Two bodies initially at different temperatures gathered into an isolated container exchange heat and reach an equilibrium state with a common final temperature. During the process, the system is out of equilibrium and its intermediate temperature is not well defined. By conceiving a quasi-static process with infinitesimal steps from the initial to the final state, a graphic representation of the intermediate temperatures is possible. We imagine an isolated container with the bodies in compartments separated by a wall, as shown in Fig. 1. If the conductivity of the wall is controlled, the heat exchange is made gradually through a sequence of very small portions of heat flowing from one body to the other. Each step is followed by a “dead time” in order to reach a momentary equilibrium state. These graphs are useful for students who need to analyze a phase change.

1.
See values and a conceptual discussion on the specific heats in
D.
Halliday
and
R.
Resnick
,
Fundamentals of Physics
, 3rd ed. extended (
Wiley
,
New York
,
1988
), Chap. 20.
2.
Other point graphics of quasi-static process have been used by
J.
Anacleto
and
J. M.
Ferreira
, “
On the representation of thermodynamic processes
,”
Eur. J. Phys.
36
,
035006
16
(
2015
).
3.
See the expression for the equilibrium temperature in
R. A.
Serway
and
J. W.
Jewett
,
Physics for Scientists and Engineers
, Vol.
1
, 6th ed. (
Brooks/Cole
,
Belmont, CA
,
2004
), Chap. 22.
4.
See values and a conceptual discussion on the latent heats in
F. W.
Sears
,
M. W.
Zemansky
,
H. D.
Young
, and
R. A.
Freedman
,
University Physics
, Vol.
1
, 9th ed. (
Addison-Wesley
,
Reading, MA
,
1996
), Chap. 17.
5.
R.
Rojas
, “
Graphical representation for thermal equilibrium when transition temperatures are present
,”
Phys. Educ.
51
,
013001
(
2016
).
6.
M. S.
Sabella
and
E. F.
Redish
, “
Knowledge organization and activation in physics problem solving
,”
Am. J. Phys.
75
,
1017
1029
(
Nov.
2007
).
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