Repeated Collision: Find Minimum Mass M

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Homework Help Overview

The discussion revolves around determining the minimum mass M required for a second collision to occur between mass M and a system consisting of two masses m and a spring. The problem is set in a frictionless environment with elastic collisions, and participants are exploring the dynamics involved in these collisions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss conservation of energy and momentum, questioning how to formulate conditions for mass M to enable a second collision. There are attempts to derive equations based on the collisions and the motion of the masses involved.

Discussion Status

The discussion is active, with participants offering various equations and interpretations regarding the collisions. Some have proposed conditions for mass M, while others are clarifying the roles of the masses and the spring in the system. There is an ongoing exploration of the time between collisions and the dynamics of the system.

Contextual Notes

Participants are considering the implications of elastic collisions and the need for mass M to maintain a certain velocity after the first collision to facilitate a second collision. There are also discussions about the relevance of the center of mass frame and the conditions necessary for repeated interactions between the masses.

  • #31
haruspex said:
Typo. He meant v1=2Mv0/(M+m)
Thanks haruspex. That was a mistake in algebra, not a typo.

With this correction, the equation for δ becomes:
\delta=\frac{2Mv_0}{ω(M+m)}sin(ωt)
and
x_1(t)=\frac{Mv_0t}{(M+m)}+\frac{Mv_0}{ω(M+m)}sin(ωt)=\frac{Mv_0}{ω(M+m)}(ωt+sin(ωt))
So, if x_M=\frac{v_0(M-m)t}{(M+m)}, we get
\frac{v_0(M-m)t}{(M+m)}=\frac{Mv_0t}{(M+m)}+\frac{Mv_0}{ω(M+m)}sin(ωt)
From this, it follows that:
-mωt=Msin(ωt)
An additional relationship is required if M barely catches up with m for a second time. This is that the velocities must match.
\frac{v_0(M-m)}{(M+m)}=\frac{Mv_0}{(M+m)}+\frac{Mv_0}{(M+m)}cos(ωt)
From this, it follows that
-m=Mcos(ωt)
The angle we're looking for is in the third quadrant where cosine and sine are both negative. So, sin(ωt)=-\sqrt{1-(\frac{m}{M})^2}
This is sufficient to solve for the value of M/m that makes good on both these equations.

Chet
 
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  • #32
Actually, I didn't want to bring this up, but you're still wrong as far as I am concerned. Recheck your algebra. I have checked my calculations numerous times and v1 = Mv0/(m+M) not 2Mv0/(m+M).
 
  • #33
Adding that latter condition, I finally obtained:
tg(x)=x
where x=wt
That gives t~4.49/w
 
  • #34
peripatein said:
Actually, I didn't want to bring this up, but you're still wrong as far as I am concerned. Recheck your algebra. I have checked my calculations numerous times and v1 = Mv0/(m+M) not 2Mv0/(m+M).
Uh Oh. I check it numerous times too, and got 2Mv0/(m+M). Here is the sequence of steps:

I started with the following:
v_M=v_0\frac{M-m}{M+m}
v_1=\frac{M(v_0-v_M)}{m}

Substituting the first equation into the second equation, I get:
v_1=\frac{Mv_0}{m}\left(1-\frac{(M-m)}{(M+m)}\right)=\frac{Mv_0}{m}\frac{(M+m)-(M-m)}{(M+m)}=\frac{Mv_0}{m}\frac{2m}{(M+m)}=\frac{2Mv_0}{M+m}
I can't see where I made a mistake.
 
  • #35
From the previous equations I presented, I get:

ωt=\sqrt{\left(\frac{M}{m}\right)^2-1}
so,
\cos\left(\sqrt{\left(\frac{M}{m}\right)^2-1}\right)=-\frac{m}{M}
This needs to be solved for m/M.
 
  • #36
I have checked mine several times as well and obtained the following:
vM = (Mv0 - 2mv1)/M
v1 = Mv0/(M+m)
Hence,
vM=v0(M-m)/(M+m)
 
  • #37
Chestermiller said:
Uh Oh. I check it numerous times too, and got 2Mv0/(m+M). Here is the sequence of steps:

I started with the following:
v_M=v_0\frac{M-m}{M+m}
v_1=\frac{M(v_0-v_M)}{m}

Substituting the first equation into the second equation, I get:
v_1=\frac{Mv_0}{m}\left(1-\frac{(M-m)}{(M+m)}\right)=\frac{Mv_0}{m}\frac{(M+m)-(M-m)}{(M+m)}=\frac{Mv_0}{m}\frac{2m}{(M+m)}=\frac{2Mv_0}{M+m}
I can't see where I made a mistake.

I get the same. peripatein, please post your calculation.
what do you mean by "sketch that"?
Sketching is not the same as solving graphically (which requires an accurate drawing).
I was trying to get you to see that the straight line representing the subsequent motion of M had to be tangential to the curve for the motion of m. This is the same as Chester's observation that the velocities must match as well as the positions, and therefore produces the same equation.
 
  • #38
I am going to leave it the way it is, so no need to repost. In any case, it doesn't matter much. The physics is the essence.
But thank you very much for your help; I am sincerely grateful! :)
 
  • #39
peripatein said:
I have checked mine several times as well and obtained the following:
vM = (Mv0 - 2mv1)/M
v1 = Mv0/(M+m)
Hence,
vM=v0(M-m)/(M+m)
The first of these equations is not consistent with the momentum balance. Where did the 2 come from? See post #6 by fightfish (which is correct).
 
  • #40
peripatein said:
Adding that latter condition, I finally obtained:
tg(x)=x
where x=wt
That gives t~4.49/w
This result for x is approximately correct. So, m/M=-cos(4.49) is the solution you have been looking for. That completes the solution.
 

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