What Does Stationarity Mean in the Context of the Euler-Lagrange Equations?

In summary, the statement 'the integral of the Lagrange equation is stationary for the path followed by the particle' means that the action, represented by the equation s = \int Ldt, is at a stationary point on the path. This typically corresponds to a minimum, as the action is minimized in real systems. The Euler-Lagrange equations are obtained by setting the variation of the action to 0, which results in a stationary point where the derivative of the function is 0."
  • #1
TheDoorsOfMe
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What does it mean when it says "the integral of the Lagrange equation is stationary for the path followed by the particle"?
 
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  • #2
Is it just saying that the integral is a constant?
 
  • #3
I would assume it means that the action [tex]s = \int Ldt[/tex] is a stationary point (i.e. a min most likely as the action is minimised in real systems).

You might want to wait for some confirmation however as I haven't studied Lagrangian mechanics in too much depth.
 
  • #4
A stationary point is a point where the derivative of a function is 0. To obtain the Euler-Lagrange equations we set the variation of the action to 0.
 
  • #5


The Euler-Lagrange equations are a set of equations used in classical mechanics to describe the motion of a particle. They are derived from the principle of least action, which states that the path a particle takes between two points is the one that minimizes the action, a quantity that combines the particle's kinetic and potential energies.

When it is said that "the integral of the Lagrange equation is stationary for the path followed by the particle," it means that the path the particle takes is the one that results in the minimum value for the integral of the Lagrange equation. In other words, the particle follows a path that minimizes the action, and therefore, the path is considered "stationary" or "unchanging."

This concept is important because it allows us to determine the path a particle will take without having to know the specific forces acting on the particle. Instead, we can use the Euler-Lagrange equations to find the path that minimizes the action and describes the particle's motion. This method is powerful and widely used in physics and engineering to solve a variety of problems involving the motion of particles.
 

1. What are Euler-Lagrange Equations?

Euler-Lagrange Equations are a set of equations used in classical mechanics to describe the motion of a system. They are derived from the principle of least action, which states that the path taken by a system between two points is the one that minimizes the action, a quantity that represents the system's energy.

2. How are Euler-Lagrange Equations derived?

Euler-Lagrange Equations are derived by applying the principle of least action to a Lagrangian function, which is a function that represents the system's kinetic and potential energies. The equations are obtained by taking the derivative of the Lagrangian with respect to the system's generalized coordinates.

3. What is the significance of Euler-Lagrange Equations?

Euler-Lagrange Equations are significant because they provide a powerful tool for solving problems in classical mechanics. They allow us to determine the equations of motion for a system without explicitly solving the differential equations of motion. This makes them particularly useful for complex systems with multiple degrees of freedom.

4. Can Euler-Lagrange Equations be applied to systems without a Lagrangian?

No, Euler-Lagrange Equations can only be applied to systems that have a Lagrangian function. If a system does not have a Lagrangian, then other methods, such as Newton's laws of motion, must be used to determine its equations of motion.

5. How are Euler-Lagrange Equations used in real-world applications?

Euler-Lagrange Equations have a wide range of applications in physics, engineering, and other fields. They are commonly used in the design and analysis of mechanical systems, such as robots and vehicles. They are also used in the study of fluid mechanics, quantum mechanics, and other areas of physics.

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