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The_Cambridge_Handbook_of_Physics_Formulas

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7.9 Plasma physics<br />

159<br />

Synchrotron radiation<br />

Power radiated<br />

by a single<br />

electron a<br />

... averaged<br />

over pitch<br />

angles<br />

Single electron<br />

emission<br />

spectrum b<br />

Characteristic<br />

frequency<br />

Spectral<br />

function<br />

( P tot =2σ T cu mag γ 2 v<br />

) 2<br />

sin 2 θ (7.286)<br />

c<br />

(<br />

≃ 1.59×10 −14 B 2 γ 2 v<br />

) 2<br />

sin 2 θ W<br />

c<br />

(7.287)<br />

P tot = 4 ( 3 σ Tcu mag γ 2 v<br />

) 2<br />

(7.288)<br />

c<br />

(<br />

≃ 1.06×10 −14 B 2 γ 2 v<br />

) 2<br />

W (7.289)<br />

c<br />

P (ν)= 31/2 e 3 B sinθ<br />

4πɛ 0 cm e<br />

F(ν/ν ch ) (7.290)<br />

≃ 2.34×10 −25 B sinθF(ν/ν ch )<br />

WHz −1<br />

(7.291)<br />

ν ch = 3 eB<br />

2 γ2 sinθ<br />

2πm e<br />

(7.292)<br />

≃ 4.2×10 10 γ 2 B sinθ Hz (7.293)<br />

∫ ∞<br />

F(x)=x K 5/3 (y)dy (7.294)<br />

x<br />

{<br />

≃<br />

2.15x 1/3 (x ≪ 1)<br />

1.25x 1/2 e −x (x ≫ 1)<br />

(7.295)<br />

a This expression also holds for cyclotron radiation (v ≪ c).<br />

b I.e., total radiated power per unit frequency interval.<br />

P tot total radiated power<br />

σ T Thomson cross section<br />

u mag magnetic energy<br />

density = B 2 /(2µ 0 )<br />

v electron velocity (∼ c)<br />

γ Lorentz factor<br />

=[1−(v/c) 2 ] −1/2<br />

θ pitch angle (angle<br />

between v and B)<br />

B magnetic flux density<br />

c speed <strong>of</strong> light<br />

P (ν) emission spectrum<br />

ν frequency<br />

ν ch characteristic frequency<br />

−e electronic charge<br />

ɛ 0 free space permittivity<br />

m e electronic (rest) mass<br />

F spectral function<br />

K 5/3 modified Bessel fn. <strong>of</strong><br />

the 2nd kind, order 5/3<br />

1<br />

0.5<br />

0<br />

F(x)<br />

1 x 2 3 4<br />

7

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