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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

(ii) At nozzle exit the Mach number is<br />

<strong>and</strong> it is necessary to solve the velocity diagram to find c2 <strong>and</strong> hence to determine T2.<br />

As<br />

Referring to Figure 4.2, across the nozzle h01 = h02 = h2 + 1 – 2 c2 2 , thus<br />

Hence, M2 = 0.97 with g R = (g - 1)Cp.<br />

(iii) The axial velocity, cx = c 2 cos a 2 = 200m/s.<br />

(iv) htt =DW/(h01 + h3ss - 1 – 2 c3 2 ).<br />

After some rearrangement,<br />

Therefore htt = 0.93.<br />

(v) Using eqn. (4.22a), the reaction is<br />

From the velocity diagram, tan b3 = U/cx <strong>and</strong> tan b2 = tana2 - U/cx<br />

EXAMPLE 4.3. Verify the assumed value <strong>of</strong> total-to-static efficiency in the above<br />

example using Soderberg’s correlation method. The average blade aspect ratio for the<br />

stage H/b = 5.0, the maximum blade thickness–chord ratio is 0.2 <strong>and</strong> the average<br />

Reynolds number, defined by eqn. (4.14), is 10 5 .<br />

Solution. The approximation for total-to-static efficiency, eqn. (4.10a), is used <strong>and</strong><br />

can be rewritten as<br />

The loss coefficients zR <strong>and</strong> zN, uncorrected for the effects <strong>of</strong> blade aspect ratio, are<br />

determined using eqn. (4.12) which requires a knowledge <strong>of</strong> flow turning angle for<br />

each blade row.<br />

For the nozzles, a1 = 0 <strong>and</strong> a2 = 70deg, thus N = 70deg.

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