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Derivation of required cooling flows

A simple heat balance for a typical convectively cooled blade (as illustrated in Fig. A.la, which shows the notation) is [Pg.183]

It is assumed that the temperature of the coolant does not fully reach the temperature of the metal before it leaves the blade, i.e. Tp, 71,1. Thus, the concept of a cooling efficiency is introduced [Pg.183]

The exposed area for heat transfer (A g) is then replaced on the premise that, for a set of similar gas turbines, there is a reasonably constant ratio between A g and the cross-sectional area of the main hot gas flow A g. Thus, writing A g = AA g = XWg/pgVg in Eq. (A3) gives [Pg.183]

For a row in which the blade length is L, the blade chord is c, the spacing is s and the flow discharge angle is a, the ratio A is given approximately by [Pg.184]

With s/c = 0.8 and a = 75°, the value of A is then about 10. The total cooled surface area is found to be greater than the. surface area of the blade profiles alone because of the presence of cooled end-wall surfaces (adding another 30-40% of surface area), complex trailing edges and other cooled components. It would appear from an examination of practical engines that A(rpg/cp. ) could reasonably be given a value of about 20. Eq. (A4) then provides the basic form on which a cooling model can be based. [Pg.184]


See other pages where Derivation of required cooling flows is mentioned: [Pg.183]    [Pg.185]    [Pg.187]   
See also in sourсe #XX -- [ Pg.183 , Pg.184 , Pg.185 , Pg.186 ]




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Derived requirements

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