Inverse curve: Difference between revisions
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A '''Photo-Carnot engine''' is a [[Carnot cycle]] engine in which the working medium is a photon inside a cavity with perfectly reflecting walls. [[Radiation]] is the working fluid, and the piston is driven by [[radiation pressure]]. | |||
A quantum Carnot engine is one in which the atoms in the heat bath are given a small bit of [[Coherence (physics)#Quantum coherence|quantum coherence]]. The phase of the atomic coherence provides a new control parameter.<ref>{{cite web | |||
|url=http://www.sciencemag.org/cgi/content/abstract/299/5608/862|title=Extracting Work from a Single Heat Bath via Vanishing Quantum Coherence -- Marlan Scully, M. Suhail Zubairy, G. S. Agarwal, and Herbert Walther, 299 (5608): 862 -- Science|publisher=www.sciencemag.org|accessdate=2008-06-18}}</ref> | |||
The deep physics behind the [[second law of thermodynamics]] is not violated; nevertheless, the quantum Carnot engine has certain features that are not possible in a classical engine. | |||
'''Derivation''' | |||
The internal energy of the photo-Carnot engine is proportional to the volume (unlike the ideal-gas equivalent) as well as the 4th power of the temperature (see [[Stefan-Boltzmann law]]). | |||
<math> U = \varepsilon\sigma T^{4}</math> | |||
The [[Radiation pressure]] is only proportional to this 4th power of temperature but no other variables, meaning that for this photo-Carnot engine an isotherm is equivalent to an isobar. | |||
<math> P = \frac{U}{3 V} = \frac{\varepsilon \sigma T^{4}}{3 V} </math> | |||
Using the First law of thermodynamics (<math> dU = dW + dQ </math>) we can determine the work done through an adiabatic (<math> dQ = 0 </math>) expansion by using the chain rule (<math> dU = \varepsilon \sigma dV T^{4} + 4 \varepsilon \sigma V T^{3} dT </math>) and setting it equal to <math> dW = -P dV = -\frac{1}{3} \varepsilon \sigma T^{4} dV </math> | |||
Combining these gives us <math> \frac{2}{3} T^{4} dV = 4 V T^{3} dT </math> which we can solve to find <math> \frac{V^{1/6}}{T} = const </math> | |||
.... | |||
The efficiency of this reversible engine must be the Carnot efficiency, regardless of the mechanism and so <math> \eta = \frac{T_H - T_C}{T_H} </math> | |||
==See also== | |||
*[[Carnot heat engine]] | |||
*[[Radiometer]] | |||
==Footnotes== | |||
{{reflist}} | |||
== Further reading == | |||
*{{cite journal|url=http://www.sciencemag.org/cgi/content/abstract/299/5608/862|title=Extracting Work from a Single Heat Bath via Vanishing Quantum Coherence|author=Marlan O. Scully, M. Suhail Zubairy, G. S. Agarwal, and Herbert Walther|journal=Science|date=2003-02-07|volume=299|issue=5608|pages=862–864|doi=10.1126/science.1078955|pmid=12511655|bibcode = 2003Sci...299..862S }} | |||
*{{cite conference|url=http://adsabs.harvard.edu/abs/2002AIPC..643...92Z|title=The Photo-Carnot Cycle: The Preparation Energy for Atomic Coherence|author=Zubairy, M. Suhail|booktitle=QUANTUM LIMITS TO THE SECOND LAW: First International Conference on Quantum Limits to the Second Law. AIP Conference Proceedings|volume=643|pages=92–97|year=2002|doi=10.1063/1.1523787}} | |||
{{Heat engines}} | |||
[[Category:Hot air engines]] | |||
{{physics-stub}} |
Revision as of 01:30, 7 December 2013
A Photo-Carnot engine is a Carnot cycle engine in which the working medium is a photon inside a cavity with perfectly reflecting walls. Radiation is the working fluid, and the piston is driven by radiation pressure.
A quantum Carnot engine is one in which the atoms in the heat bath are given a small bit of quantum coherence. The phase of the atomic coherence provides a new control parameter.[1]
The deep physics behind the second law of thermodynamics is not violated; nevertheless, the quantum Carnot engine has certain features that are not possible in a classical engine.
Derivation
The internal energy of the photo-Carnot engine is proportional to the volume (unlike the ideal-gas equivalent) as well as the 4th power of the temperature (see Stefan-Boltzmann law).
The Radiation pressure is only proportional to this 4th power of temperature but no other variables, meaning that for this photo-Carnot engine an isotherm is equivalent to an isobar.
Using the First law of thermodynamics () we can determine the work done through an adiabatic () expansion by using the chain rule () and setting it equal to
Combining these gives us which we can solve to find
....
The efficiency of this reversible engine must be the Carnot efficiency, regardless of the mechanism and so
See also
Footnotes
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Further reading
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