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The flow parameter commonly used for compressors is based on the following dimensionless<br />

grouping from dimensional analysis<br />

Rm # 1kRT 01<br />

D 2 p 01<br />

where R is the gas constant, m # the mass flowrate, k the specific heat ratio, T 01 the stagnation temperature<br />

at the compressor inlet, D a characteristic length, and p 01 the stagnation pressure at the<br />

compressor inlet.<br />

To account for variations in test conditions, the following strategy is employed. We set<br />

where the subscript “test” refers to a specific test condition and “std” refers to the standard atmosphere<br />

1 p 0 14.7 psia, T 0 518.7 °R2 condition. When we consider a given compressor operating<br />

on a given working <strong>fluid</strong> 1so that R, k, and D are constant2, the above equation reduces to<br />

m # std m# test1T 01 testT 0 std<br />

(12.54)<br />

p 01 testp 0 std<br />

In essence, m # std is the compressor-test mass flowrate “corrected” to the standard atmosphere inlet<br />

condition. The corrected compressor mass flowrate, is used instead of flow coefficient. Often,<br />

m # m # std,<br />

std is divided by A, the frontal area of the compressor flow path.<br />

While for pumps, blowers, and fans, rotor speed was accounted for in the flow coefficient,<br />

it is not in the corrected mass flowrate derived above. Thus, for compressors, rotor speed<br />

needs to be accounted for with an additional group. This dimensionless group is<br />

For the same compressor operating on the same gas, we eliminate D, k and R and, as with corrected<br />

mass flowrate, obtain a corrected speed, N std , where<br />

N std <br />

12.9 Compressible Flow Turbomachines 689<br />

a Rm# 1kRT 01<br />

a Rm# 1kRT 01<br />

D 2 p 01<br />

btest D 2 p 01<br />

bstd<br />

ND<br />

1kRT 01<br />

N<br />

1T 01T std<br />

(12.55)<br />

Often, the percentage of the corrected speed design value is used.<br />

An example of how compressor performance data are typically summarized is shown in<br />

Fig. 12.37.<br />

A gas turbine engine<br />

generally consists<br />

of a compressor,<br />

a combustor,<br />

and a turbine.<br />

12.9.2 Compressible Flow Turbines<br />

Turbines that use a gas or vapor as the working <strong>fluid</strong> are in many respects similar to hydraulic<br />

turbines 1see Section 12.82. Compressible flow turbines may be impulse or reaction turbines, and<br />

mixed-, radial-, or axial-flow turbines. The fact that the gas may expand 1compressible flow2 in<br />

coursing through the turbine can introduce some important phenomena that do not occur in hydraulic<br />

turbines. 1Note: It is tempting to label turbines that use a gas as the working <strong>fluid</strong> as gas<br />

turbines. However, the terminology “gas turbine” is commonly used to denote a gas turbine engine,<br />

as employed, for example, for aircraft propulsion or stationary power generation. As shown<br />

in Fig. 12.36, these engines typically contain a compressor, combustion chamber, and turbine.2<br />

Although for compressible flow turbines the axial-flow type is common, the radial-inflow type<br />

is also used for various purposes. As shown in Fig. 12.33, the turbine that drives the typical automobile<br />

turbocharger compressor is a radial-inflow type. The main advantages of the radial-inflow<br />

turbine are: 112 It is robust and durable, 122 it is axially compact, and 132 it can be relatively inexpensive.<br />

A radial-flow turbine usually has a lower efficiency than an axial-flow turbine, but lower initial<br />

costs may be the compelling incentive in choosing a radial-flow turbine over an axial-flow one.<br />

Axial-flow turbines are widely used compressible flow turbines. Steam engines used in electrical<br />

generating plants and marine propulsion and the turbines used in gas turbine engines are

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