Help with free body diagram for a pendulum

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Homework Help Overview

The discussion revolves around analyzing the forces and moments acting on a pendulum system, particularly focusing on the free body diagram and the equations of motion. Participants are examining the relationships between various forces, including tension, gravitational force, and the effects of a torsional spring.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants are attempting to sum forces and moments about the pendulum's center of gravity, questioning the correctness of their equations and the signs of various terms. There is discussion about the appropriateness of taking moments about an accelerating point and the implications of the rod's mass on the equations.

Discussion Status

The discussion is active, with participants providing feedback on each other's equations and clarifying the roles of different forces and torques. Some guidance has been offered regarding the signs of terms and the relationships between forces and torques, but no consensus has been reached on the final form of the equations.

Contextual Notes

Participants are navigating constraints related to the assumptions about the mass distribution of the pendulum system and the effects of the torsional spring. There is uncertainty regarding the correct application of trigonometric functions in the context of the forces involved.

theone
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Homework Statement


I want to sum the forces perpendicular to the pendulum and sum the moments about the pendulums center of gravity.

Homework Equations

The Attempt at a Solution


P\sin \theta - mg\cos \theta - N\cos \theta = -m\ddot x\cos \theta + ml\ddot \theta
-Pl\sin \theta - Nl\cos \theta + K_t\theta= I\ddot\theta

I want to know if these are correct, especially the plus/minus
 

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You have a cosine and sine swapped in the first equation.
Your second equation looks doubtful in several respects. What point are you taking moments about? Is it ok to take moments about a point that is accelerating?
Do you even need to take moments, i.e. does the rod have mass?
 
haruspex said:
You have a cosine and sine swapped in the first equation.
Your second equation looks doubtful in several respects. What point are you taking moments about? Is it ok to take moments about a point that is accelerating?
Do you even need to take moments, i.e. does the rod have mass?

The rod does have mass. The point was about the center of gravity of the combined rod/ball thing. l is the the distance from the pivot to the center of gravity. I needed a moment equation because I wanted to eliminate the Psin\theta-Ncos\theta in the first equation.

I don't really know if its ok to take moments about that point. I also don't understand the ml\ddot\theta term in the first equation...
 

for the sum of moments about the pendulum's COG, is the moment due to P negative and the moment due to N positive?
 
theone said:
for the sum of moments about the pendulum's COG, is the moment due to P negative and the moment due to N positive?
With the usual anticlockwise convention, yes.
 
haruspex said:
With the usual anticlockwise convention, yes.
For the first equation, which two terms did you identify as wrong? Is it the P and N terms?
 
theone said:
For the first equation, which two terms did you identify as wrong? Is it the P and N terms?
In each of the terms involving a trig function, the other factor is related to acceleration or force in either the vertical or horizontal direction. You should expect that all of one direction take cos, and all of the other direction take sin.
 
haruspex said:
In each of the terms involving a trig function, the other factor is related to acceleration or force in either the vertical or horizontal direction. You should expect that all of one direction take cos, and all of the other direction take sin.

But for P and mg, which are in opposite directions, I am getting the result that both are sin
 

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theone said:
But for P and mg, which are in opposite directions, I am getting the result that both are sin
They're both vertical, so should match the same trig function.
 
  • #10
haruspex said:
They're both vertical, so should match the same trig function.
so is the final answer including the signs correct: Psin\theta-mgsin\theta-Ncos\theta=m\ddot x cos\theta+ml\ddot\theta
 
  • #11
theone said:
so is the final answer including the signs correct: Psin\theta-mgsin\theta-Ncos\theta=m\ddot x cos\theta+ml\ddot\theta
Not quite. The left hand side appears to be taking up and.left as positive, the right hand side down and right as positive.
 
  • #12
haruspex said:
Not quite. The left hand side appears to be taking up and.left as positive, the right hand side down and right as positive.

