MechMad1 (Mechanical) (OP) said:
Yeah, I agree. This data may be referenced for performance. The outlet pressure will be determined by the HRSG downstream the turbine (the losses in the HRSG).
But I still don't understand something. The total pressure in the exhaust is the sum of the static and the dynamic pressure. The flow of gases surely has a dynamic pressure (due to its velocity), so to calculate the total pressure in the exhaust we should know also the dynamic pressure.
Don't know if you've ever stood in the GT exhaust areas, but any (and all!) of the different definitions "could" apply - but at different locations in the "exhaust". Your answer IS going to be VERY, very different in each area.
Right after the last blade, still inside the circular exhaust shell - usually of Hastex in the machines I weld in: Very high velocity gas, very high temperature, constrained by the circular exhaust metal that is attached to the end of the GT.
After the circular exhaust section, outside of the directed gas flow. Still high temperature exhaust gas, but here it is circulating & swirling around. Now at high temperatures still, but static pressure. This is full of eddies and is very turbulent flow , so you'd expect vibrations and "shuddering" of the outside steel walls and their insulating liner. Outside the GT, this is tan expanding section of regular carbon steel (no longer Hastex/Hastalloy) and the cross-section is rectangular always expanding towards the rectangular HRSG (boiler) section downstream. The bigger the cross-sectional area in this transition section, the lower the velocity and the higher the static pressure. Nothing much to cool the gas though, sop it stays pretty high.
Through the Heat Recovery Steam Generator HRSG) if present. Usually a constant cross-section, but of relatively low speed compared to upstream values. The finned tubes slow the gasses down through friction losses, but cool it a great deal: Net? Cooler gas is more dense, and a slightly slower velocity. Higher static pressure again, but not much higher than in the transition section. (The transition area is filled many thousand cubic feet of "nothing" ... )
After the rectangular HRSG the gas flow horizontally to a vertical exhaust tube. This is a smaller area than the HRSG, so velocity increases substantially, and static pressure goes down. Flow "turns" from horizontal through the "nest" of finned HRSG tubes to a simple round tower exhaust into the air. This "turning" creates a constantly changing (vibrational) turbulence so the wall thicknesses are larger, or are reinforced with outside ribs and stiffeners on the tower section.