A mass hits other two, one on top of the other

[Karol]

Homework Statement

[/B]
Mass m is raised to height h and released. it hits, elastically, mass M which is on a surface with friction coefficient μ₁. mass m, same as the first, lies on top of M. the coefficient between them is μ₂.
1) What's the box's velocity just before the hit
2) What is the tension T₁ in the rope immediately after releasing
3) What is the tension T₂ in the rope just before the hit
4) What is M's acceleration immediately after the hit
5) What is m's acceleration (the box on top) immediately after the hit
6) How much time M travels till it stops
7) Draw on one coordinate system M and m's velocities till they halt, relative to the floor
8) What distance M travels till it halts
9) What should be the minimal length of M so that m won't fall

Homework Equations

Potential energy of height: ##EP=mgh##
Kinetic energy: ##EK=\frac{1}{2}mv^2##
Conservation of momentum: ##m_1v_1+m_2v_2=m_1v_1'+m_2v_2'##
Acceleration, distance and speed in constant acceleration: ##V^2=V_0^2+2ax##
Centripetal force: ##F_c=\frac{mv^2}{r}##

The Attempt at a Solution

Height transformed into speed:
$$mgh=\frac{1}{2}mv^2~~\rightarrow~~v_2=2gh$$
Tension before release:
$$T_1=mg\cos\alpha=mg\frac{l-h}{l}$$
Tension before hit:
$$F_c=\frac{mv^2}{r}~~\rightarrow~~T_2=m\left[ \frac{v^2}{l}+g \right]=mg\left( \frac{2h}{l}+1 \right)$$
Conservation of momentum and energy, V is M's velocity:
$$\left\{ \begin{array}{l} \frac{1}{2}mv^2=\frac{1}{2}\left[ mv_1^2+MV_0^2 \right] \\ mv=MV_0-mv_1 \end{array}\right.$$
$$\rightarrow V_0=\frac{m\sqrt{2gh}\left[ M+\sqrt{M(2M+m)} \right]}{M(M+m)}$$
M's acceleration after the hit:
$$(M+m)g\mu_1+mg\mu_2=Ma_1~~\rightarrow~~a_1=\frac{g\left[ (M+m)\mu_1+m\mu_2 \right]}{M}$$
m's acceleration after the hit:
$$mg\mu_2=ma_2~~\rightarrow~~a_2=g\mu_2$$
The time till equality of velocities is t₁:
$$V_0-a_1t_1=a_2t_1:~~V_0-\frac{(M+m)\mu_1+m\mu_2}{M}gt_1=g\mu_2t_1$$
$$\rightarrow t_1=\frac{MV_0}{(M+m)(\mu_1+\mu_2)g}$$
Their common velocity, after time t₁:
$$V_2=a_2t_1=g\mu_2\frac{MV_0}{(M+m)(\mu_1+\mu_2)g}=\frac{MV_0\mu_2}{(M+m)(\mu_1+\mu_2)}$$
When they move at one velocity, their common deceleration a₃ is (f=friction force):
$$f=(M+m)a_3~~\rightarrow~~(M+m)g\mu_1=(M+m)a_3~~\rightarrow~~a_3=g\mu_1$$
Time till both stop t₂:
$$0=V_2-a_3t_2: ~~\frac{MV_0\mu_2}{(M+m)(\mu_1+\mu_2)}=g\mu_1t_2$$
$$\rightarrow t_2=\frac{MV_0\mu_2}{(M+m)(\mu_1+\mu_2)\mu_1g}$$
Total time to full stop:
$$t_{tot}=t_1+t_2=\frac{MV_0}{(M+m)(\mu_1+\mu_2)g}\left( 1+\frac{\mu_2}{\mu_1}\right)$$
The graph:

