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The -229 has a lower bypass ratio and higher EPR than the -129 to get equivalent thrust with lower mass flow of 248 pps vs 275 pps. It run a little hotter than the -129, but nothing like 1000 degrees. They may measure turbine temp differently ( F100 measure at the low turbine inlet - FTIT), not sure about -129. But they both use the same engine temp gauge that reads somewhere in the 900 - 1000C range at Mil power.There's something that's bugged me for years. Based on the Dash-1s (F-16 I believe) the -229s exhaust is about a thousand degrees hotter, and much higher in velocity, than that of the -129. Yet (apparently) the -129 performs better at high velocity. Any idea why this might be the case?Correct - to supercruise, an engine must have a high exhaust velocity, at the supercruise engine inlet conditions. And a clean airframe with low supersonic drag. Both are required.For a given airframe, what is the difference between an engine that can supercruise and one that can't? Is it purely a difference of dry thrust? Or would the engines exhibit other differences as well.
To supercruise, an engine must have the lowest bypass ratio possible to keep the exhaust jet's velocity high; a turbojet is preferable to a turbofan. After all, a jet can fly only as fast as the velocity of its exhaust jet and the bypass air slows the exhaust jet's velocity down.
High exhaust velocity means a high nozzle pressure ratio going thru an optimized convergent / divergent exhaust nozzle. Nozzle pressure ratio is engine pressure ratio (exhaust pressure / engine inlet pressure) x ram pressure (engine inlet pressure / ambient pressure). Higher exhaust temperature also increases thrust, but it only goes up with the square root of the absolute temperature increase (same relationship as speed vs Mach number).
To get a high EPR at Mil power with a turbofan engine, you need a high pressure ratio Fan section, and a core module big and powerful enough to drive that high pressure Fan. The F100-220 fan pressure ratio is around 3:1, and the supercruise engines are significantly higher than that. At the typical quoted supercruise condition of 40K ft, 1.5Mn, the inlet temperature of the engine is approximately 100F. Most engines reach their rotor speed and turbine temperature limits in the 60-70F range. As the inlet gets hotter, these engines lose airflow, EPR, and thrust. At 100F inlet supercruise, both the Fan/LPT and Core have have the design margin to turn faster and hotter than at 60F inlet, just to keep making the same thrust (airflow and EPR). This points to having both a robust high pressure ratio fan, and probably an even larger core module. Thus, your design points to a low bypass turbofan - i.e. the F119.
more like a leaky turbojet, certainly not in the bypass range of a TF30 even, so not truly a turbofan but rather a very optimized turbojet for supercruise..
The F119 is a low bypass turbofan. Why turbofan instead of turbojet? A turbojet has a very hot outer skin in the main combustor, turbine, and AB areas, requiring heat shielding (weight) and a significant amount of secondary airflow (i.e. drag) to keep the airframe cool. The low bypass design of the F119 enables the structural fan ducts to be the heatshield, making it a "self cooled turbojet". The bypass air is also used extensively to cool the exhaust and nozzle components.
The other part of that thrust equation in the inlet ram recovery. At 40K, 1.5Mn the engine inlet pressure is around 10 psia, approximately 3.5 times the ambient pressure. Multiply that by the supercruise EPR, and you have a nozzle pressure ratio greater than 10:1. The convergent section of the nozzle accelerates the flow to Mach 1 using about 2:1 pressure ratio, leaving 5:1 or greater to be expanded in the divergent nozzle for supersonic flow. If you have a typical fixed ratio convergent / divergent nozzle, it will not have a large enough divergent section to efficiently utilize that available nozzle pressure ratio - i.e. under expanded flow. You could make the divergent section larger, but that adds weight, drag, and overexpansion concerns at lower speeds. The F119 engine, since it has full control of the 2D nozzle divergent flaps for thrust vectoring, can also position the divergent flap angles to optimize the supersonic expansion over a wide range of flight conditions and power settings.
The higher EPR and exhaust temp of the -229 should help with supercruise type performance, but apparently the higher mass flow gives the -129 an advantage in supersonic AB thrust. I don’t have enough information about the -129 to make any definitive analysis.