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Handbook of Turbomachinery Second Edition Revised - Ventech!

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This process began in the 1920s, although at least one major U.S. utility<br />

continued to use 50 Hz until the 1940s [5].<br />

By the year 2001, the design and manufacturing capabilities <strong>of</strong><br />

manufacturers have resulted in nuclear steam turbines <strong>of</strong> 1500 Mw in<br />

capacity at 1,500rpm (see Fig. 5).<br />

STEAM TURBINE THERMODYNAMIC CYCLES<br />

A basic understanding <strong>of</strong> the thermodynamics <strong>of</strong> the steam turbine is<br />

essential to understanding the how a steam turbine is designed, operated,<br />

and maintained. There is a controlled and continual drop <strong>of</strong> both pressure<br />

and temperature as the working steam expands through the turbine flow<br />

path. As the pressure is reduced, the steam specific volume and volumetric<br />

flow increase. The pressure, temperature, and moisture content <strong>of</strong> steam<br />

control the efficiency <strong>of</strong> the process and impose severe performance<br />

requirements on turbine components [6].<br />

Review <strong>of</strong> Thermodynamic Principles<br />

Historical Developments<br />

The importance <strong>of</strong> thermodynamics in the history <strong>of</strong> technology cannot be<br />

overstated. Bernal has said: ‘‘The central and most far-reaching discovery in<br />

the physical science <strong>of</strong> the nineteenth century was that <strong>of</strong> the conservation <strong>of</strong><br />

energy—the first law <strong>of</strong> thermodynamics’’ [7]. The second law <strong>of</strong><br />

thermodynamics was discovered by Sadi Carnot. In 1824, in Re´flexions<br />

sur la puissance motrice du feu et sur les machines propre a` developper cette<br />

puissance, Carnot outlined the second law as a theoretical limit on the<br />

efficiency <strong>of</strong> reversible cycles. Carnot also discovered the first law and a<br />

value for the mechanical equivalence <strong>of</strong> heat in 1830, but those were<br />

unpublished and lost in his notes until their rediscovery in 1878.<br />

Rudolf Clausius generalized Carnot’s work and by so doing began<br />

formal thermodynamics. Clausius pointed out in 1850 that ‘‘It is impossible<br />

to construct a device which, when operating in a cycle, will produce no effect<br />

other than the transference <strong>of</strong> heat from a colder to a hotter body.’’<br />

The final acceptance <strong>of</strong> the new views was due to the work <strong>of</strong> two<br />

academic scientists, William Thompson (Lord Kelvin), in his paper ‘On<br />

the Dynamical Equivalent <strong>of</strong> Heat’ and Herman Ludwig Ferdinand<br />

Helmholtz in his paper ‘On the Conservation <strong>of</strong> Force’, who fitted them<br />

into the accepted scheme <strong>of</strong> classical physics and almost succeeded in<br />

obscuring the fact that a great revolution in human thought had been<br />

achieved [11].<br />

Copyright © 2003 Marcel Dekker, Inc.

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