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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 12:39:38 IST
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Two bodies of masses m1 and m2 are initially at rest at infinite distance apart. Thay are then allowed to move towards each other under mutual gravitational attraction. What is their relative velocity of approach at a separation distance r between them?
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 12:44:41 IST
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I think 0. If they are at infinite distance, they wont come together under mutual gravitation force.
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xxxxxxxxxxxxxxx Dylan João Colaço .xxxxxxxxxxxxxx |
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 12:53:54 IST
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look force is GmM / R^2.. so potential enery is -GmM/R..at a distance R b/w them..
now velocitty gained by m1..till then by WET.. is root(Gm2/R).. similarly root(Gm1/R) for m2.....
add them u get relative velocvity of approach..
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Diamonds r formed under greatest pressures..
so r the champs.
Kriteesh..
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 16:00:51 IST
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 18:46:46 IST
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hey elastiboysai can u plz say how v vud get mu=m1.m2/m1+m2
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 18:51:53 IST
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wait i'll post the proof
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Impossible To be Impossible is Impossible |
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 18:58:18 IST
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v1 = velocity of m1 v2 = velocity of m2
conserving momentum--
m1 v1 = m2 v2 -----------1
conserving energy --
m1 v1 2 / 2 + m2 v2 2 / 2 = Gm1 m2 / r ---------2
putting value of v2 from 1 in 2 we get --
v1 2 ( m1 + m2) / m2 = 2G m2 / r
v1 = m2 [ 2G / (m1 + m2) r ]
similarly putting value of v1 from 1 in 2 we get --
v2 = m1 [ 2G / (m1 + m2) r ]
relative velocity = v1 + v2 since they are in opposite directions v r = [ 2G / (m1 + m2) r ] * (m1 + m2) = [ 2G (m1 + m2) / r ]
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Impossible To be Impossible is Impossible |
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now solve and get (relative velocity of approach)
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"I a universe of atoms.......an atom in the universe" |
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 19:02:04 IST
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oh sorry anchit...dint see you post.
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"I a universe of atoms.......an atom in the universe" |
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 19:07:12 IST
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Wait Posting the proof for reduced mass . Im posting it in a different context btw
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 19:27:04 IST
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Consider 2 blocs m1 and m2 attached to each other by a massless spring of force constant k. Supposer l is the free length of spring, consider ur system 2 b placed on x axis, with 1 mass m2 at origin. if m1 and m2 are displaced and have coordinates by x1 and x2 extension of spring= x =(x1-x2)-l --->1 now m1d2x1/dt2 =-kx m2d2x2/dt2 =kx from the abov 2,
m1m2d2(x1-x2)/dt2=-kx(m1+m2) m1m2/(m1+m2)--=y say differentiating 1 twice we get yd2x/dt2=-kx so d2x/dt2= -k/y *x here y plays the role of mass. We can straightaway use d standard equations by treating y as the mass.
I agree my proof is not rigorous. Reduced mass is just a technique . If no external force acts on the system and only internal conservative forces are in play, mechanical energy of the system will remain conserved. in such cases , u cn play wid reduced mass
The abov problem is such an example To the system of 2 masses, gravitational force between them is an internal conservative froce n u can use d same technique..
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 19:30:02 IST
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my apologies for the bad drawing
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 24 Mar 2008 20:36:17 IST
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In such problems, apply conservation of energy and momentum both
1) As here gravitational potential energy is getting converted into kinetic energy of the two bodies
2) Also the momentum is conserved and total momentum throughout the motion of the two bodies = 0 Now solve the two equations formulated as above, it will be linear equations in two variables, and its solution gives desired results.
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The most incomprehensible thing about the world is that it is
at all comprehensible. |
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