Question

Establish the equivalence of the Hamiltonian equations (21) and Lagrangian ones (11) in an example of the motion of a single point mass in a stationary potential field, considering it in Cartesian coordinates $x, y, z$.

   Establish the equivalence of the Hamiltonian equations (21) and Lagrangian ones (11) in an example of the motion of a single point mass in a stationary potential field, considering it in Cartesian coordinates $x, y, z$.
 
Principles of Mathematical Modelling: Ideas, Methods, Examples
Principles of Mathematical Modelling: Ideas, Methods, Examples
Alexander A.… 1st Edition
Chapter 3, Problem 4 ↓

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In Cartesian coordinates, the Lagrangian is: L = T - V = (1/2)m(ẋ² + ẏ² + ż²) - V(x,y,z) where T is the kinetic energy, V is the potential energy, m is the mass, and áş‹, ẏ, ĹĽ are the velocities in the x, y, z directions.  Show more…

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Establish the equivalence of the Hamiltonian equations (21) and Lagrangian ones (11) in an example of the motion of a single point mass in a stationary potential field, considering it in Cartesian coordinates $x, y, z$.
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Key Concepts

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Lagrangian Mechanics
Lagrangian mechanics is a reformulation of classical mechanics that expresses the dynamics of a system in terms of the Lagrangian function, defined as the difference between kinetic and potential energies. By applying the principle of least action, it leads to the Euler-Lagrange equations which determine the motion of a system along paths that make the action stationary.
Hamiltonian Mechanics
Hamiltonian mechanics offers an alternative formulation to classical mechanics which uses the Hamiltonian function, typically representing the total energy of the system, derived via a Legendre transformation of the Lagrangian. The evolution of the system is then described by Hamilton's canonical equations, which provide first-order differential equations in terms of coordinates and momenta.
Legendre Transformation
The Legendre transformation is a mathematical procedure used to switch from the Lagrangian to the Hamiltonian formulation. It converts the dependency on generalized velocities into a dependency on generalized momenta, thereby facilitating the derivation of Hamilton's equations from the Euler-Lagrange equations.
Equivalence of Formulations
The equivalence of the Lagrangian and Hamiltonian formulations lies in their ability to produce the same equations of motion for a system. By properly applying the Legendre transformation and recognizing the underlying variational principle, one can show that the Hamiltonian canonical equations are mathematically equivalent to the Euler-Lagrange equations obtained in the Lagrangian framework.

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Consider a point particle of mass m whose motion in a two-dimensional plane is constrained by a differentiable function y=f(x) (a) Find the Hamiltonian H. Write down the Hamilton's equations of motion. Note that Hamiltonian H should be a function of x and p, the generalized coordinate and momentum (not generalized velocity). (Hint: the potential term is given by the usual Newtonian gravitational potential, with gravitational acceleration given by g. This gravitational force acts along the y-direction.) (b) Show that p_dot = -dH/dx (1) reproduces the Euler-Lagrange equation. In other words, show that using the Hamiltonian obtained in (a), equation (1) can be rewritten into d/dt(dL/dx_dot) - dL/dx = 0 (2) where L is the Lagrangian for this problem. (c) Work out the expression for dH/dt = d/dt(T + V) (3) but express kinetic term using x_dot instead p. Then show that (2) and (3) give identical results. Therefore, here Euler-Lagrange equation implies energy conservation. This further emphasizes the equivalence between the two formulations of classical mechanics.

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Consider a mass $m$ moving in two dimensions with potential energy $U(x, y)=\frac{1}{2} k r^{2},$ where $r^{2}=x^{2}+y^{2} .$ Write down the Lagrangian, using coordinates $x$ and $y,$ and find the two Lagrange equations of motion. Describe their solutions. [This is the potential energy of an ion in an "ion trap," which can be used to study the properties of individual atomic ions.]

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