Watt Rotational Speed Regulator's Lagrangian

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SUMMARY

The discussion centers on calculating the kinetic energy of the Watt Rotational Speed Regulator using Lagrangian mechanics. The user initially miscalculated the coordinates for the kinetic energy, leading to discrepancies with the book's results. Correct coordinates were established as \(x_{1}=l\sin{\theta}\sin{\varphi}\), \(y_{1}=l\sin{\theta}\cos{\varphi}\), and similar for \(x_{2}\) and \(y_{2}\). The final kinetic energy expression derived is \(T=ml^2(\dot \theta^2+\dot \varphi^2 \sin^{2}{\theta})\), aligning with the book's calculations.

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Hari Seldon
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Homework Statement
I am trying to find the Lagrangian of a system called "Watt Regulator". My kinetic energy doesn't match the kinetic energy on the book. I would like to know if I am calculating the coordinates of the system in the right way.
Relevant Equations
Kinetic energy of the whole system: ##T = m v^2 = m (\dot x^2+\dot y^2)##
1641375492050.png

I understand that it is a system with two degrees of freedom. And I chose as generalized coordinates the two angles shown in the pic I posted. I am having troubles in finding the kinetic energy of this system, cause the book tells me that the kinetic energy is something different then what I calculated.
So very likely I am wrongly calculating the ##x## and the ##y##.
Indeed I calculated the ##x## as
$$x = l \sin{\varphi}+l \sin{\theta}$$
and the ##y## as
$$y = l \cos{\varphi}+l cos{\theta}$$
Then I calculated the derivative of ##x## and ##y##:
$$\dot x=l \dot \varphi \cos{\varphi}+l \dot \theta \cos{\theta}$$
$$\dot y=-l \dot \varphi \sin{\varphi}-l \dot \theta \sin{\theta}$$
So my kinetic energy would be
$$T = m (\dot x^2+\dot y^2)=m l^2 [\dot \theta^2 +\dot \varphi^2+2\dot \theta \dot \varphi (\cos{\varphi} \cos{\theta}-\sin{\varphi} \sin{\theta})]$$
While the kinetic energy that the book calculated is
$$T=m l^2 (\dot \theta^2+\dot \varphi^2 \sin^2{\theta})$$
What am I doing wrong?
 
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Hari Seldon said:
Homework Statement:: I am trying to find the Lagrangian of a system called "Watt Regulator". My kinetic energy doesn't match the kinetic energy on the book. I would like to know if I am calculating the coordinates of the system in the right way.
Relevant Equations:: Kinetic energy of the whole system: ##T = m v^2 = m (\dot x^2+\dot y^2)##

View attachment 295144
I understand that it is a system with two degrees of freedom. And I chose as generalized coordinates the two angles shown in the pic I posted. I am having troubles in finding the kinetic energy of this system, cause the book tells me that the kinetic energy is something different then what I calculated.
So very likely I am wrongly calculating the ##x## and the ##y##.
Indeed I calculated the ##x## as
$$x = l \sin{\varphi}+l \sin{\theta}$$
and the ##y## as
$$y = l \cos{\varphi}+l cos{\theta}$$
Then I calculated the derivative of ##x## and ##y##:
$$\dot x=l \dot \varphi \cos{\varphi}+l \dot \theta \cos{\theta}$$
$$\dot y=-l \dot \varphi \sin{\varphi}-l \dot \theta \sin{\theta}$$
So my kinetic energy would be
$$T = m (\dot x^2+\dot y^2)=m l^2 [\dot \theta^2 +\dot \varphi^2+2\dot \theta \dot \varphi (\cos{\varphi} \cos{\theta}-\sin{\varphi} \sin{\theta})]$$
While the kinetic energy that the book calculated is
$$T=m l^2 (\dot \theta^2+\dot \varphi^2 \sin^2{\theta})$$
What am I doing wrong?
I think you are adding each of the individual projections instead of projecting twice (i.e. multiplying)

(Interesting that they would define ##\phi## from ##y##-axis but it should work out)

Also you have two particles not just one. (merely multiply ##\frac{1}{2}## by ##2## won't work because their coordinates are not the same)

##x_1## (The closer one in the pic) should be calculated as follows

Project into the ##xy##-plane

## \ell \sin \theta##

now project again onto the ##x-axis##

##x_1 = \ell \sin \theta \sin \phi##

Do this for ##y_1, z_1, x_2, y_2, z_2##
 
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Likes vanhees71 and Hari Seldon
Thank you very much for your help!
Yes, I was adding instead then projecting. So the coordinates should be the following?
$$ x_{1}=l\sin{\theta}\sin{\varphi}$$
$$ y_{1}=l\cos{\theta}\cos{\varphi}$$
$$ x_{2}=-l\sin{\theta}\sin{\varphi}$$
$$ y_{2}=l\cos{\theta}\cos{\varphi}$$
Do I need also ##z_{1}## and ##z_{2}##?
 
