In the calculus of variations and classical mechanics, the Euler-Lagrange equations is a system of second-order ordinary differential equations whose solutions are stationary points of the given action functional. The equations were discovered in the 1750s by Swiss mathematician Leonhard Euler and Italian mathematician Joseph-Louis Lagrange.
Because a differentiable functional is stationary at its local extrema, the Euler–Lagrange equation is useful for solving optimization problems in which, given some functional, one seeks the function minimizing or maximizing it. This is analogous to Fermat's theorem in calculus, stating that at any point where a differentiable function attains a local extremum its derivative is zero.
In Lagrangian mechanics, according to Hamilton's principle of stationary action, the evolution of a physical system is described by the solutions to the Euler equation for the action of the system. In this context Euler equations are usually called Lagrange equations. In classical mechanics, it is equivalent to Newton's laws of motion, but it has the advantage that it takes the same form in any system of generalized coordinates, and it is better suited to generalizations. In classical field theory there is an analogous equation to calculate the dynamics of a field.
Below is the question:
[PLAIN]http://img706.imageshack.us/img706/7549/42541832.jpg
I don't even know where to start. Theres nothing about this topic in my notes & I can't remember doing it before. I've tried searching for the key words but that didn't help much.
Does anyone have any...
I don't mean the actual definition of the Euler-Lagrange equation per-se, but rather a word definition that's slipping my mind. I remember that if you want to measure the shortest distance between two points, you have to minimize an integral of all possible paths or something. Is that thing...
I have a Lagrangian L = \frac{R^2}{z^2} ( -\dot{t}^2 +\dot{x}^2 +\dot{y}^2 +\dot{z}^2) and I want to find the Euler-Lagrange equations \frac{\partial L}{\partial q} = \frac{d}{ds} \frac{\partial L}{\partial \dot{q}}
I'm fine with the LHS and the partial differentiation on the RHS, but when it...
In the book Mathematical Methods for Engineers and Scientists 3, the derivation of the Euler-Lagrange equation starts roughly along the lines of this:
In order to minimize the functional I=\int_{x_1}^{x_2}{f(x,y,y')dx}, one should define two families of functions Y(x) and Y'(x), where Y(x) is...
I am trying to derive the dynamic equations of an aerial vehicle with 6 degrees of freedom (a quadrotor to be precise). I am using
- two coordinate systems: the Earth frame and the body frame;
- the Euler-Lagrange formalism: generalized coordinates {x,y,z,phi,theta,psi}, respectively, the...
Hi,
I am having a calculus class now and these days the instructor is introducing the Euler-Lagrange differential equation. I have no idea why the formula (general form) is like that way. Is anyone here know how to interprete the formula and help me to understand it?
dF/df-(d/dx)dF/df'=0...
Hi,
I am trying to follow a derivation of the euler lagrange equations in one of my textbooks. It says that
\int ( f\frac{dL}{dx} + f'\frac{dL}{dx'}) dt
=
f\frac{dL}{dx'} + \int f ( \frac{dL}{dx} - \frac{d}{dt}(\frac{dL}{dx'}) ) dt
where f is an arbitrary function and L is the...
Homework Statement
The metric is:
ds^{2} = y^{2}(dx^{2} + dy^{2})
I have to find the equation relating x and y along a geodesic.The Attempt at a Solution
ds = \sqrt{ydx^{2} + ydy^{2}} - is this right?
ds = \sqrt{y + yy'^{2}} dx
F = \sqrt{y + yy'^{2}}
So then I apply the Euler-Lagrange...
Hi,
I am trying to minimize:
\int_0^\infty{\exp(-t)(t\,f'(t)-f(t))^2\,dt}
by choice of f, subject to f(0)=1 and f'(x)>0 for all x.
The (real) solution to the Euler-Lagrange differential equation is:
f(t)={C_1}t
rather unsurprisingly. However, this violates f(0)=1.
If...
If we have a functional
J(y)=\int L(y,y',x)dx
then the first variation is
\delta J=\int\left(\frac{\partial L}{\partial y}\eta(x)+\frac{\partial L}{\partial y'}\eta'(x)\right)dx,
where \eta(x) is the variation of the stationary solution. Now, if L is independent of y(x), then...
Homework Statement
Show that the Lagrangian density:
L=- 1/2 [\partial_\alpha \phi_\beta ][\partial^\alpha \phi^\beta ]+1/2 [\partial_\alpha \phi^\alpha ][\partial_\beta \phi^\beta ]+1/2 \mu^2 \phi_\alpha \phi^\alpha
for the real vector field \phi^\alpha (x) leads to the field equations...
I have the following Lagrangian:
\mathcal{L} = 1/2 \partial_{\mu} \varphi \partial^{\mu} \varphi - 1/2 b ( \varphi^{2} - a^{2} )^{2} , where a,b \in \mathbb{R}_{>0} and \varphi is a real (scalar) field and x are spacetime-coordinates.
