We discuss a model consisting of two reservoirs, each with N possible ball locations, at heights Eh and El<Eh in a gravitational field. The two reservoirs contain nh and nl weight 1 balls. Empty locations are treated as weight 0 balls. The reservoirs are shaken so that all possible ball configurations are equally likely to occur. A cycle consists of exchanging a ball randomly chosen from the higher reservoir and a ball randomly chosen from the lower reservoir. We relate this system to a heat engine and show that the efficiency, which is defined as the ratio of the average work produced to the average energy lost by the higher reservoir, is 1El/Eh. When nl is comparable to nh, the efficiency is found to coincide with the maximum efficiency 1Tl/Th, where the temperatures Tl and Th are defined from a simple expression for the entropy. We also discuss the evaluation of fluctuations and the history of the Carnot discovery.

1.
P.
Ehrenfest
and
T.
Ehrenfest
, “
Ueber zwei bekannte Eingewände gegen das Boltzmannsche H-Theorem
,”
Z. Phys.
8
,
311
314
(
1907
).
2.
J.
Güémez
,
S.
Velasco
, and
A.
Calvo Hernández
, “
A generalization of the Ehrenfest urn model
,”
Am. J. Phys.
57
,
828
834
(
1989
).
3.
J.
Tobochnik
and
H.
Gould
, “
Teaching statistical physics by thinking about models and algorithms
,”
Am. J. Phys.
76
,
353
359
(
2008
).
4.
Classical heat engines may be considered as special cases of quantum heat engines.
5.
H. T.
Quan
, “
Quantum thermodynamic cycles and quantum heat engines (II)
,”
Phys. Rev. E
79
,
041129
1
(
2009
).
6.
M.
Zemansky
and
R.
Dittman
,
Heat and Thermodynamics
(
McGraw-Hill
,
New York
,
1997
).
7.
H. B.
Callen
,
Thermodynamics and an Introduction to Thermostatistics
(
Wiley
,
New York
,
1985
).
8.
J.
Arnaud
,
L.
Chusseau
, and
F.
Philippe
, “
Mechanical equivalent of quantum heat engines
,”
Phys. Rev. E
77
,
061102
1
(
2008
).
9.
If the balls could be distinguished from one another, the number of configurations would be N(N1)(Nn+1), but this number must be divided by n! to account for the fact that the exchange of balls is irrelevant.
10.
J.
Arnaud
,
L.
Chusseau
, and
F.
Philippe
, “
Carnot cycle for an oscillator
,”
Eur. J. Phys.
23
,
489
500
(
2002
).
11.
C.
Jarzynski
, “
Nonequilibrium equality for free energy differences
,”
Phys. Rev. Lett.
78
,
2690
2693
(
1997
).
12.
G. E.
Crooks
, “
Entropy production fluctuation theorem and the nonequilibrium work relation for free energy differences
,”
Phys. Rev. E
60
,
2721
2726
(
1999
).
13.
V. M.
Brodiansky
,
Sadi Carnot
(
Presses Universitaires de Perpignan
,
Perpignan
,
2006
), translated from Russian to French.
14.
A.
Kastler
,
Sadi Carnot et l’Essor de la Thermodynamique
(
Editions du CNRS
,
Paris
,
1976
), p.
195
.
15.
V. K.
La Mer
, “
Some current misinterpretations of N. L. Sadi Carnot’s memoir and cycle
,”
Am. J. Phys.
22
,
20
26
(
1954
).
16.
U.
Hoyer
, “
How did Carnot calculate the mechanical equivalent of heat?
,”
Centaurus
19
(
3
),
207
219
(
1975
).
17.
N. S.
Carnot
,
Réflexions sur la Puissance Motrice du Feu et sur Les Machines Propres à Développer cette Puissance
(
Bachelier
,
Paris
,
1824
);
translated to English by
R. B.
Thurston
from the original French of N.L.S. Carnot and accompanied by an account of Carnot's theory by Sir William Thomson (Lord Kelvin) in
Reflections on the Motive Power of Heat
(
John Wiley and Sons
,
New York
,
1897
).
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