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The above holds true only for non-viscous fluids.
For example, for a non-viscous fluid, the mechanical work done on the system may be related to the pressure p and volume V.
The gas flow is isentropic i.e., at constant entropy, as the result of the assumption of non-viscous fluid, and adiabatic process.
G0340 Geostrophic equilibrium Condition of the field of motion of a non-viscous fluid in which the pressure gradient force is exactly balanced by the Coriolis force.
For turbulent, non-viscous fluids the Dittus-Boelter Equation can be used to determine the heat transfer coefficient for both the inner and outer streams; given their diameters and velocities (or flow rates).