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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

FIG. 3.10. Apparent flow angle variation measured by three different combination<br />

probes traversed across a transverse variation <strong>of</strong> total pressure (adapted from Bryer<br />

<strong>and</strong> Pankhurst 1971).<br />

probe instruments are subject to this type <strong>of</strong> directional error when traversed across a<br />

total pressure variation such as a blade wake.<br />

An extensive bibliography on all types <strong>of</strong> measurement in fluid flow is given by<br />

Dowden (1972). Figure 3.11 shows a typical cascade test result from a traverse across<br />

two blade pitches taken by Todd (1947) at an inlet Mach number <strong>of</strong> 0.6. It is observed<br />

that a total pressure deficit occurs across the blade row arising from the fluid friction<br />

on the blades. The fluid deflection is not uniform <strong>and</strong> is a maximum at each blade trailing<br />

edge on the pressure side <strong>of</strong> the blades. From such test results, average values <strong>of</strong><br />

total pressure loss <strong>and</strong> fluid outlet angle are found (usually on a mass flow basis). The<br />

use <strong>of</strong> terms like total pressure loss <strong>and</strong> fluid outlet angle in the subsequent discussion<br />

will signify these average values.<br />

Similar tests performed for a range <strong>of</strong> fluid inlet angles, at the same inlet Mach<br />

number M1 <strong>and</strong> Reynolds number Re, enables the complete performance <strong>of</strong> the cascade<br />

to be determined (at that M1 <strong>and</strong> Re). So as to minimise the amount <strong>of</strong> testing required,<br />

much cascade work is performed at low inlet velocities, but at a Reynolds number<br />

greater than the “critical” value. This critical Reynolds number Rec is approximately 2<br />

¥ 10 5 based on inlet velocity <strong>and</strong> blade chord. With Re > Rec, total pressure losses <strong>and</strong><br />

fluid deflections are only slightly dependent on changes in Re. Mach number effects<br />

are negligible when M 1 < 0.3. Thus, the performance laws, eqn. (3.28), for this flow<br />

simplify to<br />

(3.28a)

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