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===Governing Equations and Supplemental Relations=== We begin with the set of [[PGE#Principal_Governing_Equations|principal governing equations]] that provides the foundation for all of our discussions in this H_Book, except, because we are ignoring the effects of self gravity, <math>~\nabla\Phi</math> is set to zero in the Euler equation and we drop the Poisson equation altogether. Specifically, the relevant set of governing equations is, the <div align="center"> <span id="ConservingMass:Eulerian"><font color="#770000">'''Eulerian Representation'''</font></span><br /> of the Continuity Equation, {{Math/EQ_Continuity02}} <span id="ConservingMomentum:Eulerian"><font color="#770000">'''Eulerian Representation'''</font></span><br /> of the Euler Equation, <math>\frac{\partial\vec{v}}{\partial t} + (\vec{v}\cdot \nabla) \vec{v}= - \frac{1}{\rho} \nabla P </math> <span id="PGE:AdiabaticFirstLaw">Adiabatic Form of the<br /> <font color="#770000">'''First Law of Thermodynamics'''</font></span><br /> {{Math/EQ_FirstLaw02}} . </div> We supplement this set of equations with an ideal gas equation of state, specifically, <div align="center"> {{Math/EQ_EOSideal02}} , </div> in which case the adiabatic form of the <math>1^\mathrm{st}</math> law of thermodynamics may be written as, <div align="center"> <math> \rho \frac{dP}{dt} - \gamma_\mathrm{g} P \frac{d\rho}{dt} = 0 \, . </math> </div> This, in turn implies, <div align="center"> <math> \frac{d\ln P}{d\ln\rho} = \gamma_\mathrm{g} \, , </math> </div> which we will enforce by adopting the barotropic (polytropic) equation of state, <div align="center"> <math>~P = K\rho^{\gamma_\mathrm{g}}</math> … with … <math>\gamma_\mathrm{g} \equiv \frac{d\ln P_0}{d\ln \rho_0} = \frac{\rho_0}{P_0} \biggl( \frac{dP}{d\rho} \biggr)_0 \, .</math> </div>
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