I calculated the Euler-Lagrange eq. and get...
I'm in dire need of help in understanding calculus of variations. My professor uses the Mathews and Walker text, second edition, entitled Mathematical Methods of Physics and, he has a tendency to skip around from chapters found towards the beginning of the text to those nearer the end. I...
I am stuck in trying to understand the derivation of the Euler-Lagrange equation. This mathematical move is really bothering me, I can't figure out why it is true.
\frac{\partial f(y,y';x)}{\partial\alpha}=\frac{\partial f}{\partial y}\frac{\partial y}{\partial\alpha}+\frac{\partial...
Homework Statement
If the integrand f(y, y', x) does not depend explicitly on x, that is, f = f(y, y') then
\frac{df}{dx} = \frac{\partial f}{\partial y}y' + \frac{ \partial f } {\partial y' } y''Use the Euler-Lagrange equation to replace \partial f / \partial y on the right and hence show...
I'm trying to deduce the equations of motion in the form
\frac{d}{dt} \frac{\partial \cal L}{\partial \dot{q}} - \frac{\partial \cal L}{\partial q} = 0
with little algebra directly from Hamilton's principle, like the geometric derivation of snell's law from the principle of least time. It...
I'm taking a Physics class at Stanford U. and I am having difficulty understanding how to mathematically understand or translate the Euler-LaGrange equations of motion in both Classical and Quantum Field Theory.
Any sort of English translation, background or hinting as to what type of math I...
Homework Statement
Let P be a rectangle , f_{0} : \partial P \rightarrow R) continuous and Lipschitz, C_{0} = \{ f \in C^{2}(P) : f=f_{0} \ on \ \partial P \}. and finally S : C_{0} \rightarrow R a functional:
S(f) = \int^b_a (\int^d_c (\frac{\partial f}{\partial x})^{2}\,dy)\,dx +...
Homework Statement
I'm asked to get Maxwell's equations using the Euler-lagrange equation:
\partial\left(\frac{\partial L}{\partial\left\partial_{\mu}A_{\nu}\right)}\right)-\frac{\partial L}{\partial A_{\nu}}=0
with the EM Langrangian density...
Hi, I have some questions which I encountered during my thesis-writing, I hope some-one can help me out on this :)
First, I have some problems interpreting coordinate-transformations ( "active and passive") and the derivation of the Equations of Motion. We have
S = \int L(\phi...
Euler-Lagrange equations in QFT??
Hi,
I have a problem with a Wikipedia entry::bugeye:
http://en.wikipedia.org/wiki/Euler-Lagrange_equation
The equations of motion in your quantized theory (2nd quantization) are d/dtF^=[F^,H^] i.e the quantized version of d/dtF={F,H}. My notation: F^ is the...
This is a question that I'm asking myself for my own understanding, not a homework question.
I realize that in most derivations of the Euler-Lagrange equations the coordinate system is assumed to be general. However, just to make sure, I want to apply the "brute force" method (as Shankar...
I'll just throw down some definitions and then ask my question on this one.
In a conservative system, the Lagrangian, in generalised coordinates, is defined as the kinetic energy minus the potential energy.
L=L(q_i,\dot{q}_i,t) = K(q_i,\dot{q}_i,t) - P(q_i,t).
All q_i here being functions...
This is not a homework question but one that is part of the course material and I can't really move on until I understand the basic calculus.
I have a problem interpreting "d by dx of partial dF by dy' equals partial d by dy' of dF by dx" in the following question, which I set out and then...
I have a classical mechanics question I couldn't conclude. The reason seems to be mathematical. It's this:
There's a paraboloid shaped plane of mass M, which is standing on a frictionless surface and can slide freely. It's surface is y=ax^2. A point mass m is place on the plane. Solve the...
So, I've been reading Thornton and Marion's "Classical Dynamics of Particles and Systems" and have gotten to the chapter on the calculus of variations. In trying the end of chapter problems, I find I'm totally baffled by 6-9: given the volume of a cylinder, find the ratio of the height to the...
Hi its me again, stuck once more. Sorry guys and gals :P
Ok a problem I found on http://en.wikipedia.org/wiki/Action_%28physics%29
In a 1-D case how do we get from:
\delta S = \int_{t_1}^{t_2} [L(x + \varepsilon, \dot{x} + \dot{\varepsilon})-L(x,\dot{x})]dt
to:
\delta S = \int_{t_1}^{t_2}...
hey, In my physics class we are now learinging beginging to learn about lagrange ion mechanics and I am a little stuck on the basics of it particularly fermat's principle (dealing with light travel) and applications of the Euler-Lagrange Equation, I can't seem to get many of the problems at the...