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Published byRoderick Perry Modified over 9 years ago
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Motion in a constant uniform magnetic field Section 21
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We want to know the trajectory. 1.Obtain equation of motion for relativistic momentum
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2. Use equations of relativistic dynamics to obtain differential equation for velocity. Here we used that is constant, since the H-field does not work on the particle. Take the time derivative of both sides.
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This is the differential equation for v that we want.
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3. Integrate to obtain velocity vs. time.
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Real part Imaginary part v ot and are determined by the initial conditions. = the initial phase. = constant
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4. Integrate again to obtain coordinates vs. time. p t = projection of the momentum in the XY plane.
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Trajectory is helix with constant speed along z. Angular rotation frequency =
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Low velocity v <<c
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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.)
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Stokes. Surface area element Bounded surface Invariant p t varies as H when H varies
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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
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Energy (and p 2 ) remain constant, since H does no work. ( 2 = m 2 c 4 + p 2 c 2 ). The longitudinal component of p p l, p 2 = p l 2 + p t 2. Penetration into regions with p 2 < CH is impossible. Positive definite
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Radius of helix decreases as H increases. Step per cycle Particle is then reflected (21.6)
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Inhomogeneity of H causers a drift of the guiding center transverse to H.
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What is the relativistically correct trajectory of an electron in a constant uniform magnetic field? A cycloid A catenary A helix
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Magnetic bottle
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The radius of the helix decreases as H increases. The longitudinal step per cycle decreases as H increases. Eventually, the particle is reflected.
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Naturally occurring magnetic bottle
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