to check which line is more inclined, i compare a₁ to a₃:
$$a_1=\frac{g\left[ (M+m)\mu_1+m\mu_2 \right]}{M}=\left[ \frac{M+m}{M}\mu_1+\frac{m}{M}\mu_2 \right]g>a_3=\mu_1g$$
The distance M travels till equality of velocities: ##V_2^2=V_0^2-2a_1x_1##
$$\frac{\mu_2^2M^2V_0^2}{(M+m)^2(\mu_1+\mu_2)^2}=V_0^2-2\frac{g\left[ (M+m)\mu_1+m\mu_2 \right]}{M}X_1~~\rightarrow~~x_1=...$$
The distance M travels from the equality till it stops: ##0=V_2^2-2A_3x_2##
$$0=V_0^2-2g\mu_1x_3~~\rightarrow~~x_2=...$$
$$x_{tot}=x_1+x_2$$
But the expressions are complicated.
The time till M stops:
M's absolute velocity+m's relative velocity yields m's absolute velocity: $$V_{M(abs)}+v_{m(rel)}=v_{m(abs)}$$
$$\rightarrow~v_{m(rel)}=v_{m(abs)}-V_{M(abs)}=a_2t-(V_0-a_1t)=g\mu_2t-\left( V_0-\frac{(M+m)\mu_1+m\mu_2}{M}gt \right)$$
By equating ##v_{m(rel)}## to 0 i find t, the time till m stops (equal velocities):
$$v_{m(rel)}=0~~\rightarrow~~t=\frac{MV_0}{g[(M+m)(\mu_1+\mu_2)]}$$
The distance traveled by m: ##x_1=\frac{1}{2}a_{m(rel)}t^2##:
$$a_{m(rel)}=a_{m(abs)}-V_0=g\mu_2-\frac{(M+m)\mu_1+m\mu_2}{M}g=\frac{(M-m)\mu_2-(M+m)\mu_1}{M}g$$
The distance x₁ involves the square of the above t, and it's only a part of the total distance M travels. the second part, x₂, from ##0=V_2^2-2a_3x_2##
It's tiring, maybe there's a simpler way, for some of the stages?

 

[rpthomps]

It would appear from the diagram that you would need to express the height of the mass on the string in terms of alpha.

 

[Karol]

can someone else have a look?

 

[haruspex]

Your expression for V₀ is wrong. It should be much simpler.

 

[Karol]

Momentum ##P=mv=m\cdot EK=m\cdot EP## in our case:
$$\left\{ \begin{array}{l} mgh=\frac{1}{2}\left[ mv_1^2+MV_0^2 \right] \\ m\cdot mgh=MV_0-mv_1 \end{array}\right.$$
But that still gives a complicated V₀.

 

[Karol]

I don't see which other principles i can use except for conservation of momentum and energy in order to find V₀

 

[Karol]

The COM velocity:
$$V_c=\frac{m_1v_1+m_2v_2}{m_1+m_2}$$
In our case:
$$V_0=2V_c=\frac{2m\sqrt{2gh}}{M+m}$$
Is the rest O.K.?
Their common velocity, after time t1:
$$V_2=\frac{MV_0\mu_2}{(M+m)(\mu_1+\mu_2)}=\frac{2Mm\sqrt{2gh}}{(M+m)^2(\mu_1+\mu_2)g}$$
Time till both stop t2:

 

[haruspex]

The COM velocity:
$$V_c=\frac{m_1v_1+m_2v_2}{m_1+m_2}$$
In our case:
$$V_0=2V_c=\frac{2m\sqrt{2gh}}{M+m}$$
Is the rest O.K.?

Yes, that all looks good except I did not check the part after "but the expressions are still complicated". I assume from there you are answering (9), since you already have the answers for all the other parts. For part (9), you know the initial relative velocity, V₀, the final relative velocity, 0, and the relative acceleration, a₁+a₂. You can get the relative distance straight from those.

 

[Karol]

Total time to full stop:
$$t_{tot}=t_1+t_2=\frac{MV_0}{(M+m)(\mu_1+\mu_2)g}\left( 1+\frac{\mu_2}{\mu_1}\right)$$
The expressions for the distances M travels till stop: x₁ and x₂ are very tiring.
m's relative acceleration, i found in post #1, is:
$$a_{m(rel)}=a_{m(abs)}-a_M=g\mu_2-\frac{(M+m)\mu_1+m\mu_2}{M}g=\frac{(M-m)\mu_2-(M+m)\mu_1}{M}g$$
M's minimal length x:
$$0=V_0^2-2a_{m(rel)}\cdot x~~\rightarrow~~x=\frac{V_0^2}{2a_{m(rel)}}$$
$$x=\frac{2M^2m\sqrt{2gh}}{[(M-m)\mu_2-(M+m)\mu_1](M+m)2g}$$

