How Long Until Two Masses Collide Due to Gravity?

shakgoku
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1.The question
Two point masses m_{1} and m_{2} are initially at rest. Distance between them is 'd'. How much time does it take for them to collide due to mutual gravitational attraction?2. Relavant Equations:
F = \frac{Gm_{1}m_{2}}{r^2} \<br /> <br /> \mu = \frac{m_{1}m_{2}}{m_{1}+m_{2}}Attempt at a solution:
3. force is varying with time. My first guess is to try to solve the differential equation
\mu \frac{d^2x}{dt^2} = F(x)
and tried to solve it for x(t)
But , was not successful so far. There should be a better approach..
 
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hi shakgoku! :wink:

that should work …

show us how far you got :smile:
 
tiny-tim said:
hi shakgoku! :wink:

that should work …

show us how far you got :smile:

Hello tiny tim! This is how I proceeded,

\mu \frac{d^2x}{dx^2} = - \frac{Gm_{1}m_{2}}{x^2} <br /> \\
.

.<br /> -\mu \frac{x^2}{Gm_{1}m_{2}} = \frac{d^2t}{dx^2} <br /> \\

by guess general solution will be of the form,

t = Cx^4 +C_{1} <br />.

.<br /> \frac{d^2t}{dx^2} = 12Cx^2 = -\mu \frac{x^2}{Gm_{1}m_{2}} <br />.

.<br /> <br /> C = \frac{-\mu}{12Gm_{1}m_{2}}<br /> \\<br />

And at t = 0, x = d,

C_{1} = \frac{\mu d^4}{12Gm_{1}m_{2}} <br /> <br />

..<br /> <br /> t = \frac{\mu (d^4-x^4)}{12Gm_{1}m_{2}}<br />

When the masses collide, d = 0,
using it I got,
t = \frac{d^4}{12G(m_{1}+m_{2})}\\*<br />

I doubt if my 2nd step is wrong.
 
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eugh!

you've used d2t/dx2 = 1/(d2x/dt2),

but that's not true

d2t/dx2 = d(dt/dx)/dx = 1/(dx/d(dt/dx)), and that's about as far as you can go :redface:

instead, use d2x/dt2 = dv/dt = dv/dx dx/dt = v dv/dx :smile:
 
Thanks. I had doubts but
I just got carried away because its easy to solve after making that wrong step :D

I finally made the substitution you suggested and got an integral of form

A \int_{0}^{d} \sqrt{\frac{x}{d-x}} dx =t

And I solved it to get

t = \frac{\pi d}{2} \frac{1}{\sqrt{2G(m_{1}+m_{2})d}}

Which is the answer. I throughly liked it because, \pi got involved even though point masses separated by a distance, Newton's gravitational law do not contain \pi
:)
 
π gets everywhere! :biggrin:
 
:biggrin:
I get the same answer by considering,

F = -kx

and using

k = \frac{dF}{dx}

==&gt; k = \frac{2Gm_{1}m_{2}}{x^3}

and

T = {2 \pi} \sqrt { \frac{\mu}{k}}

At

\frac{T}{4}

Collison occurs, so t = \frac{T}{4} = {\frac{\pi d}{2}}{\frac{1}{\sqrt{2G(m_{1}+m_{2})d}}} Which is same as the above answer. How does this approach work even though k is not a constant and this is not a simple harmonic motion?
Can I use this approach for any time varying force?
 
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i think it's just a coincidence :confused:
 
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