5.3 Combined First and Second Law Expressions
The first law, written in a form that is always true:








Substituting for both and
in terms of state variables,

In terms of specific quantities:

The combined first and second law expressions are often more usefully written in terms of the enthalpy, or specific enthalpy, ,
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Or, since


In terms of enthalpy (rather than specific enthalpy) the relation is

Disusun Ulang Oleh:
Arip Nurahman
Pendidikan Fisika, FPMIPA. Universitas Pendidikan Indonesia
&
Follower Open Course Ware at MIT-Harvard University. Cambridge. USA.
Materi kuliah termodinamika ini disusun dari hasil perkuliahan di departemen fisika FPMIPA Universitas Pendidikan Indonesia dengan Dosen:
1. Bpk. Drs. Saeful Karim, M.Si.
2. Bpk. Insan Arif Hidayat, S.Pd., M.Si.
Dan dengan sumber bahan bacaan lebih lanjut dari :
Massachusetts Institute of Technology, Thermodynamics
Professor Z. S. Spakovszk, Ph.D.
Office: 31-265
Phone: 617-253-2196
Email: zolti@mit.edu
Aero-Astro Web: http://mit.edu/aeroastro/people/spakovszky
Gas Turbine Laboratory: home
Ucapan Terima Kasih:Kepada Para Dosen di MIT dan Dosen Fisika FPMIPA Universitas Pendidikan Indonesia
Semoga Bermanfaat
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