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Introduction to Relativistic Hydrodynamics

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<strong>Relativistic</strong> hydrodynamics<br />

What is flow?<br />

Two definitions of flow<br />

1. Flow of energy, W µ = 0 (Landau)<br />

Landau, Lifshitz, Fluid mechanics, Pergamon Press (1959)<br />

u µ<br />

L =<br />

T µ ν uν L<br />

<br />

u α L T β α Tβγu γ<br />

L<br />

= 1<br />

ɛ T µ ν uν L<br />

2. Flow of conserved charge, V µ = 0 (Eckart)<br />

Eckart, Phys. Rev. 58, 919 (1940)<br />

u µ<br />

E =<br />

N µ<br />

√<br />

NνN ν<br />

Both definitions are related <strong>to</strong> each other by Lorentz transformations<br />

November 22nd, 2012 | TUD - IKP | D. Nowakowski | 11<br />

u µ<br />

E = Λµ ν uν µ<br />

µ<br />

W V<br />

L , uµ<br />

L ≈ uµ<br />

E + , uµ<br />

ɛ+Ps E ≈ uµ<br />

L + n<br />

uL μ<br />

u E μ<br />

V μ<br />

W μ

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