Microsoft Word - Cengel and Boles TOC _2-03-05_.doc

(ff) #1
Glossary
to accompany
Thermodynamics: An Engineering Approach, 5th edition
by Yunus A. Çengel and Michael A. Boles

7

mole fraction of the components as well as the mixture temperature and pressure, and is


independent of the identity of the other constituent gases.


Chemically correct amount of air is the stoichiometric or theoretical air, or 100 percent


theoretical air.


Choked flow occurs in a nozzle when the mass flow reaches a maximum value for the


minimum flow area. This happens when the flow properties are those required to


increase the fluid velocity to the velocity of sound at the minimum flow area location.


Choked Rayleigh flow occurs in a duct when a fluid can no longer be accelerated by


heating above sonic velocity to supersonic velocities.


Clapeyron equation, named after the French engineer and physicist E. Clapeyron


(1799–1864), relates the enthalpy change associated with a phase change (such as the


enthalpy of vaporization hfg) from knowledge of P, v, and T data alone.


Clapeyron–Clausius equation is used to determine the variation of saturation pressure


with temperature.


Classical thermodynamics is the macroscopic approach to the study of thermodynamics


that does not require knowledge of the behavior of individual particles.


Clausius inequality, first stated by the German physicist R. J. E. Clausius (1822–1888),


is expressed as the cyclic integral of δQ/T is always less than or equal to zero. This


inequality is valid for all cycles, reversible or irreversible.


Clausius statement of the second law is expressed as follows: It is impossible to


construct a device that operates in a cycle and produces no effect other than the transfer


of heat from a lower-temperature body to a higher-temperature body.


Clearance volume is the minimum volume formed in the cylinder when the piston is at


top dead center.


Closed feedwater heater is a feedwater heater in which heat is transferred from the


extracted steam to the feedwater without any mixing taking place. The two streams are


typically not at the same pressures, since they do not mix. In an ideal closed feedwater


heater the feedwater is heated to the exit temperature of the extracted steam, which


ideally leaves the heater as a saturated liquid at the extraction pressure. In actual power


plants the feedwater leaves the heater below the exit temperature of the extracted steam


because a temperature difference of at least a few degrees is required for any effective


heat transfer to take place.

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