four-potential of a field section 16. for a given field, the action is the sum of two terms s = s m...

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Four-potential of a field Section 16

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Page 1: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Four-potential of a field

Section 16

Page 2: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

For a given field, the action is the sum of two terms

• S = Sm + Smf

– Free-particle term– Particle-field interaction term

• Smf is determined by properties of the particle and properties of the field.

• By experiment:– The important property of the particle is its charge

e.– Properties of the field are determined by a 4-vector.

Page 3: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

The 4-potential of the field is denoted by Ai.

• Components of Ai are functions of coordinates and time.

• The action S must be a scalar• The action must be an integral along the world

line of the particle from event “a” to event “b”.

Page 4: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Four potential

• Ai = (f, A)– Time part A0 = f = scalar potential– Space part A = 3D “vector potential”

Page 5: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Particle’s velocity

t1

Page 6: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Since

The Lagrangian for a particle in given fields is

Free particle term (8.2)Term for interaction of particle with given fields.

Page 7: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Generalized momentum

Ordinary relativistic moment of the particle.

Page 8: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Hamiltonian of charges in given fields

Page 9: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

H

Must be expressed in terms of p, not v, to be a proper Hamiltonian.Then A will appear.

Total energy e0 of a free particle, kinetic + rest energy, in absence of field.

Page 10: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Hamiltonians must be functions of p, not v.

Ordinary particle momentum

Generalized momentum

Page 11: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Classical Lagrangian for charge in given fields

Low velocities

Binomial expansion

Constant terms in a Lagrangian do not affect the equations of motion.Rest energy is unimportant in classical limit.

Page 12: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Classical Hamiltonian of charge in given fields.

Ordinary particle momentum

Binomial expansion

Constants don’t affect Hamilton’s equations of motion

Hamiltonian

Page 13: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

Hamilton-Jacobi Equation

Hamilton-Jacobi equation for particle in given fields.

Will be used in Chapter on geometrical optics.

Page 14: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

What does the field contribute to the generalized momentum?

• A term linear in scalar potential• A term linear in vector potential• A term quadratic in particle velocity to lowest

order.

Page 15: Four-potential of a field Section 16. For a given field, the action is the sum of two terms S = S m + S mf – Free-particle term – Particle-field interaction

What does the field contribute to the generalized momentum of a particle?

• A term linear in scalar potential• A term linear in vector potential• A term quadratic in particle velocity to lowest

order.