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Analysis of Missiles. P M V Subbarao Professor Mechanical Engineering Department. Simple Propulsion Systems but not for Humans!!!. (. ). æ. ö. g. -. 1. (. ). 2. +. b. 1. s. i. n. M. ç. ÷. x. è. ø. 2. =. M. n. (. ). y. æ. ö. g. -. 1. (. ). 2. g. b. -. s.
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Analysis of Missiles P M V Subbarao Professor Mechanical Engineering Department Simple Propulsion Systems but not for Humans!!!
( ) æ ö g - 1 ( ) 2 + b 1 s i n M ç ÷ x è ø 2 = M n ( ) y æ ö g - 1 ( ) 2 g b - s i n M ç ÷ x è ø 2 M n = y M ( ) y b - q s i n Hypersonic Flyers :Comprehensive Mechanism of Intake Air Control
Mx=5.0 max curve Mx=4.0 Oblique Shock Wave Angle Chart Mx=3.0 Mx=1.5 Mx=2.5 Mx=2.0
g 2 p ( ) = + - 2 y 1 1 M n ( ) x g + 1 p x ( ) ( ) é ù + g - 2 é ù 2 1 M g 2 n T ( ) x = + - 2 ê ú y 1 1 M ê ú n ( ) ( ) x g + g + 2 1 1 T M ê ú n ë û ë û x x Performance of An Adiabatic Oblique Shock But Pressure Recovery Factor or Total Pressure Ratio for the oblique shock :
Performance of An Adiabatic Oblique Shock Across a Shock Available Resource Pressure Recovery Factor or Total Pressure Ratio for the oblique shock :
Performances of NS & OS The total pressure recovery of a normal shock rapidly deteriorates beyond Mach ~ 1.6. 90% total pressure recovery is achieved at 1.6.
Simplest Reversible Inlet of A Missiles M>1 Oblique Shock Normal Shock A single compression ram inlet involves one oblique shock and one normal shock.
Inlet with Multiple External Compressions A double compression ram inlet involves two oblique shocks and one normal shock.
Special Designs of Center Bodies If there are multiple shocks: My3 q My2 My1 Mx q q
The Ancient Flyers : Ramjets (Asthras) Only three operating components: A central Body intake (diffuser) burner (combustion chamber); nozzle
Ramjets - Basic Operating Features • External shock decelerate ambient air entering the flyer. • This Air is further decelerated in intake (diffuser). • The pressure rises due to ram effect. • Known as ram pressure and significant at supersonic speeds. • A ramjet therefore needs no machines or engine to increase the pressure. • Simplifies the design and reducing the cost. • Greatest disadvantage is that it has to be accelerated up to very high speed before it produces any useful thrust. • Also complicated supersonic intake required to avoid shock losses.
Frictionless Flow through Constant area Pipe with Heat Transfer exit inlet Momentum equation gives Integrating from inlet to exit: