With the isentropic relationships given in Equation (40), the unknown variables can be solved iteratively with Equation (forty three) by way of Equation (50) in line with the move condition (subsonic ahead, subsonic reverse, choked forward, and choked reverse). For every stream scenario, the velocity vary, unknown variables, straight utilized constraints, and iteration equation numbers are summarized in Desk 1. Notice that the throat velocity dictates the solution method however can also be an unknown parameter. The equations for a given circulate condition are repeatedly differentiable and could be solved using a Newton-kind solver. Nonetheless, when contemplating the solution as an entire, equations will not be constantly differentiable at , , or . Consequently, each move situation is evaluated separately.

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