Find the equilibrium angle of this unusual driven pendulum geometry

AI Thread Summary
The discussion focuses on finding the equilibrium angle of a driven pendulum with a hoop and mass. Participants analyze the forces acting on the hoop, including friction, normal force, and the weight of the mass. They derive torque equations and explore the relationship between the mass's position and the point of contact. The correct equilibrium angle is confirmed to be related to the sine function of the angle and the ratio of the radius and length parameters. The final consensus is that the mass must be vertically aligned under the point of contact for the equilibrium to hold.
Alif Yasa
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Homework Statement
In Picture
Relevant Equations
Force Equilibrium and Torque Equilibrium
241431


-I tried to draw the forces on the hoop when it is in the equilibrium state. I know there are friction and normal force on the contact point of the shaft and the hoop
-I also put the weight force to the M object
-But when i used the torque equilibrium, where the pivot is the contact point of the shaft and the hoop, the only torque exist is the weight force that is caused by the M object
-I expect I'm missing other forces, but i don't know what is it
 
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Alif Yasa said:
when i used the torque equilibrium, where the pivot is the contact point of the shaft and the hoop, the only torque exist is the weight force that is caused by the M object
So what does that tell you about the location of the mass?
 
I find that the torque by the mass is
T=Mg sin(x) *(R+L)
where x is the equilibrium angle
 
Alif Yasa said:
I find that the torque by the mass is
T=Mg sin(x) *(R+L)
where x is the equilibrium angle
Your diagram must be wrong. Can you post it?
 
it is something like this
241436
 
Alif Yasa said:
it is something like this
View attachment 241436
Ok, but then I do not understand how you got what you did for the torque about the point of contact.
You correctly determined that the weight of the mass is the only force that could have such a torque. So in equilibrium, what does that tell you about the position of the mass in relation to the point of contact?
 
Oh, so is it like
Mg cos(x)R-Mg sin(x)(R+L)=0
and tan(x) = R/(R+L)

Also, from the force equilibrium, i got
tan(x)=1/u
cos(x)=u/sqrt(1+u^2)

The answer from the book is
x=arcsin((Ru)/((R+L)sqrt(1+u^2))

I can get it if i multiply tan(x) from the torque with cos(x) from the force,
but why it isn't just arctan(1/u) or arctan(R/(R+L)) ?
Do it have to be done that way ?
 
Alif Yasa said:
Oh, so is it like
Mg cos(x)R-Mg sin(x)(R+L)=0
No.
Call the centre of the hoop C, the point of contact P and the mass M.
You seem to be assuming PCM is a right angle. It need not be.
E.g., without the information that the shaft is rotating, a solution would be that P is at the top of the shaft and the rod is vertical.

Think about the fact that the line of action of the weight is vertically through the mass. Where must it lie in relation to P?
 
So, if i make the angle between vertical axis and PC is y, and the equilibrium angle x

The net torques are

mg sin(x)(R cos(x+y)+R+L)-mg cos(x)(R sin(x+y)) =0
sin(x)(R+L) = R sin(y)

and from the forces

tan(y)=u
sin(y)=u/sqrt(1+u^2)

then i get
sin(x) = (Ru)/((R+L)sqrt(1+u^2))

Is that correct ?
 
  • #10
Alif Yasa said:
So, if i make the angle between vertical axis and PC is y, and the equilibrium angle x

The net torques are

mg sin(x)(R cos(x+y)+R+L)-mg cos(x)(R sin(x+y)) =0
sin(x)(R+L) = R sin(y)

and from the forces

tan(y)=u
sin(y)=u/sqrt(1+u^2)

then i get
sin(x) = (Ru)/((R+L)sqrt(1+u^2))

Is that correct ?
Looks right!
(What I was trying to get you to spot is that the mass must be vertically under P.)
 
  • #11
haruspex said:
Looks right!
(What I was trying to get you to spot is that the mass must be vertically under P.)
Thanks !
 
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