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A Brief Introduction to Space Plasma Physics.pdf - Institute of ...

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– Average random energy<br />

r r 2<br />

− = ∫<br />

2 r r r<br />

1<br />

ms ( v us<br />

) ms<br />

( v − us<br />

) fs<br />

(<br />

, v,<br />

t)<br />

dv / fs<br />

(<br />

, v,<br />

t)<br />

dv<br />

r<br />

1<br />

2<br />

2<br />

– The partial pressure <strong>of</strong> s is given by<br />

p<br />

n<br />

s<br />

s<br />

2<br />

N<br />

=<br />

( ) 2 3r −<br />

1 2<br />

(<br />

2ms<br />

( v us<br />

)<br />

where N is the number <strong>of</strong> independent velocity components<br />

(usually 3).<br />

r<br />

∫<br />

– In equilibrium the phase space distribution is a Maxwellian<br />

distribution<br />

r r<br />

⎡ 1<br />

2<br />

r r<br />

( )<br />

( − ) ⎤<br />

2<br />

ms<br />

v us<br />

fs<br />

, v = As<br />

exp⎢<br />

⎥⎦<br />

⎣ kTs<br />

where<br />

A<br />

s<br />

= n<br />

s<br />

m<br />

2π<br />

kT

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