Determine what the speed v of the bullet should be such that the rod swings exactly 90 degrees from it's initial equilibrium position. Express v in terms of m, M, g and L. Picture to come:
Well, lost kinetic energy can be converted to rotational energy, right?
So what I tried was two ways. 1) Assuming it's a perfectly inelastic collision this would imply that kinetic energy is conserved. so \(KE_{bullet}=\frac{1}{2}mv^2\) and \(KE_{rod}=\frac{1}{2}I\omega^2\) where \(I=\frac{1}{3}ML^2\). \[KE_{before}=KE_{after}\] \[\frac{1}{2}mv_i^2 + \frac{1}{2}Iw_i^2=\frac{1}{2}mv_f^2 + \frac{1}{2}Iw_f^2\] KE of rod before is 0, and velocity of bullet after is \(\large \frac{v_i}{2}\) \[\frac{1}{2}mv_i^2=\frac{1}{2}m\frac{v_i^2}{4} + \frac{1}{2}Iw_f^2\]We can take out a factor of 1/2. and rearrange \[mv_i^2-\frac{1}{4}mv_i^2 = Iw_f^2\]\[mv_i^2(1-\frac{1}{4})= Iw_f^2\]\[\frac{3}{4}mv_i^2 = \frac{1}{3}ML^2w_f^2\] If we let \(w_f=\sqrt{\frac{g}{L}}\) <- not sure about this part \[v_i^2=\frac{4MLg}{9m}\]
Do you know the answer?
Nope, which is why I was trying to verify my answer from my last post.
Well, we can use the last post, and just put \(\theta = 90^\circ\)
\[ \frac 12 LMg = \frac 16L^2M\omega ^2 \]
\[ \omega ^2=\frac{3g}{L} \]
That hasn't verified anything... has it? that just says we need a angular velocity of that much to get to 90.
Wait, how did you get that equation?
which one?
\[\frac 12 LMg = \frac 16L^2M\omega ^2\]
Left side is potential, right side is kinetic rotational
Ah yeah I see. Okay that works.
\[ mv^2 =\frac 14mv^2+I\omega ^2 \implies \frac 34mv^2 = I\omega^2 \]
\[ v^2 = 4\frac{Ig}{mL} \]
\[ v = \sqrt{\frac{4MLg}{3m}} \]
A lot of algebra and places that mistakes could have been made.
But you've assumed \(w=\sqrt\frac{g}{L}\) - but shouldn't you be proving your \(w=\frac{3g}{L}\)
The point of the other question was to prove that.
I see what you did. So what I did was wrong in my first post was assuming \(w=\sqrt{\frac{g}{L}}\) when it should be assumed to be the w you need to reach 90 degrees \(\omega^2=\frac{3g}{L}\). And then from conservation of kinetic energy \[\frac{3}{4}mv^2=I\omega^2\] we find the equation for v \[v^2=\frac{4I\omega^2}{3m}=\frac{4ML^2(3g)}{9m(L)}=\frac{4MLg}{3m}\] \[v=\sqrt{\frac{4MLg}{3m}}\]
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