I meant for the mg\ddot x cos\theta to be negative. Is that the only mistake
 
  • #13
theone said:
I meant for the mg\ddot x cos\theta to be negative. Is that the only mistake
What about the ##ml\ddot \theta## term? Also, you said the rod has mass, so that should be in the equation, and you need a contribution from the torsion spring.
 
  • #14
haruspex said:
What about the ##ml\ddot \theta## term? Also, you said the rod has mass, so that should be in the equation, and you need a contribution from the torsion spring.

for the rod mass, I considered the rod and ball a single object. Is that ok?
I don't know what the contribution from the torsion spring is. and like I said earlier, I don't really understand the ##ml\ddot \theta## term
 
  • #15
theone said:
for the rod mass, I considered the rod and ball a single object. Is that ok?
I don't know what the contribution from the torsion spring is. and like I said earlier, I don't really understand the ##ml\ddot \theta## term
The ##ml\ddot \theta## term is the acceleration of the mass (in the tangential direction) relative to the acceleration of the block.
The torsion spring applies a torque. What is the relationship between force and torque?
If you are considering the ball and mass as one object, then you need to figure out the mass centre of the combination and see how that affects the ##ml\ddot \theta## term and the torsion spring tem.
 
  • #16
haruspex said:
The ##ml\ddot \theta## term is the acceleration of the mass (in the tangential direction) relative to the acceleration of the block.
The torsion spring applies a torque. What is the relationship between force and torque?
If you are considering the ball and mass as one object, then you need to figure out the mass centre of the combination and see how that affects the ##ml\ddot \theta## term and the torsion spring tem.
The spring applies ##{K_t\theta}## of torque , so then the force it applies is ##\frac{K_t\theta}{l}##, with l being the length of the rod from the pivot to the combined COG?
 
  • #17
theone said:
The spring applies ##{K_t\theta}## of torque , so then the force it applies is ##\frac{K_t\theta}{L}##, with L being the total length of the rod?
That's the force applied to the mass, if the rod is massless. But as I wrote, if you consider the mass and rod as a single unit, you need to deal in terms of their common mass centre, and how far that will be from the joint.
 
  • #18
haruspex said:
That's the force applied to the mass, if the rod is massless. But as I wrote, if you consider the mass and rod as a single unit, you need to deal in terms of their common mass centre, and how far that will be from the joint.

So is it...
Psin\theta-mgsin\theta-Ncos\theta+\frac{K_t \theta}{l}=m\ddot x cos\theta-ml\ddot \theta cos\theta

with l being the distance from the base of the pivot to the combined object's COG?
The force due to the torsional spring acts perpendicular to the length of the rod, right?
 
Last edited:
  • #19
theone said:
So is it...
Psin\theta-mgsin\theta-Ncos\theta+\frac{K_t \theta}{l}=m\ddot x cos\theta-ml\ddot \theta cos\theta

with l being the distance from the base of the pivot to the combined object's COG?
The force due to the torsional spring acts perpendicular to the length of the rod, right?
Yes, except that you've made the ##m\ddot x## term positive again (you said it was meant to be negative), and you've introduced a cos factor on the ##\ddot \theta## term.
 
  • #20
haruspex said:
Yes, except that you've made the ##m\ddot x## term positive again (you said it was meant to be negative), and you've introduced a cos factor on the ##\ddot \theta## term.

thanks
and finally, does the force due to the torsional spring act up and left or down and right? In the equation above, I put it as up and left.
And also, if I were to take a force balance on the cart, would I need to include anything other than P and N to account for the torsional spring?
 
  • #21
theone said:
thanks
and finally, does the force due to the torsional spring act up and left or down and right? In the equation above, I put it as up and left.
up and left
theone said:
And also, if I were to take a force balance on the cart, would I need to include anything other than P and N to account for the torsional spring?
Yes, the torque from the spring reacts on the block exactly opposite to its torque on the arm. This is in addition to P and N.
 

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