Torque on Rod Due to Normal Force at a Hinge

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SUMMARY

The discussion focuses on the torque generated by the normal force at a hinge when a support stick is removed from a rod system. The participants confirm that torque is only meaningful with respect to a specified axis, specifically the hinge axis in this case. The net torque equation is established as τnet = Iα, and the normal force at the hinge is derived from the vertical force balance equation Fnet, vertical = Mg - N. The analysis concludes that the reasoning regarding the normal force is correct, provided that the forces acting on the system are accurately accounted for.

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erfz

Homework Statement


In this diagram,
free_f2gif.gif

I wondered if there is any torque due to the normal force from the hinge, once the support stick is removed. I also want to know what the normal force would be at the hinge. The cup and ball are to be ignored here (essentially massless).

Homework Equations


##F_{net} = ma##
##\tau_{net} = I\alpha##
##\tau = Frsin(\phi)##, where ##\phi## is the angle between F and r

The Attempt at a Solution


My assumption would be yes: there is a torque due to the normal force acting straight up from the hinge on the point touching the table. However, the solution to the problem measures torque from the hinge axis (going in and out of the page), and states that the torque is ##\tau_{net} = Mgcos(\theta)\frac{L}{2}##.
I'm confused by this, but I feel that there are two possibilities here:
  1. The torque due to the hinge is somehow 0
  2. The "net" in the expression ##\tau_{net} = I\alpha## depends on the axis it is measured with respect to, just like ##\tau = Frsin(\phi)##. That is to say that the only torques that contribute to the net are those not acting at the axis of choice.
Is one of my suppositions correct?

As for the normal force at the hinge, I was thinking that I could say that ##F_{net, ~vertical} = Mg - N## at the center of mass? This happening at only the center of mass is just a guess. So then, if I go through ##\tau = I\alpha = \frac{1}{3}ML^2 \alpha = Mgcos(\theta)\frac{L}{2}##, I can derive that ##\alpha = \frac{3g}{2L}cos(\theta)## and that the linear acceleration down from this is ##a_{down} = \alpha cos(\theta) \frac{L}{2}##. Using this for the ##F_{net}##, I get that ##a_{down} = g - N##, so ##N = g - a_{down}##.
Is this reasoning correct here?

Thanks!
 

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erfz said:
torque due to the normal force
Torque due to a force is only meaningful in respect of a specified axis. Which axis do you mean?
In particular, if a force acts at a point P then it creates no torque about P.
 
haruspex said:
Torque due to a force is only meaningful in respect of a specified axis. Which axis do you mean?
In particular, if a force acts at a point P then it creates no torque about P.
I see. I meant the axis at the hinge, going in and out of the page.
So this means that supposition 2 is the accurate one.
 
erfz said:
I see. I meant the axis at the hinge, going in and out of the page.
So this means that supposition 2 is the accurate one.
Yes, but they are both true.
 
haruspex said:
Torque due to a force is only meaningful in respect of a specified axis. Which axis do you mean?
In particular, if a force acts at a point P then it creates no torque about P.
haruspex said:
Yes, but they are both true.
Fantastic!
Is there anything wrong you see with my reasoning of the normal force?
 
erfz said:
Is there anything wrong you see with my reasoning of the normal force?
There seem to be some other forces with vertical components, from the stick, the ball and the cup.
But you have not actually stated the problem that goes with the diagram, so it is hard to say. You mention accelerations, for example.
 
haruspex said:
There seem to be some other forces with vertical components, from the stick, the ball and the cup.
But you have not actually stated the problem that goes with the diagram, so it is hard to say. You mention accelerations, for example.
Sorry I should've made it more clear that I'm only considering the system after the supporting stick is removed and that the ball and cup are massless.
I'm really only considering the rod and the hinge for what I'm asking.
 
erfz said:
Sorry I should've made it more clear that I'm only considering the system after the supporting stick is removed and that the ball and cup are massless.
I'm really only considering the rod and the hinge for what I'm asking.
Ah, yes, I did see that earlier but when I came back to the thread I forgot. A risk with multitasking.
erfz said:
at the center of mass?
For linear force analysis, the line of action does not matter, only the direction.

The rest of your work looks fine, except that you forgot to divide N by M at the end.
 
haruspex said:
For linear force analysis, the line of action does not matter, only the direction.
Sorry, I'm not sure what you mean by this. Do you mean the analysis does not require forces be considered at the center of mass? How can that be if different points on the rod have different linear accelerations downward?

haruspex said:
The rest of your work looks fine, except that you forgot to divide N by M at the end.
Haha silly error on my part.
 
  • #10
erfz said:
Sorry, I'm not sure what you mean by this. Do you mean the analysis does not require forces be considered at the center of mass? How can that be if different points on the rod have different linear accelerations downward?
If a force F is exerted on a rigid mass m (floating in space, say) then the acceleration of its mass centre is F/m. The force can be exerted at any point and at any angle. Its line of action does not need to pass through the mass centre.
 
  • #11
haruspex said:
If a force F is exerted on a rigid mass m (floating in space, say) then the acceleration of its mass centre is F/m. The force can be exerted at any point and at any angle. Its line of action does not need to pass through the mass centre.
That's great to know, but I'm not sure why you bring it up. Is there something in my work that contradicts this statement? My main assumption was that the force analysis is to be considered at the center of mass, which is important since every point on the bar has different downward acceleration (proportional to the distance from the hinge). That is to say that ##M_{cm} a_{cm, ~down} = M_{cm}g - N##.
 
  • #12
erfz said:
That's great to know, but I'm not sure why you bring it up. Is there something in my work that contradicts this statement? My main assumption was that the force analysis is to be considered at the center of mass, which is important since every point on the bar has different downward acceleration (proportional to the distance from the hinge). That is to say that ##M_{cm} a_{cm, ~down} = M_{cm}g - N##.
Because you wrote:
erfz said:
I was thinking that I could say that ##F_{net, ~vertical} = Mg - N## at the center of mass? This happening at only the center of mass is just a guess.
 
  • #13
So is that to say that I was correct in my assumption?
 
  • #14
erfz said:
So is that to say that I was correct in my assumption?
Yes.
 
  • #15
haruspex said:
Yes.
Wonderful. Thank you for all your help!
 

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