For non-isentropic constant-area flow with stagnation temperature change the following relation was determined: To_2(y + 1)M² (1 + ² = ¹ M²) - 2 = (1+yM²)² To It is possible to use the above equation and calculate the downstream Mach number without resorting to iteration for a flow where the upstream Mach number, as well as the upstream and downstream stagnation temperatures, are known. This is a common calculation for flows through engine combustors. Presuming the left side is a known quantity, show that the above equation can be directly solved as a quadratic in M² and which roots correspond to the subsonic/supersonic solution. Rewrite the equation as: aMª + bM² + c = 0, and then M² = (−b ± √b² − 4ac)/2a. Determine the appropriate expressions for a, b, and c.

For non-isentropic constant-area flow with stagnation temperature change the following relation was determined: To_2(y + 1)M² (1 + ² = ¹ M²) - 2 = (1+yM²)² To It is possible to use the above equation and calculate the downstream Mach number without resorting to iteration for a flow where the upstream Mach number, as well as the upstream and downstream stagnation temperatures, are known. This is a common calculation for flows through engine combustors. Presuming the left side is a known quantity, show that the above equation can be directly solved as a quadratic in M² and which roots correspond to the subsonic/supersonic solution. Rewrite the equation as: aMª + bM² + c = 0, and then M² = (−b ± √b² − 4ac)/2a. Determine the appropriate expressions for a, b, and c.

Elements Of Electromagnetics

7th Edition

ISBN:9780190698614

Author:Sadiku, Matthew N. O.

Publisher:Sadiku, Matthew N. O.

ChapterMA: Math Assessment

Section: Chapter Questions

Problem 1.1MA

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