The film cooling ejection on High Pressure (Hp) turbine component surface is strongly affected by the complex flow structure in the nozzle guide vane or rotor blade passages. The action of secondary flow in the main passage could dominate the film cooling effectiveness distribution on the component surfaces. The film cooling ejections from endwall and airfoil trailing edge are mixed by the secondary flow. Considering a small part of the coolant ejection from trailing edge discharge flow will move from the airfoil trailing edge pressure side to endwall downstream and then cover some area, the interaction between the coolants injected from endwall and airfoil trailing edge is worth investigating. Though the temperature of coolant discharge flow from trailing edge increases after the mixing process in the internal cooling procedure, the ejections moving from airfoil to endwall still have the potential of second order cooling. This part of the coolant is called “Phantom cooling flow” in the paper. A typical scale-up model of Hp turbine NGV is used in the experiment to investigate the cooling performance of ejection from trailing edge. Instead of the airfoil trailing edge platform itself, the film cooling effectiveness is measured on the downstream part of the endwall. This paper is focused on the trailing edge discharge flow with compound angle effects and the coolant from discharge holes moving from trailing edge to endwall surface. The coolant flow is injected from the straight discharge holes with a compound angle of 15deg and 45deg respectively. The film cooling holes on the endwall are used simultaneously to investigate the combined effects. The blowing ratio and different configurations of compound angle holes are selected to be the changing parameters in the paper. The experiment is completed with the blowing ratio changing from M = 0.7 to M = 1.3 and the compound angle is introduced to the entire row of trailing edge discharge holes (full span), with inlet Reynolds numbers of Re = 3.5×105 and an inlet Mach number of Ma = 0.1.

This content is only available via PDF.
You do not currently have access to this content.