With the isentropic relationships given in Equation (40), the unknown variables might be solved iteratively with Equation (43) via Equation (50) in keeping with the move condition (subsonic forward, subsonic reverse, choked forward, and choked reverse). For each circulation situation, the velocity range, unknown variables, straight applied constraints, and iteration equation numbers are summarized in Desk 1. Observe that the throat velocity dictates the answer methodology however can also be an unknown parameter. The equations for a given move condition are repeatedly differentiable and will be solved utilizing a Newton-type solver. Nevertheless, when considering the answer as an entire, equations are usually not constantly differentiable at , , or . Because of this, every movement condition is evaluated separately.

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