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WORKING FLUID SELECTION AND DESIGN OF SMALL-SCALE WASTE HEAT RECOVERY SYSTEMS BASED ON ORGANIC RANKINE CYCLES

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WORKING FLUID SELECTION AND DESIGN OF SMALL-SCALE WASTE HEAT RECOVERY SYSTEMS BASED ON ORGANIC RANKINE CYCLES ( working-fluid-selection-and-design-small-scale-waste-heat-re )

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38 3 Numerical methods solved velocity vectors are the absolute velocity ⃗c, relative velocity w⃗ , and the peripheral velocity ⃗u. The sum of velocity vectors w⃗ and ⃗u forms the absolute velocity vector ⃗c ⃗c = w⃗ + ⃗u. (3.18) The tangential component of the absolute velocity c⃗ was used in monitoring the shape u of the velocity triangle at the rotor inlet by using a velocity ratio cu/u while the radial component of the absolute velocity c⃗ was used in the continuity equation. Examples of r velocity triangles at the rotor inlet are presented in Figure 3.4a and Figure 3.4b and at the (a) (b) Figure 3.4: Examples of velocity triangles at the turbine stator outlet (a) having a relative flow angle β1=0 and (b) having a relative flow angle β1 >0. outlet of the turbine rotor in Figure 3.5. The velocity triangle at the outlet was calculated at the mean line of the blade and at the blade hub and shroud in order to determine the blade setting angles at the rotor outlet. Figure 3.5: Example of a radial turbine rotor outlet velocity triangle. If the velocity triangle at the turbine rotor inlet is as presented in Figure 3.4a, straight blades at the rotor inlet can be used because the angle of the relative velocity is β1=0. If

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WORKING FLUID SELECTION AND DESIGN OF SMALL-SCALE WASTE HEAT RECOVERY SYSTEMS BASED ON ORGANIC RANKINE CYCLES

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