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Motion in a constant uniform magnetic field Section 21

Motion in a constant uniform magnetic field Section 21

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Page 1: Motion in a constant uniform magnetic field Section 21

Motion in a constant uniform magnetic field

Section 21

Page 2: Motion in a constant uniform magnetic field Section 21

We want to know the trajectory.

1. Obtain equation of motion for relativistic momentum

Page 3: Motion in a constant uniform magnetic field Section 21

2. Use equations of relativistic dynamics to obtain differential equation for velocity.

Here we used that e is constant, since the H-field does not work on the particle.

Take the time derivative of both sides.

Page 4: Motion in a constant uniform magnetic field Section 21
Page 5: Motion in a constant uniform magnetic field Section 21

This is the differential equation for v that we want.

Page 6: Motion in a constant uniform magnetic field Section 21

3. Integrate to obtain velocity vs. time.

Page 7: Motion in a constant uniform magnetic field Section 21

Real part

Imaginary part

vot and a are determined by the initial conditions.

a = the initial phase.

= constant

Page 8: Motion in a constant uniform magnetic field Section 21

4. Integrate again to obtain coordinates vs. time.

pt = projection of the momentum in the XY plane.

Page 9: Motion in a constant uniform magnetic field Section 21

Trajectory is helix with constant speed along z. Angular rotation frequency = .w

Page 10: Motion in a constant uniform magnetic field Section 21

Low velocity v <<c

Page 11: Motion in a constant uniform magnetic field Section 21

For an H-field that is uniform on the scale of the particle orbit, the change in magnitude and direction is “Adiabatic”.

Orbit changes only slightly during one period.

Adiabatic invariant (Mechanics)

Projection of the generalized momentum in the plane perpendicular to H.

Integrate over the complete period of motion (circumference of a circle.)

Page 12: Motion in a constant uniform magnetic field Section 21

Stokes.

Surface area element

Bounded surface

Invariant

pt varies as ÖH when H varies

Page 13: Motion in a constant uniform magnetic field Section 21

If H magnitude varies slowly in space…

As electron moves through changing field,H appears to be changing temporally in magnitude, while remaining spatially uniform to the charge.

stronger

Page 14: Motion in a constant uniform magnetic field Section 21

Energy (and p2) remain constant, since H does no work. (e2 = m2c4+ p2c2).

The longitudinal component of p º pl, p2 = pl2 + pt

2.

Penetration into regions with p2 < CH is impossible.

Positive definite

Page 15: Motion in a constant uniform magnetic field Section 21

Radius of helix decreases as H increases.

Step per cycle

Particle is then reflected

(21.6)

Page 16: Motion in a constant uniform magnetic field Section 21

Inhomogeneity of H causers a drift of the guiding center transverse to H.

Page 17: Motion in a constant uniform magnetic field Section 21

What is the relativistically correct trajectory of an electron in a constant uniform magnetic field?

• A cycloid• A catenary• A helix

Page 18: Motion in a constant uniform magnetic field Section 21

Magnetic bottle

Page 19: Motion in a constant uniform magnetic field Section 21

Magnetic bottle

• The radius of the helix decreases as H increases. • The longitudinal step per cycle decreases as H increases.• Eventually, the particle is reflected.

Page 20: Motion in a constant uniform magnetic field Section 21

Naturally occurring magnetic bottle