---
title: "Lagrangian mechanics"
firstLetter: "L"
publishDate: 2021-07-01
categories:
- Physics

date: 2021-07-01T18:44:43+02:00
draft: false
markup: pandoc
---

# Lagrangian mechanics

**Lagrangian mechanics** is a formulation of classical mechanics,
which is equivalent to Newton's laws,
but offers some advantages.
Its mathematical backbone is the
[calculus of variations](/know/concept/calculus-of-variations/).

For a moving object with position $x(t)$ and velocity $\dot{x}(t)$,
we define the Lagrangian $L$ as the difference
between its kinetic and potential energies:

$$\begin{aligned}
    \boxed{
        L(x, \dot{x}, t) \equiv T - V = \frac{1}{2} m \dot{x}^2 - V(x)
    }
\end{aligned}$$

From variational calculus we then get the Euler-Lagrange equation,
which in this case turns out to just be Newton's second law:

$$\begin{aligned}
    \dv{t} \Big( \pdv{L}{\dot{x}} \Big) = \pdv{L}{x}
    \qquad \implies \qquad
    m \ddot{x} = - \pdv{V}{x} = F
\end{aligned}$$

But compared to Newtonian mechanics,
Lagrangian mechanics scales better for large systems.
For example, to describe the dynamics of $N$ objects $x_1(t), ..., x_N(t)$,
we only need a single $L$
from which the equations of motion can easily be derived.
Getting these equations directly from Newton's laws could get messy.

At no point have we assumed Cartesian coordinates:
the Euler-Lagrange equations keep their form
for any independent coordinates $q_1(t), ..., q_N(t)$:

$$\begin{aligned}
    \dv{t} \Big( \pdv{L}{\dot{q_n}} \Big) = \pdv{L}{q_n}
\end{aligned}$$

We define the **canonical momentum conjugate** $p_n(t)$
and the **generalized force conjugate** $F_n(t)$ as follows,
such that we can always get Newton's second law:

$$\begin{aligned}
    \boxed{
        p_n \equiv \pdv{L}{\dot{q}_n} \qquad F_n \equiv \pdv{L}{q_n}
    }
    \qquad \implies \qquad
    \dv{p_n}{t} = F_n
\end{aligned}$$

But this is actually a bit misleading,
since $p_n$ need not be a momentum, nor $F_n$ a force,
although often they are.
For example, $p_n$ could be angular momentum, and $F_n$ torque.

Another advantage of Lagrangian mechanics is that
the conserved quantities can be extracted from $L$ using Noether's theorem.
In the simplest case, if $L$ does not depend on $q_n$
(then known as a **cyclic coordinate**),
then we know that the "momentum" $p_n$ is a conserved quantity:

$$\begin{aligned}
    F_n = \pdv{L}{q_n} = 0
    \qquad \implies \qquad
    \dv{p_n}{t} = 0
\end{aligned}$$

Now, as the number of particles $N$ increases to infinity,
variational calculus will give infinitely many coupled equations,
which is obviously impractical.

Such a system can be regarded as continuous, so the $N$ functions $q_n$
can be replaced by a single density function $u(x,t)$.
This approach can also be used for continuous fields,
in which case the complex conjugate $u^*$ is often included.
The Lagrangian $L$ then becomes:

$$\begin{aligned}
    L(u, u^*, u_x, u_x^*, u_t, u_t^*, x, t)
    = \int_{-\infty}^\infty \mathcal{L}(u, u^*, u_x, u_x^*, u_t, u_t^*, x, t) \dd{x}
\end{aligned}$$

Where $\mathcal{L}$ is known as the **Lagrangian density**.
By inserting this into the functional $J$
used for the derivation of the Euler-Lagrange equations, we get:

$$\begin{aligned}
    J[u]
    = \int_{t_0}^{t_1} L \dd{t}
    = \int_{t_0}^{t_1} \int_{-\infty}^\infty \mathcal{L} \dd{x} \dd{t}
\end{aligned}$$

This is simply 2D variational problem,
so the Euler-Lagrange equations will be two PDEs:

$$\begin{aligned}
    0 &= \pdv{\mathcal{L}}{u} - \pdv{x} \Big( \pdv{\mathcal{L}}{u_x} \Big) - \pdv{t} \Big( \pdv{\mathcal{L}}{u_t} \Big)
    \\
    0 &= \pdv{\mathcal{L}}{u^*} - \pdv{x} \Big( \pdv{\mathcal{L}}{u_x^*} \Big) - \pdv{t} \Big( \pdv{\mathcal{L}}{u_t^*} \Big)
\end{aligned}$$

If $\mathcal{L}$ is real,
then these two Euler-Lagrange equations will in fact be identical.

Finally, note that for abstract fields,
the Lagrangian density $\mathcal{L}$ rarely has
a physical interpretation, and is not unique.
Instead, it must be reverse-engineered from a relevant equation.



## References
1.  R. Shankar,
    *Principles of quantum mechanics*, 2nd edition,
    Springer.