With the isentropic relationships given in Equation (forty), the unknown variables may be solved iteratively with Equation (43) by Equation (50) in keeping with the circulation situation (subsonic ahead, subsonic reverse, choked ahead, and choked reverse). For every stream scenario, the velocity range, unknown variables, directly utilized constraints, and iteration equation numbers are summarized in Desk 1. Notice that the throat velocity dictates the solution technique however can be an unknown parameter. The equations for a given move condition are continuously differentiable and will be solved using a Newton-type solver. Nevertheless, when contemplating the solution as a complete, equations will not be constantly differentiable at , , or . As a result, each flow condition is evaluated individually.

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