What is Lagrangian mechanics, and what's the difference compared to Newtonian mechanics? I'm a mathematician/computer scientist, not a physicist, so I'm kind of looking for something like the explanation of the Lagrangian formulation of mechanics you'd give to someone who just finished a semester of college physics.

Things I'm hoping to have explained to me:

  • What's the overall difference in layman's terms? From what I've read so far, it sounds like Newtonian mechanics takes a more local "cause-and-effect"/"apply a force, get a reaction" view, while Lagrangian mechanics takes a more global "minimize this quantity" view. Or, to put it more axiomatically, Newtonian mechanics starts with Newton's three laws of motion, while Lagrangian mechanics starts with the Principle of Least Action.
  • How do the approaches differ mathematically/when you're trying to solve a problem? Kind of similar to above, I'm guessing that Newtonian solutions start with drawing a bunch of force vectors, while Lagrangian solutions start with defining some function (calculating the Lagrangian...?) you want to minimize, but I really have no idea.
  • What are the pros/cons of each approach? What questions are more naturally solved in each? For example, I believe Fermat's Principle of Least Time is something that's very naturally explained in Lagrangian mechanics ("minimize the time it takes to get between these two points"), but more difficult to explain in Newtonian mechanics since it requires knowing your endpoint.
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    $\begingroup$ Lagrangian formulation is what you obtain when you consider systems that are defined on "curved spaces" (in a sense that I won't make precise, but think e.g. about pendulum constrained to a circle). In Newtonian picture you need to include reaction forces that keep the particles glued to that space (thought of as a subspace of some $N$-dimensional Euclidean space). Lagrangian mechanics takes this burden off your shoulders and lets you talk about the "curved" configuration space directly and just focus on the way particles interact there intrinsically. $\endgroup$
    – Marek
    Commented Apr 20, 2011 at 20:40
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    $\begingroup$ This short, basic essay might help give you an idea of how the two are related: arxiv.org/abs/physics/0004029 $\endgroup$
    – Griffin
    Commented Jun 18, 2013 at 1:40
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    $\begingroup$ @grautur: Lagrange's equations can be derived by many ways; one of them is principle of least action. Other ways include d'Alembert's principle. So your last statement in 1st dot above is not strictly correct. $\endgroup$
    – atom
    Commented Sep 13, 2017 at 6:15

7 Answers 7


In Newtonian mechanics you have to use mainly rectangular co ordinate system and consider all the constraint forces. Lagrange's scheme avoids the considerations of the constraint forces deftly and you can use any set of "generalized coordinates" like angle, radial distance etc. consistent with the constraint relations. The number of those generalized coordinates are the same with the number of degrees of freedom of the system.

In all dynamical systems we arbitrarily choose some generalized co ordinates consistent with the constraints of the system. In Newtonian mechanics, the difference between the kinetic and potential energy of the system gives you the so called Lagrangian. Then we have n number of differential equations. $n$ is the number of degrees of freedom of the system.

The main advantage of Lagrangian mechanics is that we don't have to consider the forces of constraints and given the total kinetic and potential energies of the system we can choose some generalized coordinates and blindly calculate the equation of motions totally analytically unlike Newtonian case where one has to consider the constraints and the geometrical nature of the system.

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    $\begingroup$ Mostly right, but we're free to use whatever coordinate system we like in Newtonian mechanics, too, so long as we take care to use the curvilinear differential operators when working in non-rectangular coordinates. $\endgroup$ Commented Apr 20, 2011 at 3:30
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    $\begingroup$ @Jerry: That's why I have written "mainly". $\endgroup$
    – user1355
    Commented Apr 20, 2011 at 3:32
  • $\begingroup$ @JerrySchirmer Could you give an example? How do you represent velocities in an arbitrary coordinate system in Newtonian mechanics? If for example one coordinate is an angle, then its time derivative will just be an angular velocity and not a proper velocity. How is this taken care of? $\endgroup$ Commented Nov 9, 2021 at 4:59
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    $\begingroup$ @HelloGoodbye given $\ddot x=F(x,\dot x)$, we can always change variables and obtain the corresponding equation in another coordinate system. The problem is that the new equation won't in general have the form $\ddot q=\tilde F(q,\dot q)$. For example (in very compact notation), if $\ddot x=F$, then $\partial_t^2(f\circ x)=(\partial^2 f)\dot x^2+(\partial f)F$. You make this into an equation for $f\circ x$ and its time derivative, and you get your equation in the new variables (e.g. angles from Cartesians). Contrast this with EL equations, which look the same in all coordinates $\endgroup$
    – glS
    Commented Jan 27, 2022 at 17:07

To answer the second part of your question, I will give a classic example of harmonic motion. The potential energy of a spring is $U=\frac{1}{2}kx^2$, where $k$ is the spring constant and $x$ is the displacement.

Newtonian Mechanics:


So $m\frac{d^2x}{dt^2}=-kx$, which is an easy differential equation.

Lagrangian Mechanics:

First we know the Euler-Lagrange Equations $\frac{\partial L}{\partial q} = \frac{d}{dt}\frac{\partial L}{\partial \dot{q}}$, we identify coordinates $q=x$, and we define our Lagrangian $L=T-V$ ($T$ is kinetic energy and $V$ is potential energy).



