Physics Notes - Herong's Tutorial Notes - v3.24, by Herong Yang
What Is Lagrangian
This section provides a quick introduction to the Lagrangian, which is a derived property of a mechanical system defined as the difference of kinetic energy and potential energy of the system.
What Is Lagrangian? Lagrangian, L, is a derived property of a a mechanical system defined as the difference of kinetic energy and potential energy of the system:
L = T - V (G.1) # T is the kinetic energy # V is the potential energy # L the difference of kinetic energy and potential energy
When a mechanical system changes over time, t, the value of Lagrangian may change too. The kinetic energy, the potential energy and Lagrangian of the system can be viewed as functions of t. So Lagrangian can also be expressed as:
L(t) = T(t) - V(t) (G.1)
Now let's compare it with the Hamiltonian of the system introduced earlier in the book:
H(t) = T(t) + V(t) (H.1) # H is the total of kinetic energy and potential energy
So Lagrangian L is related to Hamiltonian H through the following equation:
H = 2*T - L or: H(t) = 2*T(t) - L(t)
The physical meaning of Hamiltonian is much easier to understand than the Lagrangian function. Hamiltonian function can be directly related to the Law of conservation of Energy For an isolated conservative system, the derivative of Hamiltonian against time is zero:
T(t) + V(t) = constant H(t) = constant (H.2) or: dH/dt = 0 (H.3)
Lagrangian was introduced by Joseph-Louis Lagrange (1736-1813), an Italian mathematician and astronomer.
Lagrangian for a Single Object
For a single object, the kinetic energy, T, can be expressed as:
T = 0.5*m*v*v # m is the mass of the object # v is the velocity of the object
So the Lagrangian for a single object can be expressed as:
L = T - V or: L = 0.5*m*v*v - V # T = 0.5*m*v*v applied
If we apply the Hamiltonian definition to Lagrangian, we can have:
L = T - V or: L = 2*T - H # H = T + V applied or: L = m*v*v - H # T = 0.5*m*v*v applied or: L = p*v - H # p is the momentum defined as p = m*v
Table of Contents
Introduction of Frame of Reference
Introduction of Special Relativity
Time Dilation in Special Relativity
Length Contraction in Special Relativity
The Relativity of Simultaneity
Minkowski Spacetime and Diagrams
Action - Integral of Lagrangian
Action - Functional of Position Function x(t)
Hamilton's Principle - Stationary Action
Other Proofs of the Lagrange Equation
Lagrange Equation on Free Fall Motion
Lagrange Equation on Simple Harmonic Motion
Lagrangian in Cartesian Coordinates
Lagrange Equations in Cartesian Coordinates
Introduction of Generalized Coordinates