For time-dependent irrotational flow with , constant mass density, and no body force, the Euler equations for an inviscid fluid integrate to
A time-dependent change of gauge in may set .
An inviscid uniform tube plug driven by entrance excess pressure obeys and . From rest, the first zero of occurs after a quarter harmonic period, independent of its initial volume. The maximum speed is proportional to that initial volume. Entrance losses, a reservoir kinetic head or independently prescribed initial flow change this ideal model.

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  1. Euler equations for an inviscid fluid
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