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(a) x (a) Ideal case: instantaneous valve opening x x (b) Real case: non-instantaneous valve open- 4 3.5 3 2.5 2 0.97 4.02 4 3.98 3.96 1.02 0.97 (b) PIT1 PIT2 PIT3 PIT4 PIT3 PIT4 0.98 0.99 PIT1 PIT2 1 1.01 0.975 0.98 t [s] 0.985 0.99 t [s] x ing Figure 7.8: Position-time diagrams of classical expansion fans. In the ideal case with an instan- taneous valve opening and in absence of a nozzle, all characteristics emerge from a single point. In the realistic case, the last characteristic starts at a later time instance than the first one, due to the finite opening time. All characteristics are curved upwards in the nozzle area except the first one, because of the higher flow velocity in the nozzle, which slows down the wave propagation speed. Figure 7.9: Portions of the signals from an expansion in nitrogen mapped to the valve position, with two levels of magnification. Commissioning of the FAST setup P [bar] P [bar] 191PDF Image | New Concepts FOR Organic Rankine Cycle Power Systems
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