Hari Seldon said:
Thank you very much for your help!
Yes, I was adding instead then projecting. So the coordinates should be the following?
$$ x_{1}=l\sin{\theta}\sin{\varphi}$$
$$ y_{1}=l\cos{\theta}\cos{\varphi}$$
$$ x_{2}=-l\sin{\theta}\sin{\varphi}$$
$$ y_{2}=l\cos{\theta}\cos{\varphi}$$
Do I need also ##z_{1}## and ##z_{2}##?

I would think so because as ##\theta## changes so would ##z_1## and ##z_2## (which are the same)
 
@Hari Seldon I just realized I didn't full respond to your previous post

I agree with your ##x_1## and ##x_2## but not your ##y_1## and ##y_2##.

I'm getting

##x_1 = \ell \sin \theta \sin \phi##

##y_1 = \ell \sin \theta \cos \phi##

##z_1 = \ell \cos \theta##

##x_2 = - \ell \sin \theta \sin \phi##

##y_2 = - \ell \sin \theta \cos \phi##

##z_1 = \ell \cos \theta##

Remember finding the ##x##-projection involves two steps 1) projecting onto the ##xy##-plane and 2) projecting onto the ##x-axis##

Likewise

Remember finding the ##y##-projection involves two steps 1) projecting onto the ##xy##-plane and 2) projecting onto the ##y-axis##

The first two steps are the same so they should both have the same first factor.
 
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Likes Hari Seldon
Perfect!
So given the following coordinates of the two masses:
$$x_{1}=l\sin{\theta}\sin{\varphi}~~~x_{2}=-l\sin{\theta}\sin{\varphi}$$
$$y_{1}=l\sin{\theta}\cos{\varphi}~~~y_{2}=-l\sin{\theta}\cos{\varphi}$$
$$z_{1}=l\cos{\theta}~~~~~z_{2}=l\cos{\theta}$$
We can calculate the derivative of them
$$\dot x_{1}=l\dot \theta \cos{\theta}\sin{\varphi}+l\dot \varphi \cos{\varphi} \sin{\theta}$$
$$\dot y_{1}=l\dot \theta \cos{\theta}\cos{\varphi}-l\dot \varphi \sin{\varphi} \sin{\theta}$$
$$\dot z_{1}=-l\dot \theta \sin{\theta}$$

$$\dot x_{2}=-l\dot \theta \cos{\theta}\sin{\varphi}-l\dot \varphi \cos{\varphi} \sin{\theta}$$
$$\dot y_{2}=-l\dot \theta \cos{\theta}\cos{\varphi}+l\dot \varphi \sin{\varphi} \sin{\theta}$$
$$\dot z_{2}=-l\dot \theta \sin{\theta}$$

Then we can calculate the kinetic energy of the system
$$T=T_{1}+T_{2}$$
$$T_{1}=\frac {1} {2} m v_{1}^{2}=\frac {1} {2} m (\dot x_{1}^{2}+\dot y_{1}^{2}+\dot z_{1}^{2})=\frac {1} {2} m l^2 (\dot \theta^2 \cos^{2}{\theta} \sin^{2}{\varphi}+\dot \varphi^2 \cos^{2}{\varphi} \sin^{2}{\theta}+2 \dot \theta \dot \varphi \cos{\theta} \cos{\varphi} \sin{\theta} \sin{\varphi}+\dot \theta^2 \cos^{2}{\theta} \cos^{2}{\varphi}+\dot \varphi^2 \sin^{2}{\varphi} \sin^{2}{\theta}-2 \dot \theta \dot \varphi \cos{\theta} \cos{\varphi} \sin{\theta} \sin{\varphi}+\dot \theta^2 \sin^{2}{\theta})$$
$$T_{1}=\frac {1} {2} m l^2(\dot \theta^2 \cos^{2}{\theta}+\dot \varphi^2 \sin^{2}{\theta}+\dot \theta^2 \sin^{2}{\theta})=$$
$$=\frac {1} {2} m l^2(\dot \theta^2+\dot \varphi^2 \sin^{2}{\theta})$$Similarly for ##T_{2}## we find
$$T_{2}=\frac {1} {2} m l^2(\dot \theta^2+\dot \varphi^2 \sin^{2}{\theta})$$
And then
$$T=m l^2 (\dot \theta^2+\dot \varphi^2 \sin^{2}{\theta})$$

Now we calculate the potential energy
$$V=-mgz_{1}-mgz_{2}=-2mgl \cos{\theta}$$
Finally we can write the Lagangian
$$L=T-V=ml^2(\dot \theta^2+\dot \varphi^2 \sin^{2}{\theta})+2mgl \cos{\theta}$$

Thank you very much for your help @PhDeezNutz !
 
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Likes PhDeezNutz
Looks great!
 
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Likes Hari Seldon

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