"Solving Rope Through a Hole Physics Problem

[Saitama]

Homework Statement

A rope of mass M and length ##l## lies on a friction less table, with a short portion, ##l_0## hanging through a hole. Initially the rope is at rest.

a. Find a general solution for x(t), the length of rope through the hole.

(Ans: ##x=Ae^{\gamma t}+Be^{-\gamma t}##, where ##\gamma^2=g/l##)

b. Evaluate the constants A and B so that the initial conditions are satisfied.

Homework Equations

The Attempt at a Solution

The forces acting on the rope are weight and tension (T) due to the part of rope on the table. If x is the length of rope hanging, l-x is the length of rope on the table. Let ##\lambda## be the mass per unit length of rope.
Newton's second law for hanging part,
$$\lambda xg-T=\lambda xa$$
Newton's second law for rope on table,
$$T=\lambda (l-x)a$$
From the two equations,
$$a=\frac{gx}{l+2x}$$
I can substitute a=d^2x/dt^2 but Wolfram Alpha gives no solution for this.

Any help is appreciated. Thanks!

 

[Chestermiller]

Homework Statement

A rope of mass M and length ##l## lies on a friction less table, with a short portion, ##l_0## hanging through a hole. Initially the rope is at rest.

a. Find a general solution for x(t), the length of rope through the hole.

(Ans: ##x=Ae^{\gamma t}+Be^{-\gamma t}##, where ##\gamma^2=g/l##)

b. Evaluate the constants A and B so that the initial conditions are satisfied.

Homework Equations

Hi Pranav-Arora. Check your algebra. You made a mistake. It should be la=xg.

The Attempt at a Solution

The forces acting on the rope are weight and tension (T) due to the part of rope on the table. If x is the length of rope hanging, l-x is the length of rope on the table. Let ##\lambda## be the mass per unit length of rope.
Newton's second law for hanging part,
$$\lambda xg-T=\lambda xa$$
Newton's second law for rope on table,
$$T=\lambda (l-x)a$$
From the two equations,
$$a=\frac{gx}{l+2x}$$
I can substitute a=d^2x/dt^2 but Wolfram Alpha gives no solution for this.

Any help is appreciated. Thanks!

Hi Pranav-Arora. Your formulation is correct, but check your algebra. It should be la=xg.

 

[Saitama]

Hi Pranav-Arora. Your formulation is correct, but check your algebra. It should be la=xg.

Oh yes, sorry about that. Thanks a lot!

At t=0, ##x(0)=l_0##, x'(0)=0
##x(0)=A+B=l_0##

Since ##x'(t)=A\gamma e^{\gamma t}-B\gamma e^{-\gamma t}\Rightarrow x'(0)=0=A-B##
Solving the two equations, ##A=B=l_0/2##.
Hence,
$$x(t)=\frac{1}{2}\left(l_0e^{\gamma t}+l_0e^{-\gamma t}\right)$$
Looks good?

 

[janhaa]

It can be solved this way too, by Newton's second law :

[tex]F=Ma=\rho g x A[/tex]

[tex]M\frac{d^2x}{dt^2}=\rho g x A[/tex]

[tex]M\frac{d^2x}{dt^2}=\frac{M}{l^3} g x l^2[/tex]

[tex]\frac{d^2x}{dt^2}=\frac{gx}{l} [/tex]

and the solution of this DE is

[tex]x(t)=x=A\cdot exp(\sqrt{\frac{g}{l}}t)+B\cdot exp(-\sqrt{\frac{g}{l}}t)[/tex]

same as yours...

 

[Saitama]

@janhaa: What are ##\rho## and ##A##?

 

[janhaa]

@janhaa: What are ##\rho## and ##A##?

[tex]\rho[/tex] is density
and
[tex]A: area = l^2[/tex]