Available energy - Part I: Gibbs revisited

被引:20
作者
Gaggioli, RA [1 ]
Richardson, DH [1 ]
Bowman, AJ [1 ]
机构
[1] Marquette Univ, Dept Mech Engn, Milwaukee, WI 53201 USA
来源
JOURNAL OF ENERGY RESOURCES TECHNOLOGY-TRANSACTIONS OF THE ASME | 2002年 / 124卷 / 02期
关键词
D O I
10.1115/1.1448336
中图分类号
TE [石油、天然气工业]; TK [能源与动力工程];
学科分类号
0807 ; 0820 ;
摘要
The concept of available energy, as defined by Gibbs is revisited. Being more general, this concept of available energy differs from that referred to commonly by the some name, or as "exergy" or "availability." He gave representations of available energy for two circumstances. The first was the available energy of a "body," for the case when a body, alone is in a nonequilibrium condition and therefore has energy available. In turn, he presented the available energy of "the body and medium," for the energy that is available because a body is not in equilibrium with some arbitrarily specified medium or "reference environment." Gibbs' did not present formulas to represent available energy. His representations were verbal descriptions regarding surfaces, curves and lines. Although his verbiage age was augmented some graphics, visualization of the geometrical entities he described depended largely on the imagination of the reader. In Part I, we take advantage of modern graphics software to illustrate more vividly not only the available energy lie described verbally but also his interesting concepts of "available vacuum" and "capacity for entropy." We argue that all of these concepts are equivalent. Since Gibbs, representations with formulas have been developed and are common for the "available energy of body and medium." Gaggioli has developed formulas which are more general, to represent "the available energy of the body (alone)" and to assign an exergy to subsystems of the body as a measure of each subsystem contribution to the available energy. In contrast to the available energy, exergy is an additive property, so that balance equations can be written. This exergy is independent of any "reference environment, " which is important both theoretically and practically because of its relevance to proper selection of "the dead state." In those special cases when the dead state is one in equilibrium with a "reference environment," this more generalized exergy encompasses that concept called (today) exergy in textbooks and journals.
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页码:105 / 109
页数:5
相关论文
共 10 条
[1]  
[Anonymous], 1998, INT J THERMOPHYS
[2]  
Gaggioli R.A., 1999, P ECOS 99 JUN 8 10 T, P5
[3]  
GAGGIOLI RA, 1998, P INT SEM CONT PROBL
[4]  
GAGGIOLI RA, P ECOS98, V1, P185
[5]  
GAGGIOLI RA, 1995, P ECOS95, V1, P45
[6]  
Gibbs J.W., 1961, SCI PAPERS JW GIBBS, V1, P55
[7]  
GIBBS JW, 1961, COLLECTED WORKS J W, V1, P1
[8]  
GIBBS JW, 1961, COLLECTED WORKS J W, V1, P32
[9]  
GYFTOPOULOS EP, 1991, FUNDAMENTALS THERMOD
[10]  
Keenan J.H., 1941, Thermodynamics