So we plug this all into our little Euler Lagrange Equation, and, solving through, you get (drum roll), $m\frac{d^2x}{dt^2}=-kx$!


So after all of this we get the same equation as with Newtonian mechanics and with a lot more work right? In this example probably, and most other simple systems. However, Lagrangian Mechanics has some very powerful applications.

Consider the following system: You have multiple pendula connected by springs, and each pendulum begins with some initial position and velocity. How do you go about solving this system? In Newtonian Mechanics it will get extremely complex to work out all the forces involved. However, taking a Lagrangian perspective, much of the hard work is taken care of as you can easily define $q_i=\theta_i$, $\theta$ being the angular displacement of each the pendulum. And instead of having to deal with the various forces you just deal with the potential and kinetic energy.

An even more, exponentially more, important application is in classical field theory (I know it has some important connections to with QFT, but I am not in any position to knowledgeably comment on that). Electromagnetism and General Relativity are two excellent examples. You can derive Maxwell's equations entirely from the electromagnetic Lagrangian ( $L=-\frac{1}{4}F_{\mu\nu}F^{\mu\nu}+A_{\mu}J^\mu$) and you can derive extremely important results in general relativity from the Hilbert Action ($S_H=\int \sqrt{-g}Rd^nx$) and similar variational principles.

  • Lagrangian mechanics can be derived from Principle of Least Action, or from Newtonian mechanics. This is not a fundamental difference.
  • Pretty much. In Newtonian mechanics you start with drawing a bunch of vectors and then list your equations. In Lagrangian mechanics you first identify all constraints, choose generalized coordinates, then write down Lagrangian, and plug it into the Lagrangian equation $\frac{d}{dt}\frac{\partial L}{\partial \dot{q_i}}-\frac{dL}{dq_i}=0$
    • Lagrangian mechanics are better when there are lots of constraints. The more the constraints, the simpler the Lagrangian equations, but the more complex the Newtonian become. Lagrangian mechanics is not very suited for non-ideal or non-holonomic systems, such as systems with friction.
    • Lagrangian mechanics is also much more extensible. It can remain almost the same form in hydrodynamics, electrodynamics, electric circuits, special and general relativity, etc.
    • Principle of Least Time is closely related to Principle of Least Action, but they are in fact very different. I don't see how you can derive the former from the latter.

The Lagrangian formulation assumes that in a system, the forces of constraints don't do any work, they only reduce the number degrees of freedom of the system. So one need not know the form of force the constraint forces have unlike Newtonian mechanics!!!


main advantage of lagrangian and hamiltonian mechanics over Newtonian mechanics we can deal with scalar quantities , energy, whereas in the later we have to deal with vector quantities. Besides this we can approach easily to any system ( e.g. mechanical, electrical, optical etc.) with the lagrangian and Hamiltonian mechanics. But this easy acess can not be achieved with NEWTONIAN MECHANICS.


It is all about Frame of reference. In Newtonian physics you stand at a point and watch something move in relation to the stationary observation point based on forces applied. In lagrangian physics you are the something moving that experiences the forces. Reynolds transport theorem relates the two frames of reference.


According to Newton:




As you can see, there is no freedom to choose the trajectory - it is determined with the instant values of force and velocity. "Future" is determined with "present".

A particle never "chooses" the optimal trajectory to go from a known position in the past $r(t_1)$ to a known position in the future $r(t_2)$. The future data are not involved in the dynamics. But the least action "principle", apart from good equations, is based on the future data $r(t_2)$ which is mathematically possible but physically meaningless.

There is no a "least action principle" proceeding only from the initial data. Instead, the Newton equations with the initial data suffice to solve physical problems ;-)

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    $\begingroup$ @Vladimir: Lagrangian mechanics works just fine in the limit of short time scales: the theory is every bit as local as Newtonian mechanics, and can be derived directly from Newtonian mechanics (say the way Legrange did it before Hamilton ever talked about Least Action). These two methods (and indeed Hamiltonian mechanics) are equivalent; its just that sometimes one is more convenient that the other. $\endgroup$ Commented Apr 21, 2011 at 22:01
  • $\begingroup$ @dmckee I agree that they are equivalent when they are applied as the "initial data" problems. I disagree that they are equivalent if one keeps searching an "optimum trajectory" with help of known future position. The future position is never known. And I see how misleading is the least action "ideology". However, I appreciate the Noether way of constructing some conserved quantities. $\endgroup$ Commented Apr 21, 2011 at 22:07
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    $\begingroup$ @Vladimir: I am afraid you don't understand the meaning and beauty of the least action principle. Given initial and final position what should be the dynamical equation of motion for a particle to make the action stationary? The answer would be Euler Lagrange equation. This is an enormously powerful way of thinking about classical mechanics and indeed even quantum mechanics!! $\endgroup$
    – user1355
    Commented Apr 22, 2011 at 4:38
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    $\begingroup$ @Vlad: Your mistake is considering the least action principle as an initial and final value "problem under classical mechanics". It is not an ideology and let me tell you politely that you are extremely confused to say the least. $\endgroup$
    – user1355
    Commented Apr 22, 2011 at 4:41
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    $\begingroup$ @Vladimir, the stationary action principle in this case comes from D'Alembert's principle and its integration over time. It's not something plucked from the air as a postulate. $\endgroup$ Commented Apr 22, 2011 at 11:35

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