Planar pendulum with rotating pivot

In summary, a planar pendulum with a rotating pivot describes a pendulum system where the pivot point itself rotates around a fixed axis, affecting the dynamics of the pendulum's motion. This setup introduces complexities in the pendulum's behavior, including changes in amplitude, frequency, and stability, due to the additional rotational motion. The analysis of such systems often involves nonlinear dynamics and can lead to interesting phenomena such as chaotic behavior under certain conditions. Understanding the interactions between the pendulum and the rotating pivot can provide insights into various applications in physics and engineering.
  • #1
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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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  • #2
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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  • #3
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!
 
  • #4
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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  • #5
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!
 
  • #6
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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  • #7
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!
 
  • #8
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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FAQ: Planar pendulum with rotating pivot

What is a planar pendulum with a rotating pivot?

A planar pendulum with a rotating pivot is a mechanical system where a pendulum is attached to a pivot point that is capable of rotation. This system allows the pivot to move in a circular path, which adds complexity to the dynamics of the pendulum. The motion of the pendulum is influenced not only by gravity but also by the rotational motion of the pivot, leading to interesting behaviors and oscillations.

How does the rotation of the pivot affect the motion of the pendulum?

The rotation of the pivot introduces additional forces and accelerations that affect the pendulum's motion. As the pivot rotates, it alters the effective gravitational force acting on the pendulum, which can lead to changes in the pendulum's period, amplitude, and stability. Depending on the speed and direction of the pivot's rotation, the pendulum can exhibit complex motion patterns, including chaotic behavior.

What are the equations of motion for a planar pendulum with a rotating pivot?

The equations of motion for a planar pendulum with a rotating pivot can be derived using Lagrangian mechanics. The system is typically described by a set of differential equations that take into account the angular position of the pendulum, the angular velocity of the pivot, and the gravitational force. The resulting equations can be quite complex, often requiring numerical methods for solutions, especially when non-linear effects are significant.

What are some practical applications of planar pendulums with rotating pivots?

Planar pendulums with rotating pivots have various applications in engineering and robotics. They can be used in the design of dynamic systems, such as robotic arms or amusement park rides, where controlled oscillatory motion is desired. Additionally, they serve as educational tools in physics to demonstrate principles of dynamics, stability, and chaos theory.

How can one analyze the stability of a planar pendulum with a rotating pivot?

Stability analysis of a planar pendulum with a rotating pivot typically involves examining the equilibrium points of the system and determining their stability using techniques such as linearization or Lyapunov's method. By analyzing the eigenvalues of the linearized system around these equilibrium points, one can predict whether small perturbations will lead to stable or unstable motion. Numerical simulations can also be employed to visualize the behavior of the system over time.

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