momo1111
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Homework Statement
[itex]2[/itex] masses connected with a solid rod .distace between them is [itex]2L[/itex] ,
total mass is [itex]M[/itex] .
[itex]B[/itex] total mass is [itex]m[/itex] ,length [itex]L[/itex] can freely move between [itex]A[/itex] and [itex]A'[/itex]
on flat and frictionless surface. all collisions are elastic.
at the beginning [itex]B[/itex] was stuck to [itex]A[/itex] and all the system was moving to the right ,[itex]v_0[/itex] and kinetic energy [itex]T_0[/itex] .
at some moment ,explosion take place and the system get additional kinetic energy [itex]T[/itex] .
1.what is the velocity of [itex]B[/itex] ,[itex]v_B[/itex] as function of [itex]v_0,T,m,M[/itex] ?
2.what is the velocity of [itex]A+A'[/itex] ,immediately after the explosion ?
3.what is the relation between [itex]T_0[/itex] and [itex]T[/itex] ,if [itex]A[/itex] don't move to the left ?
4.after the explosion [itex]B[/itex] start to move between [itex]A[/itex] and [itex]A'[/itex],what is the time between the
collision of [itex]B[/itex] with [itex]A[/itex] , and the collision between [itex]B[/itex] and [itex]A'[/itex] ?
Homework Equations
The total kinetic energy (in the lab frame) is :
[itex]K = K_{cm} +\frac{1}{2} \sum_{n=0}^N m_i (v'_i)^2[/itex]
The Attempt at a Solution
before the explosion:
[itex]T = \frac{1}{2}(M+m)v_{cm}^2 + 0 +0[/itex] ,given [itex]v_0 = v_{cm}\hat x[/itex] we get [itex]T = \frac{1}{2}(M+m)v_0^2 + 0 +0[/itex]
after :
[itex]T+ T_0 = \frac{1}{2}(M+m)v'^2_{cm} + \frac{1}{2}Mv'^2_A +\frac{1}{2}mv'^{2}_B[/itex]
or
[itex] \frac{1}{2}(M+m)v_0^2+ T_0 = \frac{1}{2}(M+m)v'^2_{cm} + \frac{1}{2}Mv'^2_A +\frac{1}{2}mv'^{2}_B[/itex]
[itex]v'_{cm}[/itex] = is the velocity of center of mass after the explosion ..so it move the same velocity
as before ,which mean - [itex]v'_{cm} = v_0[/itex] .
so we get :
(1) [itex]0 = Mv'_A +mv'_B[/itex] - momentum
(2) [itex]T_0 = \frac{1}{2}Mv'^2_A +\frac{1}{2}mv'^{2}_B[/itex]
i get that if
[itex]m - \frac{m^2}{M} > 0[/itex] then [itex]v'_B = \pm\sqrt{\frac{2T_0}{m - \frac{m^2}{M} }}\hat x'[/itex]
and [itex]v_B = v_0 \hat x+ ( \pm\sqrt{\frac{2T_0}{m - \frac{m^2}{M} }}) \hat x[/itex]Q:
1. is this the solution ?
2.if 1 is o.k then [itex]v_b[/itex] ...easy
3 - what it means "move to the left " ? ...at c.m reference system ,it`s look to me that 2 masses can't move
to the same direction ,do they ? if so , (1) - wrong solution .
any way don't have a clue ..
4.??