SMALL-SCALE RADIAL INFLOW TURBINE FOR WHR ORC

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SMALL-SCALE RADIAL INFLOW TURBINE FOR WHR ORC ( small-scale-radial-inflow-turbine-for-whr-orc )

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CHAPTER 3: Methodology for Developing Radial Inflow Turbine (RIT) Such improvements can be attributed to two main factors. Firstly, due to the shape of the rotor leading edge for the original case there was flow blockage at the rotor inlet and consequently a recirculation zone (shown by red arrow in Figure 3-30) that occupied a small portion of the inlet passage as depicted by the velocity streamlines in Figure 3-30(a). However, the modified leading edge shape reduced the flow blockage and almost entirely eliminated the formation of the flow reversal as illustrated by Figure 3-30(b). Furthermore, the reduction in the blade thickness increased the effective flow area compared to the original case (considering the growth of the boundary layer blockage on the blade surfaces and end walls for both cases) and therefore slightly larger mass flow rate was predicted by the CFD for the modified case (0.0884kg/s) compared to the original case (0.0863kg/s). However, even with larger mass flow rate the average value of the absolute flow velocity at rotor outlet for the modified case (56.86m/s) was slightly lower than the original case (57.4m/s) as shown in Figure 3-31. This is due to the fact that with the growth of boundary layer in the original case where the effective flow area was reduced, the flow was required to move with higher velocity in order to conserve mass and hence led to larger exit kinetic loss. The accumulative effects of these two factors resulted in better performance for the modified thickness and it was selected for further CFD investigations in the next section. 101 | P a g e

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