The Student Room Group
Reply 1
Elastic collision means energy is conserved
so12Mu2=12Mv12+12mv22 \frac{1}{2}Mu^2 = \frac{1}{2}Mv_1^2 +\frac{1}{2}mv_2^2

momentum consideration gives:
Mu=Mv1+mv2 Mu = Mv_1 + mv_2

Rearrange the momentum equation to get v1 in terms of u and v2. then use the energy equation to eliminate v1 from the system.
Reply 2
It's been a while since I did collisions but.... since its elastic then e=1.

Mu=MV1+mV2

V1=(Mu-mV2)/M

e = Seperation /apprach

So 1 = (V2 - ((Mu-mV2)/M) /u

u = (MV2-Mu+mV2)M

Mu = MV2-Mu+mV2

MV2+mV2 = 2Mu

V2 = (2Mu/M+m)


And you just factorise and take the u out.
Reply 3
In your first equation you did Mu+m....the seconf object is stationary so its momentum is 0, its just Mu not Mu +m...
So before the collision, energy and momentum of the system is:

E=12Mu2 E = \frac{1}{2} M u^2
P=Mu P = Mu

After the collision, the mass M now has velocity v_1 and the mass it hit, m, has velocity v_2:

E=12Mv12+12mv22 E = \frac{1}{2} M v_1^2 + \frac{1}{2} m v_2^2
P=Mv1+mv2 P = Mv_1 + mv_2

Equating this two equations together before and after the collision since the collision is elastic:

Mu=Mv1+mv2v1=Mumv2M Mu = Mv_1 + mv_2 \to v_1 = \frac{Mu-mv_2}{M}
Mu2=Mv12+mv22Mu2=M[Mumv2M]2+mv22 Mu^2 = Mv_1^2 + mv_2^2 \to Mu^2 = M\left[\frac{Mu-mv_2}{M}\right]^2 + mv_2^2 ---- (1)

expanding out the bracket:
M[Mumv2M]2=Mu22muv2+m2v22MM\left[\frac{Mu-mv_2}{M}\right]^2 = Mu^2 - 2muv_2 + \frac{m^2 v_2^2}{M}
So eq (1) becomes:

Mu2=Mu22muv2+m2v22M+mv22v2=2MuM+m Mu^2 = Mu^2 - 2muv_2 +\frac{m^2 v_2^2}{M} +mv_2^2 \to v_2 = \frac{2Mu}{M+m}

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