 

[haruspex]

Total time to full stop:
$$t_{tot}=t_1+t_2=\frac{MV_0}{(M+m)(\mu_1+\mu_2)g}\left( 1+\frac{\mu_2}{\mu_1}\right)$$
The expressions for the distances M travels till stop: x₁ and x₂ are very tiring.
m's relative acceleration, i found in post #1, is:
$$a_{m(rel)}=a_{m(abs)}-a_M=g\mu_2-\frac{(M+m)\mu_1+m\mu_2}{M}g=\frac{(M-m)\mu_2-(M+m)\mu_1}{M}g$$
M's minimal length x:
$$0=V_0^2-2a_{m(rel)}\cdot x~~\rightarrow~~x=\frac{V_0^2}{2a_{m(rel)}}$$
$$x=\frac{2M^2m\sqrt{2gh}}{[(M-m)\mu_2-(M+m)\mu_1](M+m)2g}$$

I thought you calculated the two absolute accelerations with opposite directions as positive, so isn't the relative acceleration the sum, not the difference?

 

[Karol]

$$a_{m(rel)}=a_{m(abs)}-a_M=g\mu_2-\left( -\frac{(M+m)\mu_1+m\mu_2}{M}g \right)=\frac{(M+m)(\mu_1+\mu_2)}{M}g$$
$$0=V_0^2-2a_{m(rel)}\cdot x~~\rightarrow~~x=\frac{V_0^2}{2a_{m(rel)}}=\frac{4Mm^2gh}{(M+m)^3(\mu_1+\mu_2)g}$$

 

[haruspex]

$$a_{m(rel)}=a_{m(abs)}-a_M=g\mu_2-\left( -\frac{(M+m)\mu_1+m\mu_2}{M}g \right)=\frac{(M+m)(\mu_1+\mu_2)}{M}g$$
$$0=V_0^2-2a_{m(rel)}\cdot x~~\rightarrow~~x=\frac{V_0^2}{2a_{m(rel)}}=\frac{4Mm^2gh}{(M+m)^3(\mu_1+\mu_2)g}$$

Looks right. You can cancel the 'g's.
Note that as M tends to zero, x tends to zero. That is clearly not right in practice. Do you see why the discrepancy?

 

[Karol]

Note that as M tends to zero, x tends to zero. That is clearly not right in practice. Do you see why the discrepancy?

$$a_M=\frac{(M+m)\mu_1+m\mu_2}{M}g$$
When M diminishes a_M increases and makes x smaller. it happens in reality, why do you say it's not right in practice?

 

[haruspex]

$$a_M=\frac{(M+m)\mu_1+m\mu_2}{M}g$$
When M diminishes a_M increases and makes x smaller. it happens in reality, why do you say it's not right in practice?

It certainly strikes me as weird that making M massless means that the mass m resting on it would stay with it. The explanation is that in reality the swinging mass m does not cease to exist as soon as it strikes M. By pretnding that it does, M retains no momentum/energy and immediately comes to a stop because of the friction. In practice, the swinging m would keep pushing it along.

 

[Karol]

So a_M becomes smaller also by the same explanation, that M retains less momentum/energy?
And:
$$a_M=\frac{(M+m)\mu_1+m\mu_2}{M}g$$
Describes what really happens until M tends to zero, only then the swinging mass would continue pushing it, right?

 

[haruspex]

So a_M becomes smaller also by the same explanation, that M retains less momentum/energy?
And:
$$a_M=\frac{(M+m)\mu_1+m\mu_2}{M}g$$
Describes what really happens until M tends to zero, only then the swinging mass would continue pushing it, right?

If m > M then swinging m will continue moving forwards, but initially more slowly than M. But M is being decelerated by friction, while the swinging m is not, so might catch up and strike M again. In the extreme case, a very light M is arrested almost immediately, so effectively coalesces with the swinging m.

 

[Karol]

Thank you very much Haruspex and rpthomps.