How to Find the Reaction Force in a Falling Rope Problem?

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Homework Help Overview

The problem involves a uniform rope of mass M and length a, initially held at rest and then released, leading to a discussion on the reaction force exerted by the support as the rope falls. The context includes concepts of energy conservation and dynamics related to changing mass during motion.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the changing mass of the moving portion of the rope and its implications for momentum calculations. There are questions about differentiating velocity to find acceleration and how to express dp/dt in terms of the variables given. Some participants suggest plugging in specific values for R to explore the second part of the problem.

Discussion Status

The discussion is active with participants exploring various approaches to the problem. Some guidance has been offered regarding the treatment of mass and momentum, and there is a recognition of the need to derive expressions based on the given relationships. Multiple interpretations of how to proceed with the calculations are being explored.

Contextual Notes

Participants are navigating the complexities of a non-constant mass system and the implications for momentum and reaction forces. There is a specific condition noted regarding the support collapsing if the reaction force exceeds 3/2Mg, which is central to the problem's exploration.

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Homework Statement



A uniform rope of mass M and length a is held at rest with its two ends close together and the rope hanging symmetrically below.((in this position, the rope has two long vertical segments connected by a small curved segment at the bottom.) One of the ends is then released. It can be shown by energy conservation that the velocity of the free end when it has descended by a distance x is given by

v^2= (x(2a-x))g/(a-x)

Find the reaction R exerted by the support at the fixed end when the free end has descended a distance x. The support will collapse if R exceeds 3/2Mg. Find how far the free end will fall before this happens.



Homework Equations



dp/dt= Mg-R, dp/dt is change in momentum and R is the reaction force.

The Attempt at a Solution



Mass of moving rope is changing. At rest, T=0 . When rope is release T=1/2*Mv^2 and V= Mghr+Mghl.

hl=x, hr=1/2(a-x)

R=Mg-dp/dt

should I differentiate v^2 in order to obtain dv/dt and then should I proceed to multiply dv/dt by M in order to get dp/dt. Now that I have dp/dt I can calculate the R now right?
 
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Any body not understand my solution or the problem ?
 
The mass of the moving portion of the rope is not constant. Therefore,

p = mv

dp/dt = mdv/dt +vdm/dt

m = density*length = M/L*x

dm/dt = M/L*dx/dt = M/L*v

vdm/dt = v*M/L*v = M/L*v2

Your were given v2 in terms of x so dv/dt can be found. Therefore, dp/dt can be found as a function of x.
 
chrisk said:
The mass of the moving portion of the rope is not constant. Therefore,

p = mv

dp/dt = mdv/dt +vdm/dt

m = density*length = M/L*x

dm/dt = M/L*dx/dt = M/L*v

vdm/dt = v*M/L*v = M/L*v2

Your were given v2 in terms of x so dv/dt can be found. Therefore, dp/dt can be found as a function of x.

For the second part of the problem , should I plug in R= 3/2Mg and solved for x?
 
Yes, your approach to the second part of the problem is correct.
 
chrisk said:
Yes, your approach to the second part of the problem is correct.

Not sure how to solve for x:

Last part of my second solution: 6*a=(2a^2-2ax-3x^2)/(a-x)
 
Multilply both sides of the equation by (a - x), distribute this factor on the left side of the equation with 6a. Then move all terms to one side thus setting one side equal to zero. This will give a quadratic equation in x equal to zero. Solve for x using the quadratic formula or completing the square.
 

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