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Mathematics 8 Online
OpenStudy (anonymous):

A cubical block of side "a" is moving with velocity v on a horizontal smooth plane. It hits a ridge at point O. Find the angular speed of the block after it hits the point O. Please view the attached image for more details

OpenStudy (anonymous):

This is the attached diagram

OpenStudy (anonymous):

So this thing is just heading towards O which then acts as a point of rotation?

OpenStudy (anonymous):

Yes

OpenStudy (anonymous):

Okay...I just to do something, then I'll take a look.

OpenStudy (anonymous):

*just go to do something*

OpenStudy (anonymous):

Okay, I will be waiting

OpenStudy (anonymous):

Still waiting?

OpenStudy (anonymous):

Yes

OpenStudy (anonymous):

I'm thinking you can attack the problem by considering conservation of energy, assuming only internal, conservative forces are acting.

OpenStudy (anonymous):

You have two regimes - translational (before the ridge), then rotational.

OpenStudy (anonymous):

The kinetic energy of the block before hand is \[K_i=\frac{1}{2}Mv^2\]

OpenStudy (anonymous):

The kinetic energy of the block just after impact, as it enters the rotational regime, is\[K_f=\frac{1}{2}I \omega^2\]

OpenStudy (anonymous):

Is this making sense so far?

OpenStudy (anonymous):

Yes

OpenStudy (anonymous):

If I am not mistaken then the angular speed is coming to be (v/a)(sqrt6)

OpenStudy (anonymous):

Now, your problem is now about finding the moment of inertia for a block whose axis of rotation is about one of its edges. A solid, rectangular parallelpiped is given by...

OpenStudy (anonymous):

I get something close, but different.

OpenStudy (anonymous):

Oh I am sorry, I calculated the I around the Cm

OpenStudy (anonymous):

Which is wrong

OpenStudy (anonymous):

Yes

OpenStudy (anonymous):

So how do you calculate it around that corner?

OpenStudy (anonymous):

Parallel Axis Theorem

OpenStudy (anonymous):

Oh yes, you are right

OpenStudy (anonymous):

The new moment of inertia will be\[I=I_{cm}+Mh^2\] where h is the distance from the CM axis to the new, parallel axis.

OpenStudy (anonymous):

\[I_{cm}=\frac{Ma^2}{6}\]

OpenStudy (anonymous):

\[Mh^2=M \left( \frac{a}{2} \right)^2=M \frac{a^2}{4}\]

OpenStudy (anonymous):

I think it is \[1/6(Ma^2)+2M\]

OpenStudy (anonymous):

So \[I=\frac{5Ma^2}{12}\]

OpenStudy (anonymous):

You see the corner wise distance will be sqrt 2

OpenStudy (anonymous):

I mean sqrt 2 times a

OpenStudy (anonymous):

\[w^2=\frac{12v^2}{5a^2}\]

OpenStudy (anonymous):

Yes, you're right there.

OpenStudy (anonymous):

So change h to a.sqrt(2)

OpenStudy (anonymous):

a/sqrt(2)

OpenStudy (anonymous):

\[h=\frac{a}{\sqrt{2}}\]

OpenStudy (anonymous):

So I am supposed to solve the equation \[0.5 Mv^2=0.5[(1/6)Ma^2+2M]\omega\] Am I right

OpenStudy (anonymous):

am i right?

OpenStudy (anonymous):

I think the moment of inertia should be\[I=\frac{Ma^2}{6}+Mh^2=\frac{Ma^2}{6}+M \left( \frac{a}{\sqrt{2}} \right)^2=\frac{Ma^2}{6}+\frac{Ma^2}{2}\]

OpenStudy (anonymous):

\[=\frac{4Ma^2}{6}=\frac{2Ma^2}{3}\]

OpenStudy (anonymous):

Then\[\frac{1}{2}Mv^2=\frac{1}{2}\frac{2Ma^2}{3} \omega ^2\]

OpenStudy (anonymous):

i.e.\[v^2=\frac{2a^2}{3} \omega ^2 \rightarrow \omega ^2 = \frac{3v^2}{2a^2}\]

OpenStudy (anonymous):

Ok I understand that

OpenStudy (anonymous):

Are you agreeing? I'm doing this on-the-fly, so if you pick up anything, interrupt.

OpenStudy (anonymous):

Any how I have got the thing

OpenStudy (anonymous):

Did your answer agree?

OpenStudy (anonymous):

Lokisan, I have got what I expected, I can handle the rest

OpenStudy (anonymous):

There was some problem with the site, and some of our converstation got split up

OpenStudy (anonymous):

Okay. Happy physics.

OpenStudy (anonymous):

lol, thanks for the genius comment. we'll just see how this question pans out.

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