Lagrangian function of a double undamped pendulum

In summary, the ecuations I must obtain are as follows:1. Find the Lagrangian for an undamped pendulum using the diagram shown.2. I get so many different things but I can't reach the desired result.3. I've no idea what to do if all else fails.4. If all else fails, you could try $$T = {1\over 2} m_1\Bigl(\dot x_1^2+\dot y_1^2\Bigr) + {1\over 2} m_2\Bigl(\dot x_2^2+\dot y_2^2\Bigr) $$ but of course you
  • #1
PaBlo14101066
4
1
I must find the Lagrangian for an undamped pendulum using the diagram showed below, I've no idea what to do with the second angle φ2 because is measured from the line that joins the two pivot points.
1605973261966.png

The ecuations I must obtain are as follows
1605973305616.png

I get so many different things but I can't reach the desired result
 
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  • #2
PaBlo14101066 said:
I've no idea what to do
If all else fails, you could try $$T = {1\over 2} m_1\Bigl(\dot x_1^2+\dot y_1^2\Bigr) + {1\over 2} m_2\Bigl(\dot x_2^2+\dot y_2^2\Bigr) $$ but of course you already know how the subscript 1 term ends up, so the work is in the ##m_2## term.

Idem ##V##.
 
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  • #3
BvU said:
If all else fails, you could try $$T = {1\over 2} m_1\Bigl(\dot x_1^2+\dot y_1^2\Bigr) + {1\over 2} m_2\Bigl(\dot x_2^2+\dot y_2^2\Bigr) $$ but of course you already know how the subscript 1 term ends up, so the work is in the ##m_2## term.

Idem ##V##.
Yes, I know, and also there must be a rotational kinetic energy, I made the algebra considering that φ2 is measured from the vertical and obtained
1605974501155.png

But even though I consider $$\phi_2=\phi_1+\phi'$$ I don't get to the equations of the second image
 
  • #4
Don't you get, in terms of ##\hat{x}## and ##\hat{y}##,$$\dot{\mathbf{r}}_1 = l_1 \dot{\varphi}_1 \begin{pmatrix} \cos{\varphi_1} \\ \sin{\varphi_1} \end{pmatrix}$$and$$\dot{\mathbf{r}}_2 = l_3 \dot{\varphi}_1 \begin{pmatrix} \cos{\varphi_1} \\ \sin{\varphi_1} \end{pmatrix}

+ l_2 (\dot{\varphi}_1 + \dot{\varphi}_2) \begin{pmatrix} \cos{(\varphi_1 + \varphi_2)} \\ \sin{(\varphi_1 + \varphi_2)} \end{pmatrix}

$$Now you can find ##\dot{\mathbf{r}}_1 \cdot \dot{\mathbf{r}}_1## and ##\dot{\mathbf{r}}_2 \cdot \dot{\mathbf{r}}_2##. Does that work?
 
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  • #5
etotheipi said:
Don't you get, in terms of ##\hat{x}## and ##\hat{y}##,$$\dot{\mathbf{r}}_1 = l_1 \dot{\varphi}_1 \begin{pmatrix} \cos{\varphi_1} \\ \sin{\varphi_1} \end{pmatrix}$$and$$\dot{\mathbf{r}}_2 = l_3 \dot{\varphi}_1 \begin{pmatrix} \cos{\varphi_1} \\ \sin{\varphi_1} \end{pmatrix}

+ l_2 (\dot{\varphi}_1 + \dot{\varphi}_2) \begin{pmatrix} \cos{(\varphi_1 + \varphi_2)} \\ \sin{(\varphi_1 + \varphi_2)} \end{pmatrix}

$$Now you can find ##\dot{\mathbf{r}}_1 \cdot \dot{\mathbf{r}}_1## and ##\dot{\mathbf{r}}_2 \cdot \dot{\mathbf{r}}_2##. Does that work?
I think that's it, I would have to do the algebra, but as far as it looks, looks fine
 
  • #6
PaBlo14101066 said:
I think that's it, I would have to do the algebra, but as far as it looks, looks fine

Yes, I believe it does indeed get what you're after. The only fiddly part of the calculation is$$
\begin{align*}
\begin{pmatrix} \cos{\varphi_1} \\ \sin{\varphi_1} \end{pmatrix} \cdot \begin{pmatrix} \cos{(\varphi_1 + \varphi_2)} \\ \sin{(\varphi_1 + \varphi_2)} \end{pmatrix} &=

\cos{\varphi_1} \left( \cos{\varphi_1} \cos{\varphi_2} - \sin{\varphi_1} \sin{\varphi_2}\right) + \sin{\varphi_1} \left( \sin{\varphi_1} \cos{\varphi_2} + \cos{\varphi_1} \sin{\varphi_2}\right)

\\
&= \cos{\varphi_2} \left( \cos^2{\varphi_1} + \sin^2{\varphi_1} \right) \\

&= \cos{\varphi_2}

\end{align*}
$$but the rest should fall out okay.
 
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  • #7
etotheipi said:
Yes, I believe it does indeed get what you're after. The only fiddly part of the calculation is$$
\begin{align*}
\begin{pmatrix} \cos{\varphi_1} \\ \sin{\varphi_1} \end{pmatrix} \cdot \begin{pmatrix} \cos{(\varphi_1 + \varphi_2)} \\ \sin{(\varphi_1 + \varphi_2)} \end{pmatrix} &=

\cos{\varphi_1} \left( \cos{\varphi_1} \cos{\varphi_2} - \sin{\varphi_1} \sin{\varphi_2}\right) + \sin{\varphi_1} \left( \sin{\varphi_1} \cos{\varphi_2} + \cos{\varphi_1} \sin{\varphi_2}\right)

\\
&= \cos{\varphi_2} \left( \cos^2{\varphi_1} + \sin^2{\varphi_1} \right) \\

&= \cos{\varphi_2}

\end{align*}
$$but the rest should fall out okay.
Yes, that's it. Thank you very much. You've earned heaven (whatever heaven is to you) :)
 
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Related to Lagrangian function of a double undamped pendulum

1. What is a Lagrangian function?

A Lagrangian function is a mathematical tool used in classical mechanics to describe the dynamics of a physical system. It is defined as the difference between the kinetic energy and potential energy of the system.

2. How is the Lagrangian function used in a double undamped pendulum?

In a double undamped pendulum, the Lagrangian function is used to determine the equations of motion for the two pendulum masses. It takes into account the masses, lengths, and angles of the pendulum as well as the force of gravity.

3. What are the advantages of using the Lagrangian function in a double undamped pendulum?

The Lagrangian function allows for a more elegant and concise representation of the equations of motion compared to other methods. It also takes into account the constraints of the system, making it easier to analyze and solve for the motion of the pendulum.

4. How does the Lagrangian function handle the double pendulum's complex motion?

The Lagrangian function takes into account the kinetic and potential energy of each individual mass in the double pendulum, allowing for a more accurate description of its complex motion. This is especially useful when the pendulum is in a non-linear or chaotic state.

5. Can the Lagrangian function be applied to other physical systems?

Yes, the Lagrangian function can be applied to a wide range of physical systems, including mechanical, electrical, and gravitational systems. It is a powerful tool for analyzing the dynamics of complex systems and is widely used in various branches of physics and engineering.

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