Can Conservation of Mechanical Energy Solve This Pulley Problem?

In summary, the conversation discusses a problem involving a system of masses connected by a light inelastic string and two pulleys. By applying the principle of conservation of mechanical energy, the system is shown to come to rest when the middle mass falls a distance of (4am1m2)/(4m1^2-m2^2). However, it is pointed out that this approach may not work and the correct solution involves finding an equation for the distance fallen, d, in terms of the distance raised, s, and the distance between the pulleys, a, using geometry.
  • #1
sr-candy
15
0

Homework Statement


A light inelastic string passes round two small smooth pulleys A and B in the same horizontal line at a distance 2a apart, and carries masses m1 at each end and a mass m2(<2m1) at its middle point. The system is released from rest with m2 at the middle point of AB

By applying the principle of conservation of mechanical energy, show that the system comes to instantaneous at rest when m2 has fallen a distance, d = (4am1m2)/(4m1^2-m2^2)
There is an original version of the question attached, check it if you can't understand what i am tring to express

Homework Equations


by consevation of energy, initial potential energy=final potential energy

The Attempt at a Solution


what i am thinking is that the distance fallen, ie. PE loss of m2 is gain and of PE of 2m1
and since both at the initial and final postion , the system is at rest so the
initial KE = Final KE = 0
But i just can't come up with the expression given by the question
 

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  • #2
I don't think you can solve this problem just using conservation of energy. At the resting position the string tensions need to balance the forces of gravity. You need to use that.
 
  • #3
thx for replying,

i am very close to the answer, but i find that there is something wrong, i don't know if it is because of my calculation or my concept

let the distance fallen of m2 be d
and the distance raised of m1 be s

by conservation of energy

m2gd = 2m1gs---------1

by Newton's second law

2m1sinA = m2----------2

d/(a+s) = sinA---------3

after i solve these three question,

i found that d = 2am1m2/(4m1^2-m2^2) (this ans times 2 = the answer required)

is it something wrong with my equations or my calculation?
 
  • #4
Oh, I see what the question is. m2 will fall and potential energy will be converted to kinetic energy, it will stop falling when the potential energy reaches the same value it started with (hence no more kinetic energy). But at this point it's not in equilibrium so it will rebound, but you don't care about that, you just want to find out where it stops. So i) the forces aren't balanced there, so your Newton's law relation is incorrect ii) PE isn't conserved, it's constantly changing. Your 'conservation of PE' relation is also incorrect, the relation between a and s is fixed by geometry. Write the total PE as 2*m1*g*s-m2*g*d. When d=0 the PE=0. Now what you want to do is find another value of d where PE=0. That will be the stopping point. So you will need to solve for s in terms of d.
 
  • #5
i am quite confuse here,

1.Isnt that your "conservation of PE" equation is exactly like mine?

m2gd = 2m1gs 2*m1*g*s-m2*g*d=02.how can i know that it will rebound, and what is providing for the upward force?
 
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  • #6
Yes, it is. And that is the equation to solve. Sorry to confuse you. I only meant to point out that 'conservation' of PE is the wrong concept. It's not conserved. The system will oscillate around the point where the forces balance between the initial point where PE is equal to 0 and another point where PE equals 0. In between, PE is not equal to 0. I think you are trying to solve the correct equation. Can you show how you got the wrong answer?
 
  • #7
sure

m2*g*d=2*m1*g*s
s=(m2*d)/(2*m1)---------1

2*m1*g*sinA=m2*g

sinA= m2/(2*m1)----------2

d/(a+s) = sinA------------3

d=a*sinA + s*sinA--------4

sub 1 and 2 into 4

d=a(m2/2m1)+(m2d/2m1)(m2/2m1)

d= (m2a/2m1)+m2^2*d/4m1^2

(4m1^2d-m2^2d)/4m1^2=m2a/2m1

d= 2am1m2/(4m1^2-m2^2)

sry the symbol and numbers may be confusing
 
  • #8
I think your force balance equation involving sin(A) is wrong. Because, like I said, when the weights become stationary, the forces aren't balanced. Just solve m2*d=2*m1*s. I may have sent you down this track by misunderstanding the problem initially. Can you find an equation for s in terms of a and d?
 
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  • #9
i can't find any equation relating s , a , d except the geometry one
 
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  • #10
sr-candy said:
i can't find any equation relating s , a , d except the geometry one

Use the geometry one. (s+a)^2=a^2+d^2. Solve for s.
 
  • #11
i am trying , but one question

if the "Newtons law" is wrong, then i can never solve sinA

that means i hv 2 equations only, equation 1 and (s+a)^2=a^2+d^2

but i have 3 unknowns s, a, d is it possible to solve them?
 
  • #12
oh, sry my mistake "a" is given
 
  • #13
problem solved, thanks a lot
 

Related to Can Conservation of Mechanical Energy Solve This Pulley Problem?

What is the definition of work?

Work is defined as the transfer of energy from one object to another by applying a force over a distance.

What is the formula for calculating work?

The formula for calculating work is W = F*d, where W is work, F is the force applied, and d is the distance over which the force is applied.

What is the difference between work and power?

Work is the transfer of energy, while power is the rate at which work is done. In other words, work is a measure of the total amount of energy transferred, while power is a measure of how quickly the energy is transferred.

How is work related to energy?

Work and energy are closely related concepts. Work is the transfer of energy, and energy is the ability to do work. Whenever work is done, energy is transferred from one object to another.

What is the principle of conservation of energy?

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

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