60 | Thermodynamics
CLOSED
SYSTEM
(m = constant)WorkHeatSystem boundaryFIGURE 2–11
Energy can cross the boundaries of a
closed system in the form of heat and
work.
Room air
25 °C
No heat
transferHeat Heat25 °C5°C8 J/s 16 J/s15 °CFIGURE 2–12
Temperature difference is the driving
force for heat transfer. The larger the
temperature difference, the higher is
the rate of heat transfer.
2–3 ■ ENERGY TRANSFER BY HEAT
Energy can cross the boundary of a closed system in two distinct forms:
heatand work(Fig. 2–11). It is important to distinguish between these two
forms of energy. Therefore, they will be discussed first, to form a sound
basis for the development of the laws of thermodynamics.
We know from experience that a can of cold soda left on a table eventu-
ally warms up and that a hot baked potato on the same table cools down.
When a body is left in a medium that is at a different temperature, energy
transfer takes place between the body and the surrounding medium until
thermal equilibrium is established, that is, the body and the medium reach
the same temperature. The direction of energy transfer is always from the
higher temperature body to the lower temperature one. Once the tempera-
ture equality is established, energy transfer stops. In the processes described
above, energy is said to be transferred in the form of heat.
Heatis defined as the form of energy that is transferred between two
systems (or a system and its surroundings) by virtue of a temperature
difference(Fig. 2–12). That is, an energy interaction is heat only if it
takes place because of a temperature difference. Then it follows that there
cannot be any heat transfer between two systems that are at the same
temperature.
Several phrases in common use today—such as heat flow, heat addition,
heat rejection, heat absorption, heat removal, heat gain, heat loss, heat
storage, heat generation, electrical heating, resistance heating, frictional
heating, gas heating, heat of reaction, liberation of heat, specific heat, sensi-
ble heat, latent heat, waste heat, body heat, process heat, heat sink, and heat
source—are not consistent with the strict thermodynamic meaning of the
term heat, which limits its use to the transferof thermal energy during a
process. However, these phrases are deeply rooted in our vocabulary, and
they are used by both ordinary people and scientists without causing any
misunderstanding since they are usually interpreted properly instead of
being taken literally. (Besides, no acceptable alternatives exist for some of
these phrases.) For example, the phrase body heatis understood to mean
the thermal energy contentof a body. Likewise,heat flowis understood
to mean the transfer of thermal energy,not the flow of a fluidlike substance
called heat, although the latter incorrect interpretation, which is based on
the caloric theory, is the origin of this phrase. Also, the transfer of heat
into a system is frequently referred to as heat additionand the transfer of
heat out of a system as heat rejection. Perhaps there are thermodynamic rea-
sons for being so reluctant to replace heatby thermal energy: It takes less
time and energy to say, write, and comprehend heatthan it does thermal
energy.
Heat is energy in transition. It is recognized only as it crosses the bound-
ary of a system. Consider the hot baked potato one more time. The potato
contains energy, but this energy is heat transfer only as it passes through
the skin of the potato (the system boundary) to reach the air, as shown in
Fig. 2–13. Once in the surroundings, the transferred heat becomes part of
the internal energy of the surroundings. Thus, in thermodynamics, the term
heatsimply means heat transfer.SEE TUTORIAL CH. 2, SEC. 3 ON THE DVD.INTERACTIVE
TUTORIAL