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Table 1:

Mass, energy and luminosity budgets of the preshock and postshock gas in the Stephan's Quintet galaxy-wide shock, directly inferred from observationsa.
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\begin{tabular}{c\vert c c c \vert c c c c c}
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& & & & & & & & \\
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a All the numbers are scaled to our aperture ( ${\cal A} = 5.2$ $\times $ 2.1 kpc2) where Spitzer observations were performed. The preshock gas is mainly the H I gas contained in the tidal tail of NGC 7319. After the shock, the mass is distributed between the hot X-ray emitting plasma and the $\rm H_2$ gas (see text for details). Before the shock, most of the energy available is the kinetic energy of the H I gas that will be shocked. The shock splits the energy budget in two parts: thermal and kinetic energy. The former is stored in the hot plasma whereas the latter goes into turbulent motions that heat the $\rm H_2$ gas. Observations show that mechanical energy is the dominant energy reservoir.
b XMM-Newton observations of the extended X-ray emission in the shock and the tidal tail (Trinchieri et al. 2005).
c H$~ \alpha$ and O I optical line observations by Xu et al. (2003).
d Based on extrapolation of H I observations in the tidal tail by Williams et al. (2002); Sulentic et al. (2001).
e From Spitzer IRS observations. The $\rm H_2$ line flux is summed over the S(0) to S(5) lines (Appleton et al. 2006).
f This bulk kinetic energy is a lower limit because an unknown mass of turbulent cold molecular gas can contribute to this energy.
g Luminosities are indicated assuming a distance to SQ of 94 Mpc.

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