Simple pendulum with moving support

In summary, a simple pendulum with a moving support is a variation of the classical pendulum system where the pivot point is not fixed but can move in a certain direction. This setup introduces additional dynamics as the motion of the support affects the pendulum's oscillation. The analysis of such a system involves considering the forces acting on the pendulum, the effect of the support's motion on the pendulum's period, and the potential for more complex behaviors compared to a standard fixed-pivot pendulum. This system has applications in various fields, including engineering and physics, where understanding the interaction between moving supports and pendulum dynamics can lead to innovative designs and solutions.
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Homework Statement
I am trying to find the coordinates of a simple pendulum on a rotating support.
Relevant Equations
Please see below.
For this problem,
1712977179205.png

1712977196393.png

The correct coordinates are,
1712977351430.png

However, I am confused how they got them.

So here is my initial diagram. I assume that the point on the vertical circle is rotating counterclockwise, that is, it is rotating from the x-axis to the y-axis.

1712977615661.png


Thus ## \omega t > 0## for the point. i.e angle subtended from positive x-axis to positive y-axis is positive. However, this does not give the correct relations for the point.

To get the correct relations, you must make the diagram,
1712977718709.png

Due to the odd and even function properties of sine and cosine, this gives the desired solution since $$-\omega t < 0$$. However, does anybody please know what convention this is called, i.e. angle $$\omega t$$ rotated from the positive x-axis to the negative y-axis is positive?

Thanks for any help!
 

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The question does not specify whether the rotation is clockwise or anticlockwise. If it is anticlockwise then the diagrammed position can be thought of as being with t negative.
 
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haruspex said:
The question does not specify whether the rotation is clockwise or anticlockwise. If it is anticlockwise then the diagrammed position can be thought of as being with t negative.
Thank you for your reply @haruspex!

If the question does not specify the direction of rotation, is it in general safe to assume that is it anticlockwise, from the positive x-axis to the positive y-axis?

This question is from landau mechanics 3rd edition page 11, problem 3.

Thanks!
 
  • #4
ChiralSuperfields said:
Thank you for your reply @haruspex!

If the question does not specify the direction of rotation, is it in general safe to assume that is it anticlockwise, from the positive x-axis to the positive y-axis?
If x is to the right and y is up then yes, but here the positive y axis is down, so all bets are off.
 
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ChiralSuperfields said:
If the question does not specify the direction of rotation, is it in general safe to assume that is it anticlockwise, from the positive x-axis to the positive y-axis?
The question indeed does not specify the sense of the rotation. However, in order to write equations and solve the problem, one is free to choose but must choose a sense of rotation. The author of the solution has chosen
##x(t)=a\cos\!\gamma t~\implies \dot x(t)=-\gamma a \sin\!\gamma t##
##y(t)=-a\sin\!\gamma t~\implies \dot y(t)=-\gamma a \cos\!\gamma t##
It follows that
##x(0)=a~;~~ \dot x(0)=0##
##y(0)=0~;~~ \dot y(0)=-\gamma a ##
Conventionally assuming that ##\gamma## represents an angular speed not an angular velocity, we see that at ##t=0## the point of support is on the positive x-axis moving in the negative y-direction, i.e. "up" in the original Figure 3. Thus, the author of the solution implicitly chose the rotation to be counterclockwise by specifying ##x(t)## and ##y(t)##.

We can interpret the original Figure 3 as showing the point of support at time ##t## such that ##~\frac{3}{2}\pi < \gamma t < 2\pi##. Your first modified Figure 3 would be correct if you labeled the "larger angle" as ##\gamma t.##
 
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FAQ: Simple pendulum with moving support

What is a simple pendulum with a moving support?

A simple pendulum with a moving support is a pendulum system where the point of suspension can change its position, typically in a horizontal direction. This setup allows for the investigation of the effects of the support's motion on the pendulum's oscillation characteristics, such as its period and amplitude.

How does the motion of the support affect the pendulum's period?

The motion of the support can significantly influence the period of the pendulum. If the support moves horizontally with a constant velocity, it can alter the effective length of the pendulum, leading to changes in the oscillation period. The interaction between the pendulum's motion and the support's motion can create complex dynamics that may require advanced mathematical modeling to fully understand.

What are the applications of studying simple pendulums with moving supports?

Studying simple pendulums with moving supports has various applications in fields such as engineering, robotics, and physics education. It can be used to design systems that require precise control of oscillatory motion, analyze the stability of structures under dynamic loads, or serve as an educational tool to demonstrate principles of mechanics and dynamics.

Can the support move in different ways, and how does that affect the pendulum?

Yes, the support can move in various ways, such as with constant velocity, oscillating, or in a non-linear manner. Each type of motion affects the pendulum differently. For example, if the support oscillates vertically, it may introduce additional forces that can lead to complex motion patterns, including coupled oscillations. The specific effects depend on the parameters of the system, such as the frequency and amplitude of the support's motion.

What are the key equations governing the motion of a simple pendulum with a moving support?

The motion of a simple pendulum with a moving support can be described using a combination of Newton's laws and harmonic motion equations. The equations typically involve the pendulum's length, the angle of displacement, gravitational acceleration, and the parameters of the support's motion. The resulting equations can become quite complex, often requiring numerical methods for solutions, especially when the support's motion is non-linear.

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