Max Theta for Block and Rod System

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The discussion revolves around finding the maximum angle theta for a block and rod system using different methods. The first method, based on conservation of energy, fails due to the inelastic nature of the collision between the block and the rod. The second method attempts to apply torque and angular momentum but confuses the integration of torque with work, leading to incorrect results. Participants clarify that the correct approach involves determining the speed and energy of the system immediately after the collision, followed by calculating how high it rises. The conversation highlights the importance of correctly applying conservation principles in inelastic collisions.
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Homework Statement


11-56.gif


Find the maximum theta given that
h (initial height of block)
m (mass of block)
M (mass of rod)
L (length of rod)

Homework Equations





The Attempt at a Solution



I did it three different ways and none of them worked. What is wrong with these ideas?

Method 1: Potential Energy

The gravitational potential energy of the block and rod's center of mass must be equal before and after since initially and finally, the system has no kinetic energy

U_{blocki} + U_{rodi} = U_{blockf} + U_{rodf}

mgh + Mg\frac{L}{2} = mg(L-L\cos\theta) + Mg(L-\frac{L}{2}\cos\theta)

mh + \frac{ML}{2} = mL(1-\cos\theta) + \frac{ML}{2}(1+1-\cos\theta)

mh + \frac{ML}{2} = mL(1-\cos\theta) + \frac{ML}{2} + \frac{ML}{2}(1-\cos\theta)

mh = (mL + \frac{ML}{2})(1-\cos\theta)

\cos\theta = 1 - \frac{mh}{mL + \frac{ML}{2}}



Method 2: Torque

The velocity of the block at the bottom of the ramp is
v = \sqrt{2gh}

The angular momentum of the system is the angular momentum of the block just before it hits (since the rod is at rest)

l = I\omega = (mL^2)(\frac{v}{L})

l = mL\sqrt{2gh}

Gravity provides torque which changes the angular momentum from that quantity down to zero, so

I found the torque of the block and the rod separately and added them together
\tau_{block} = r \times F = L(mg)\sin\theta

\tau_{rod} = r \times F = \frac{L}{2}(Mg)\sin\theta

mL\sqrt{2gh} = \int_0^{\theta_{max}} \tau d\theta

mL\sqrt{2gh} = \int_0^{\theta_{max}} (Lmg+\frac{LMg}{2})\sin\theta d\theta

m\sqrt{2gh} = (mg + \frac{Mg}{2})(1-\cos\theta_{max})

\cos\theta_{max} = 1 - \frac{m\sqrt{2gh}}{mg + \frac{Mg}{2}}


Why aren't they the same?
 
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I didn't check your solutions in detail, but your Method 1 assumes conservation of energy. But that collision of block with rod looks like an inelastic collision to me.
 
Ah yes, that makes complete sense
Now I understand why the energy conservation method didn't work through the inelastic collision.

The second method uses torque and conservation of angular momentum. It should work in an inelastic collision yet it doesn't :(
 
chickendude said:
The second method uses torque and conservation of angular momentum. It should work in an inelastic collision yet it doesn't :(
It's not clear to me what you're doing by integrating torque with respect to theta. That gives the work done, not the change in angular momentum! If you do this right, it will work. (You're mixing this up with angular impulse, which is torque*time, not torque*theta.)

But it's much easier than all that. First find the speed and thus energy of the block+rod system immediately after the collision. (What's conserved during the collision?) Then figure out how high it rises. (What's conserved after the collision?)
 
ah, yes, I just got it through that method.Yeah, I confused angular impulse with work.
When we were doing linear momentum and impulse, I would make that mistake as well (integrate with respect to x rather than t), but now I see the problem.

Thanks a lot!
 
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