Zeroth Law of Thermodynamics<\/strong> states:<\/p>\n
If two systems are both in thermal equilibrium with a third, then they are in thermal equilibrium with each other.<\/div><\/div>\n
We can discover an important property of thermal equilibrium<\/strong><\/a> by considering three systems<\/strong>. A, B, and C are initially\u00a0not in thermal equilibrium<\/strong>. We separate systems A and B with an adiabatic wall (ideal insulating material), but we let system C interact with systems A and B. We wait until thermal equilibrium<\/strong> is reached; then, A and B are in thermal equilibrium with C. But are they in thermal equilibrium with each other?<\/p>\n
According to many experiments<\/strong>, there will be no net energy flow<\/strong> between A<\/strong> and B<\/strong>. This is experimental evidence<\/strong> of the following statement:<\/p>\n
If two systems are both in thermal equilibrium with a third, then they are in thermal equilibrium with each other. \u00a0<\/em><\/strong><\/p>\n
$\"Zeroth$ <\/a>
Zeroth law of thermodynamics: If two systems are both in thermal equilibrium with a third, then they are in thermal equilibrium with each other.<\/figcaption><\/figure>\n
This statement is known as the zeroth law of thermodynamics<\/strong>. It has this unusual name because it was not until scientists realized that this obvious postulate needed to be stated first after the great first and second laws of thermodynamics were worked out.<\/p>\n
$\"zeroth-law-of-thermodynamics-heat\"$ <\/a>This law provides a definition<\/strong> and method<\/strong> of defining temperatures<\/strong><\/a>, perhaps the most important intensive property<\/a><\/strong> of a system when dealing with thermal energy conversion problems. Temperature is a system property that determines whether the system will be in thermal equilibrium with other systems. When two systems are in thermal equilibrium, their temperatures are, by definition, equal, and no net thermal energy will be exchanged between them. Thus the importance of the zeroth law is that it allows a useful definition of temperature.<\/p>\n
\u00a0
<\/span>References:<\/div>
Reactor Physics and Thermal Hydraulics:<\/strong>\n\n
J. R. Lamarsh, Introduction to Nuclear Reactor Theory, 2nd ed., Addison-Wesley, Reading,\u00a0MA (1983).<\/li>\n
J. R. Lamarsh, A. J. Baratta, Introduction to Nuclear Engineering, 3d ed., Prentice-Hall, 2001, ISBN: 0-201-82498-1.<\/li>\n
W. M. Stacey, Nuclear Reactor Physics, John Wiley & Sons, 2001, ISBN: 0- 471-39127-1.<\/li>\n
Glasstone, Sesonske. Nuclear Reactor Engineering: Reactor Systems Engineering,\u00a0Springer; 4th edition, 1994, ISBN:\u00a0978-0412985317<\/li>\n
Todreas Neil E., Kazimi Mujid S. Nuclear Systems Volume I: Thermal Hydraulic Fundamentals, Second Edition. CRC\u00a0Press; 2\u00a0edition, 2012, ISBN:\u00a0978-0415802871<\/li>\n
Zohuri B., McDaniel P. Thermodynamics in Nuclear Power Plant Systems. Springer; 2015, ISBN:\u00a0978-3-319-13419-2<\/li>\n
Moran Michal J., Shapiro Howard N. Fundamentals of Engineering Thermodynamics, Fifth Edition,\u00a0John Wiley & Sons, 2006, ISBN:\u00a0978-0-470-03037-0<\/li>\n
Kleinstreuer C. Modern Fluid Dynamics. Springer, 2010,\u00a0ISBN 978-1-4020-8670-0.<\/li>\n
U.S. Department of Energy, THERMODYNAMICS, HEAT TRANSFER, AND FLUID FLOW. DOE Fundamentals Handbook, Volume 1, 2, and 3. June 1992.<\/li>\n<\/ol>\n<\/div><\/div><\/div>
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See above:<\/h2>\n
Temperature<\/i> <\/span><\/a><\/p><\/div><\/div>
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