Double pendulum: energy function

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Discussion Overview

The discussion revolves around the energy function of a double pendulum in a uniform gravitational field, exploring the differences between motion restricted to a vertical plane and motion in three-dimensional space. Participants examine the potential and kinetic energy components of the system and their implications for the energy function.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant states that the energy function is the sum of potential energy ($PE=m_1gy_1+m_2gy_2$) and kinetic energy ($KE=\frac{1}{2}m_1v_1^2+\frac{1}{2}m_2v_2^2$).
  • Another participant clarifies that in a vertical plane, motion is described using only $x$ and $y$ coordinates, while motion in space includes a third coordinate, possibly $z$.
  • There is a discussion about the implications of a uniform gravitational field, with one participant noting that it represents constant vertical acceleration, contrasting it with the inverse square law of gravity.
  • Participants explore how to express kinetic energy differently for motion in a vertical plane versus motion in space, raising questions about the use of $z$ coordinates and the potential for polar coordinates.
  • One participant suggests that using polar coordinates is unnecessary unless it aids in solving a follow-up question.
  • There is a query regarding whether the potential energy is the same in both cases, to which multiple participants affirmatively respond.

Areas of Agreement / Disagreement

Participants generally agree on the formulation of potential energy in both cases and the distinction between kinetic energy in the two scenarios. However, there are ongoing questions about the necessity of different coordinate systems and the implications of these choices, indicating some unresolved aspects of the discussion.

Contextual Notes

The discussion includes assumptions about the definitions of coordinates and the nature of gravitational fields, which may not be universally agreed upon. There are also unresolved mathematical steps regarding the transition between different coordinate systems.

mathmari
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Hey! :o

I am looking at the following:

Find the energy function for the double pendulum, with vertical constant and uniform gravity field
  • for motion restricted at vertical plane
  • for motion in space
We have that the energy function is the sum of the potential and the kinetic energy, right?

The potential energy of the system is given by $PE=m_1gy_1+m_2gy_2$.

The kinetic energy is given by $KE=\frac{1}{2}m_1v_1^2+\frac{1}{2}m_2v_2^2$.

Therefore, the energy function is equal to $$E=PE+KE=m_1gy_1+m_2gy_2+\frac{1}{2}m_1v_1^2+\frac{1}{2}m_2v_2^2$$ Is this correct?

How can we distinct between motion restricted at vertical plane and motion in space? And what does a uniform gravitational field imply?

(Wondering)
 
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mathmari said:
How can we distinct between motion restricted at vertical plane and motion in space?

Hey mathmari! (Smile)

In a vertical plane we only have $x$ and $y$.
So $v_1^2 = \dot x_1^2 + \dot y_1^2$.

For motion in space we also have a 3rd coordinate (perhaps we should pick the vertical coordinate to be $z$ instead of $y$ to avoid confusion.) (Thinking)

mathmari said:
And what does a uniform gravitational field imply?

That we have constant vertical acceleration by gravity $g$, which is what you already have.
That is as opposed to how gravity actually works, which is $\frac{GM}{r^2}$, where $M$ is the mass of the earth, and $r$ is the distance to the center of the earth. At the surface we can treat it as a uniform field though. (Thinking)
 
I like Serena said:
Hey mathmari! (Smile)

In a vertical plane we only have $x$ and $y$.
So $v_1^2 = \dot x_1^2 + \dot y_1^2$.

For motion in space we also have a 3rd coordinate (perhaps we should pick the vertical coordinate to be $z$ instead of $y$ to avoid confusion.) (Thinking)

So, to difference between the two motions is at the kinetic energy?

Do we get for the first case:

The potential energy of the system is given by $PE=m_1gy_1+m_2gy_2$.
The kinetic energy is given by $KE=\frac{1}{2}m_1v_1^2+\frac{1}{2}m_2v_2^2=\frac{1}{2}m_1\left (\dot x_1^2 + \dot y_1^2\right )+\frac{1}{2}m_2\left (\dot x_2^2 + \dot y_2^2\right )$.

and for the second case:

The potential energy of the system is given by $PE=m_1gy_1+m_2gy_2$.
Here do we have to use also $z_1,z_2$ ? But how?
The kinetic energy is given by $KE=\frac{1}{2}m_1v_1^2+\frac{1}{2}m_2v_2^2=\frac{1}{2}m_1\left (\dot x_1^2 + \dot y_1^2+\dot z_1^2\right )+\frac{1}{2}m_2\left (\dot x_2^2 + \dot y_2^2+\dot z_2^2\right )$.

? Or do we have to use for example polar coordinates? (Wondering)
 
Last edited by a moderator:
Yep. (Nod)

We can write the same thing in polar coordinates, but there is no need.
The only reason to do so, is if it helps us to solve a follow up question, and we can do it then.
 
I like Serena said:
Yep. (Nod)

So, we do we get the following energy function?

  1. for motion restricted at vertical plane

    The potential energy of the system is given by $PE=m_1gy_1+m_2gy_2$.
    The kinetic energy is given by $KE=\frac{1}{2}m_1v_1^2+\frac{1}{2}m_2v_2^2=\frac{1}{2}m_1\left (\dot x_1^2 + \dot y_1^2\right )+\frac{1}{2}m_2\left (\dot x_2^2 + \dot y_2^2\right )$.

    So, the total energy is given by $$E=PE+KE=m_1gy_1+m_2gy_2+\frac{1}{2}m_1\left (\dot x_1^2 + \dot y_1^2\right )+\frac{1}{2}m_2\left (\dot x_2^2 + \dot y_2^2\right )$$
  2. for motion in space

    The potential energy of the system is given by $PE=m_1gy_1+m_2gy_2$.
    The kinetic energy is given by $KE=\frac{1}{2}m_1v_1^2+\frac{1}{2}m_2v_2^2=\frac{1}{2}m_1\left (\dot x_1^2 + \dot y_1^2+\dot z_1^2\right )+\frac{1}{2}m_2\left (\dot x_2^2 + \dot y_2^2+\dot z_2^2\right )$.

    So, the total energy is given by $$E=PE+KE=m_1gy_1+m_2gy_2+\frac{1}{2}m_1\left (\dot x_1^2 + \dot y_1^2+\dot z_1^2\right )+\frac{1}{2}m_2\left (\dot x_2^2 + \dot y_2^2+\dot z_2^2\right )$$
Is the potential energy in both cases the same? (Wondering)
 
Yes and yes. (Mmm)
 
I like Serena said:
Yes and yes. (Mmm)

Ok! Thank you very much! (Smile)
 

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