Abstract
Euler equations, derived in 1755, are among the most important equations for general fluid analysis. Although this fundamental governing set of equations looks simple at first glance for incompressible, inviscid fluid flow, it does lead to a crucial numerical discretization dilemma related to existence, uniqueness, stability and oscillation problems. Take gradual pipe expansion flow, for instance: in the process of deriving Euler equations, the seemingly innocent artificial equalization of crosswise and forward-biased streamwise pressure will give serious discretization error compared with use of the Bernoulli equation. Here, the wall pressures,
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