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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

x/l. Some examples <strong>of</strong> these tables are quoted by Horlock (1958, 1966). Summarising,<br />

the useful parameters for describing a cascade blade are camber line shape, b/l, a/l, type<br />

<strong>of</strong> thickness distribution <strong>and</strong> maximum thickness to chord ratio, tmax/l.<br />

Two important geometric variables, which define the cascade shown in Fig. 3.2, are<br />

the space–chord ratio, s/l, <strong>and</strong> the stagger angle, x, the angle between the chord line<br />

<strong>and</strong> the reference direction which is a line perpendicular to the cascade front.<br />

Throughout the remainder <strong>of</strong> this book unless stated to the contrary, all fluid <strong>and</strong> blade<br />

angles are referred to this reference direction so as to avoid the needless complication<br />

arising from other directional references. However, custom dies hard; in steam turbine<br />

practice, blade <strong>and</strong> flow angles are conventionally measured from the tangential direction<br />

(i.e. parallel to the cascade front). Despite this, it is better to avoid ambiguity <strong>of</strong><br />

meaning by adopting the single reference direction already given.<br />

The blades angles at entry to <strong>and</strong> at exit from the cascade are denoted by a¢1 <strong>and</strong> a¢2<br />

respectively. A most useful blade parameter is the camber angle q which is the change<br />

in angle <strong>of</strong> the camber line between the leading <strong>and</strong> trailing edges <strong>and</strong> equals a¢1–a¢2<br />

in the notation <strong>of</strong> Figure 3.2. For circular arc camber lines the stagger angle is<br />

x = 1 – 2 (a¢1 + a¢2).<br />

Analysis <strong>of</strong> cascade forces<br />

The fluid approaches the cascade from far upstream with velocity c1 at an angle a1<br />

<strong>and</strong> leaves far downstream <strong>of</strong> the cascade with velocity c 2 at an angle a 2. In the<br />

b<br />

<br />

t<br />

a<br />

a¢ 2<br />

x<br />

c 2<br />

d<br />

y<br />

q<br />

a¢ 2<br />

a 2<br />

FIG. 3.2. Compressor cascade <strong>and</strong> blade notation.<br />

x<br />

s<br />

a¢<br />

1<br />

<br />

a¢ 1<br />

a 1<br />

c 1 = inlet flow velocity vector<br />

c 2 = outlet flow velocity vector<br />

(averaged across the pitch)<br />

i<br />

c 1

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