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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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256 <strong>Fluid</strong> <strong>Mechanics</strong>, <strong>Thermodynamics</strong> <strong>of</strong> <strong>Turbomachinery</strong><br />

It is worth commenting that higher total-to-static efficiencies have been obtained<br />

in other small radial turbines operating at higher pressure ratios. Rodgers (1969) has<br />

suggested that total-to-static efficiencies in excess <strong>of</strong> 90% for pressure ratios up to<br />

five to one can be attained. Nusbaum <strong>and</strong> K<strong>of</strong>skey (1969) reported an experimental<br />

value <strong>of</strong> 88.8% for a small radial turbine (fitted with an outlet diffuser, admittedly!)<br />

at a pressure ratio p01/p4 <strong>of</strong> 1.763. In the design point exercise given above the high<br />

rotor enthalpy loss coefficient <strong>and</strong> the corresponding relatively low total-to-static efficiency<br />

may well be related to the low relative velocity ratio determined on the hub.<br />

Matters are probably worse than this as the calculation is based only on a simple onedimensional<br />

treatment. In determining velocity ratios across the rotor, account should<br />

also be taken <strong>of</strong> the effect <strong>of</strong> blade to blade velocity variation (outlined in this chapter)<br />

as well as viscous effects. The number <strong>of</strong> vanes in the rotor (ten) may be insufficient<br />

on the basis <strong>of</strong> Jamieson’s theory* (1955) which suggests 18 vanes (i.e. Zmin = 2ptan<br />

a2). For this turbine, at lower nozzle exit angles, eqn. (8.13) suggests that the relative<br />

velocity ratio becomes even less favourable despite the fact that the Jamieson blade<br />

spacing criterion is being approached. (For Z = 10, the optimum value <strong>of</strong> a2 is about<br />

58deg.)<br />

Mach number relations<br />

Assuming the fluid is a perfect gas, expressions can be deduced for the important<br />

Mach numbers in the turbine. At nozzle outlet the absolute Mach number at the nominal<br />

design point is<br />

1<br />

Now, T = T - c ( 2C<br />

)= T - U cosec C .<br />

2 a<br />

2 01 2 2<br />

where a2 = a 01(T 2/T 01) 1/2 . Hence,<br />

p 01 2 2 p<br />

2<br />

2<br />

At rotor outlet the relative Mach number at the design point is defined by<br />

*Included in a later part <strong>of</strong> this chapter.<br />

(8.14)

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