4–3 SPECIFIC HEATS
We know from experience that it takes different amounts of energy to raise
the temperature of identical masses of different substances by one degree.
For example, we need about 4.5 kJ of energy to raise the temperature of 1 kg
of iron from 20 to 30°C, whereas it takes about 9 times this energy (41.8 kJ
to be exact) to raise the temperature of 1 kg of liquid water by the same
amount (Fig. 4 –17). Therefore, it is desirable to have a property that will
enable us to compare the energy storage capabilities of various substances.
This property is the specific heat.
The specific heatis defined as the energy required to raise the temperature
of a unit mass of a substance by one degree(Fig. 4 –18). In general, this
energy depends on how the process is executed. In thermodynamics, we are
interested in two kinds of specific heats:specific heat at constant volumecv
andspecific heat at constant pressurecp.
Physically, the specific heat at constant volume cvcan be viewed as the
energy required to raise the temperature of the unit mass of a substance
by one degree as the volume is maintained constant. The energy required to
178 | Thermodynamics
(c) Under stated assumptions and observations, the energy balance on the
system can be expressed as
Net energy transfer Change in internal, kinetic,
by heat, work, and mass potential, etc., energies
Notice that even though the water is expanding during this process, the sys-
tem chosen involves fixed boundaries only (the dashed lines) and therefore
the moving boundary work is zero (Fig. 4–16). Then W0 since the system
does not involve any other forms of work. (Can you reach the same conclu-
sion by choosing the water as our system?) Initially,
The quality at the final state is determined from the specific volume
information:
Then
Substituting yields
Discussion The positive sign indicates that the assumed direction is correct,
and heat is transferred to the water.
Qin 1 5 kg 231 104.88104.83 2 kJkg 4 0.25 kJ
104.88 kJ>kg
104.83 kJ>kg 1 2.3 10 ^521 2304.3 kJ>kg 2
u 2 ufx 2 ufg
x 2
v 2 vf
vfg
0.0020.001
43.340.001
2.3 10 ^5
u 1 uf @ 25°C104.83 kJ>kg
Qin¢Um 1 u 2 u 12
EinEout¬
¬
¢Esystem
Vacuum
P = 0
W = 0
H 2 O Heat
FIGURE 4 –16
Expansion against a vacuum involves
no work and thus no energy transfer.
20 30°C
IRON
1 kg
←
4.5 kJ
20 30°C
WATER
1 kg
←
41.8 kJ
FIGURE 4 –17
It takes different amounts of energy to
raise the temperature of different
substances by the same amount.
Specific heat = 5 kJ/kg ·°C
∆T = 1°C
m = 1 kg
5 kJ
FIGURE 4 –18
Specific heat is the energy required to
raise the temperature of a unit mass of
a substance by one degree in a
specified way.
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SEE TUTORIAL CH. 4, SEC. 3 ON THE DVD.
INTERACTIVE
TUTORIAL