How Do You Solve This Rotational Motion Problem?

[coldblood]

Hi friends,
Please help me in solving this problem, I'll appreciate the help.

The problem is as:

https://fbcdn-sphotos-c-a.akamaihd.net/hphotos-ak-ash3/q71/s720x720/1493276_1461728287387610_1599334130_n.jpg

Attempt -

https://fbcdn-sphotos-d-a.akamaihd.net/hphotos-ak-ash4/q87/s720x720/1482774_1461728540720918_889630073_n.jpg



Thank you all in advance.

 

[tiny-tim]

hi coldblood!

this is a collision

energy will be lost

both v and ω will change suddenly

hint: can you use conservation of momentum in any direction? if not, why not?

can you use conservation of angular momentum about any point? if not, why not?​

 

[coldblood]

can you use conservation of momentum in any direction? if not, why not?

can you use conservation of angular momentum about any point? if not, why not?[/INDENT]

I think I can conserve momentum in the direction of line OP, because in this direction the wheel exerts force on the step during collision.

And the wheel rotates about point P, hence I can conserve angular momentum about that point.

 

[tiny-tim]

hi coldblood!

I think I can conserve momentum in the direction of line OP, because in this direction the wheel exerts force on the step during collision.

no, because the impulse at the step is completely unknown …

it could be in any direction, so no direction is safe

And the wheel rotates about point P, hence I can conserve angular momentum about that point.

yes, but that's not quite the right reasoning …

the impulse at the step (obviously) has no torque about the step, so there wil be no impulsive (ie sudden) change in angular momentum (the weight does have a torque, and so does the reaction force from the ground, but they're not impulsive, so they don't contribute to the impulsive change)

ok, so use impulsive conservation of angular momentum …

what do you get? ​

 

[coldblood]

(the weight does have a torque, and so does the
what do you get? [/INDENT]

The torque of mg :

mg (R cos 30⁰) But it will be anticlockwise.

The torque of reactionary force will be zero.

 

[tiny-tim]

The torque of mg :

mg (R cos 30⁰) But it will be anticlockwise.

yes, but it's not impulsive …

when you do impulsive conservation of angular momentum,

you are comparing angular momentum "before" with angular momentum "after",

∆(angular momentum) = angular impulse = torque times ∆t​

and the gap, ∆t, in time between "before" and "after" is (taken to be) infinitesimally small

in that infinitesimally small time, the torque-times-time of mg is obviously infinitesimally small, ie we ignore it

(same with the reaction force: it too is not impulsive, its impulsive torque is taken to be zero)

so what impulsive forces are there?

and what is the total impulsive torque?​

 

[haruspex]

This thread is heading in the right direction to deduce A, but I can't agree that B and C are true.

 

[tiny-tim]

This thread is heading in the right direction to deduce A, but I can't agree that B and C are true.

for now, let's keep our eyes firmly on A …

i haven't even looked at B or C yet ​

 

[coldblood]

what is the total impulsive torque?[/INDENT]

Will the torque due to friction act as impulsive torque here or the torque due to reaction force?

 

[tiny-tim]

loosely speaking:

if the surface changes suddenly, the reaction force is impulsive; if it changes smoothly, it's not impulsive​

the step is a sudden change, so the force from it is impulsive

the ground is flat, so the force from it is not impulsive

 

[haruspex]

Yes, that's a useful guide, but fwiw, here's how I think of it. If a force is limited in magnitude then its integral over an arbitrarily short time is arbitrarily small, so no impulsive momentum change. The gravitational force is so limited, and in consequence so are the normal force from the ground and any friction on the ground.
The normal force from the step has to deliver a certain momentum change regardless of how short the duration of impact, so the force is unlimited. Consequently, so is the frictional force.