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PHYS6001, Classical Mechanics, Fall semester 2015 Homework set 7, due Oct 29 2015 1. [10pts] Show that the Lorentz force can be obtained as a generalized force from the “potential” , where and denote the scalar potential and vector potential, the charge, and the velocity of the particle. The electromagnetic field, i.e. the electric and the magnetic fields are related to the potentials by 2. [10pts] The Lagrangian of a system is given in terms of generalized coordinates and by Obtain the Hamiltonian and Hamilton's equations of motion and compare with Lagrange’s equations of motion. 3. [10pts] A spherical pendulum of length with a massless rod is supported at the origin of a coordinate system. Use spherical coordinates as indicated. F = q E + q v × B φ A q v E = −∇φ ( r ) A t B = ∇× A q 1 q 2 L = ! q 1 2 + ! q 2 2 a + bq 1 2 + kq 2 2 + k 2 ! q 1 ! q 2 l

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Page 1: set7

PHYS6001, Classical Mechanics, Fall semester 2015 Homework set 7, due Oct 29 2015

1. [10pts] Show that the Lorentz force ! can be obtained as a generalized force from the “potential”

! ,

where ! and ! denote the scalar potential and vector potential, ! the charge, and ! the velocity of the particle. The electromagnetic field, i.e. the electric and the magnetic fields are related to the potentials by

!

2. [10pts] The Lagrangian of a system is given in terms of generalized coordinates ! and ! by

!

Obtain the Hamiltonian and Hamilton's equations of motion and compare with Lagrange’s

equations of motion.

3. [10pts] A spherical pendulum of length ! with a massless rod is supported at the origin of a coordinate system. Use spherical coordinates as indicated.

!

F = qE + qv × B

φ A q v

E = −∇φ(r )− ∂A∂t

B = ∇× A

q1 q2

L = !q12 +

!q22

a + bq12 + kq2

2 + k2 !q1 !q2

l

Page 2: set7

a) Write the kinetic and potential energy and the Lagrangian in terms of the polar and azimuthal angles ! and !

b) Determine the generalized momenta and the Hamiltonian

c) Write down Hamilton’s equations of motion and compare with previous homework

4) Proof Jacobi's identity for Poisson brackets !

ϕ θ

[u,[v,w]]+ [v,[w,u]]+ [w,[u,v]]= 0