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Charge in a constant uniform electric & magnetic field

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Presentation on theme: "Charge in a constant uniform electric & magnetic field"— Presentation transcript:

1 Charge in a constant uniform electric & magnetic field
Section 22

2 We consider non-relativistic motion only. (Why
We consider non-relativistic motion only. (Why? Because otherwise it’s too hard? Or is there a reason that this is all that matters?) Then, p = mv Choose Z || H Choose X &Y so that H & E lie in the YZ plane Z H E Y X

3 Equation of motion Non-relativistic case

4 The Z equation is the easiest.
Integrate twice This is the equation for uniform acceleration in the z direction.

5 Add X and Y equations

6 Cyclotron frequency in Gaussian units
Sum of the solutions of the homogeneous equation and the particular solution.

7 Homogeneous equation Particular solution

8 Complete solution Complex constant Real Now shift the origin of time by a/w to eliminate constant phase.

9 Same as if a = 0. Then b = a. At t = 0, Velocity components are periodic functions of time.

10 Time-averaged values Average X velocity is constant: the drift velocity Perpendicular to both E & H X Y Z H E vD

11 Drift velocity H

12 All derivations in this section assume v << c.
But both fields can be large. In SI units Ey << c B = c m0 H.

13 Trajectory The velocity equations were Integrate
The constant is determined by the initial conditions.

14 What is a cycloid? What is a trochoid?

15

16

17 Trajectory (ignoring constant acceleration along z due to Ez)
X Y Z B E

18 Which trochoid is a cycloid?
1 2 3


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