is also in the middle of light elastic string.
Between P and B, there is tension force acting downwards on P.
Between A and P, there is tension force acting upwards and because P is in the middle of the elastic string, there will be two tension forces acting upwards on P (each from half part of elastic string and the extension of each part is L/2)

a. Resultant force acting on P = 0
Tension upwards = weight + tension downwards
k.x + k.x = mg + tension downwards
( λ / L) (1/2 L) + ( λ / L) (1/2 L) = mg + tension downwards
λ = mg + tension downwards
3 mg = mg + tension downwards
tension downwards = 2mg

Is this correct?

Thanks
 
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It looks correct, but next time please post a diagram, preferably a free body diagram.
 
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Untitled.png

The left picture is how I imagine the system will be. The right picture is the free body diagram. P is the ring and the two F's is the upwards tension resulting from the ring threaded to the middle of elastic string.

For (b), I tried to use conservation of energy but failed:
Taking the initial position of P as reference point (height = 0), total energy at this point will be the same as total energy at point A after the inextensible string being cut.

elastic potential energy due to two components of elastic string = kinetic energy at A + gravitational potential energy at A (the elastic string is slack before the object reaches A so there is no elastic potential energy at A)

1/2 k x2 + 1/2 k x2 = 1/2 m v2 + mgh

1/2 (λ / L) (1/2 L)2 + 1/2 (λ / L) (1/2 L)2 = 1/2 m v2 + mgL

λL/4 = 1/2 m v2 + mgL

3mgL / 4 = 1/2 m v2 + mgL

1/2 m v2 = - 1/4 mgL

I got the kinetic energy is negative. Where is my mistake?

Thanks
 
Last edited:
songoku said:
3mgL / 4 = 1/2 m v2 + mgL
Compare the left hand side with the right hand side. The left hand side can never be equal to the right hand side because (3/4)mgL is always less than mgL even if the kinetic energy at A is zero. What does this suggest to you?
 
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kuruman said:
Compare the left hand side with the right hand side. The left hand side can never be equal to the right hand side because (3/4)mgL is always less than mgL even if the kinetic energy at A is zero. What does this suggest to you?
The maximum height P can travel is 3/4 L so it will never reach A. But how to answer question (b)? The speed of P just before it hits A is zero? Does not really make sense to me

Thanks
 
songoku said:
1/2 k x2 + 1/2 k x2
You originally wrote k=λ/L, which is correct if k is the string constant of the whole string. But in the energy expression above you need k to be the constant for only half the string.
It will be less confusing to think in terms of the energy stored in the string length L stretched to length 2L.
 
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haruspex said:
You originally wrote k=λL, which is correct if k is the string constant of the whole string. But in the energy expression above you need k to be the constant for only half the string.
It will be less confusing to think in terms of the energy stored in the string length L stretched to length 2L.

You mean the working should be like this?
1/2 k x2 = 1/2 m v2 + mgh
1/2 (λ/L) (2L)2 = 1/2 m v2 + mgL
1/2 (3mg / L) (4L2) = 1/2 m v2 + mgL
6mgL = 1/2 m v2 + mgL
1/2 m v2 = 5 mgL
v = √(10 gL)

Thanks
 
songoku said:
1/2 (λ/L) (2L)2
Not quite. The extension of the whole string is L, not 2L.
 
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haruspex said:
Not quite. The extension of the whole string is L, not 2L.
Oh yes, my bad. I will change the extension to L

Thank you very much for the help kuruman and haruspex
 

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