Planar pendulum with rotating pivot

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Homework Help Overview

The discussion revolves around the coordinates of a mass in a planar pendulum system with a rotating pivot. Participants are examining the correct expressions for the coordinates based on the position of the mass and the pivot, particularly focusing on the signs of the variables involved.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants are analyzing the expressions for the coordinates of the mass, questioning the signs of the variables based on the quadrant in which the motion occurs. There is an exploration of how the definitions of the variables relate to their values in different positions.

Discussion Status

The discussion is active, with participants providing insights and clarifications regarding the signs of the coordinates. Some participants express confusion about the correct expressions and the implications of the quadrant on the values of the coordinates, while others attempt to clarify the relationships between the variables.

Contextual Notes

Participants are working within the constraints of a homework problem, which may impose specific definitions and expectations regarding the coordinate system and the motion of the pendulum. There is an ongoing examination of the assumptions made in the problem setup.

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Homework Statement
Please see below
Relevant Equations
##x = x_p + x_m = R\cos(\omega t) + l\sin(\phi)##

##y = -y_p - y_m = -R\sin(\omega t) -l\cos\phi##
For this problem,
1713422077986.png

My working for finding the coordinates of the mass is,
##x = x_p + x_m = R\cos(\omega t) + l\sin(\phi)##
##y = -y_p - y_m = -R\sin(\omega t) -l\cos\phi##

However, I am told that correct coordinates of the mass is
##x = x_p + x_m = R\cos(\omega t) + l\sin(\phi)##
##y = y_p - y_m = R\sin(\omega t) -l\cos\phi##

I am confused why the y_p is positive since it is clearly negative in the diagram. Can someone please explain to me?

Also if anybody has any tips for finding coordinates in general for physics that would be greatly appreciated! It seems to be the hardest part in mechanics problems.

Thanks!
 
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ChiralSuperfields said:
I am confused why the y_p is positive since it is clearly negative in the diagram. Can someone please explain to me?
The diagram clearly shows that the positive y axis points upwards. In the position shown, ##\omega t## is in the fourth quadrant so ##y_p## will have a negative value.
What does look wrong is the ##-y_m##. If ##y_m## is the offset from P to m in the positive y-axis direction then ##y=y_p+y_m=R\sin(\omega t)-l\cos(\phi)##.
 
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haruspex said:
The diagram clearly shows that the positive y axis points upwards. In the position shown, ##\omega t## is in the fourth quadrant so ##y_p## will have a negative value.
What does look wrong is the ##-y_m##. If ##y_m## is the offset from P to m in the positive y-axis direction then ##y=y_p+y_m=R\sin(\omega t)-l\cos(\phi)##.
Thank you for your reply @haruspex! I agree that ##-y_m## is wrong.

Sorry, are you saying I'm correct and the answer is wrong? i.e ##y=-R\sin(\omega t)-l\cos(\phi)## is indeed correct since you said that ##y_p < 0##? If so I should raise with marker.

Thanks!
 
ChiralSuperfields said:
Sorry, are you saying I'm correct and the answer is wrong?
No. You are confusing the sign of the variable in the equation with the sign of its value in a particular state.
##y, y_p, y_m## are all measured with up positive. Since ##y_p## is defined as the height of P above the origin and ##y_m## is defined as the height of m above P, it is necessarily true that ##y##, the height of m above the origin, is ##y_p+y_m##.
In the diagram, ##\omega t## is in the fourth quadrant so its sine is negative and ##y_p## will have a negative value. The way ##\phi## is defined, ##y_m=-l\cos(\phi)##, and in the diagrammed position that will also be negative. Adding those two negative values produces a negative value of greater magnitude, exactly as shown in the diagram.
 
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haruspex said:
No. You are confusing the sign of the variable in the equation with the sign of its value in a particular state.
##y, y_p, y_m## are all measured with up positive. Since ##y_p## is defined as the height of P above the origin and ##y_m## is defined as the height of m above P, it is necessarily true that ##y##, the height of m above the origin, is ##y_p+y_m##.
In the diagram, ##\omega t## is in the fourth quadrant so its sine is negative and ##y_p## will have a negative value. The way ##\phi## is defined, ##y_m=-l\cos(\phi)##, and in the diagrammed position that will also be negative. Adding those two negative values produces a negative value of greater magnitude, exactly as shown in the diagram.
Thank you for your reply @haruspex!

Sorry I am still confused. The y-coordinate in the first quadrant (not shown in the diagram) is ##y=R\sin(\omega t) - l\cos(\phi)## and in the fourth quadrant (shown in the diagram) is ##y=-R\sin(\omega t)-l\cos(\phi)##? Is that please correct?

If each of those coordinates are correct for their respective quadrants, do you please know which are we meant to use for finding the Lagrangian and why?

Thanks!
 
ChiralSuperfields said:
Thank you for your reply @haruspex!

Sorry I am still confused. The y-coordinate in the first quadrant (not shown in the diagram) is ##y=R\sin(\omega t) - l\cos(\phi)## and in the fourth quadrant (shown in the diagram) is ##y=-R\sin(\omega t)-l\cos(\phi)##? Is that please correct?

If each of those coordinates are correct for their respective quadrants, do you please know which are we meant to use for finding the Lagrangian and why?

Thanks!
No, the equation can't magically change. It has to be the one equation for all configurations that arise in the motion.
Consider two positions, first quadrant, ##\omega t=\pi/6## and fourth quadrant, ##\omega t=-\pi/6##.
In the first quadrant, ##y=R\sin(\omega t) - l\cos(\phi)=R/2- l\cos(\phi)##. In the fourth quadrant, ##y=R\sin(\omega t) - l\cos(\phi)=-R/2- l\cos(\phi)##. Same equation, different values.
 
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haruspex said:
No, the equation can't magically change. It has to be the one equation for all configurations that arise in the motion.
Consider two positions, first quadrant, ##\omega t=\pi/6## and fourth quadrant, ##\omega t=-\pi/6##.
In the first quadrant, ##y=R\sin(\omega t) - l\cos(\phi)=R/2- l\cos(\phi)##. In the fourth quadrant, ##y=R\sin(\omega t) - l\cos(\phi)=-R/2- l\cos(\phi)##. Same equation, different values.
Ooooh thank you @haruspex!

I think I see what you are saying now. Am I please correct to say that we are not meant to fudge the ##R\sin(\omega t)## sign like I was since ##-\omega t < 0## in fourth quadrant?

Thanks!
 
ChiralSuperfields said:
Ooooh thank you @haruspex!

I think I see what you are saying now. Am I please correct to say that we are not meant to fudge the ##R\sin(\omega t)## sign like I was since ##-\omega t < 0## in fourth quadrant?

Thanks!
Right.
 
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