Biomedical Engineering Reference
In-Depth Information
U j , other than in an electro-hydro facility, or for simple flow loop calcu-
lations. Thus, Eqn (3.123) can be simplified to
In most cases, E j z
X
N S
X
N S
d
ð
nU
Þ
¼ Q
W s þ
F j0
H j0
F j H j
(3.127)
d t
j
¼1
j
¼1
The energy balance equation for open system is reduced to that for closed system if there is
no flow in or out of the system, i.e. F
0. When chemical reaction occurs, internal energy
changes and so are the enthalpies according to the species change.
Since
¼
X
N S
nU
¼
nH
pV
¼
H j n j
pV
(3.128)
j
¼1
and enthalpy is only a function of temperature for ideal gases and nearly so for condensed
matters (i.e. liquids or solids),
d H j
d t ¼
d T
d t
C P j
(3.129)
where C Pj is the molar heat capacity of species j. Differentiating both sides of Eqn (3.108) and
substituting Eqn (3.129) as needed, we obtain
X
N S
X
N S
d n j
d t
d
ð
nU
Þ
d T
d t þ
d
ð
pV
Þ
¼
C P j n j
H j
(3.130)
d t
d t
j
¼1
j
¼1
which expresses how the left hand side of Eqn (3.126) can be evaluated. Next, we apply the
general mole balance equation,
X
N R
d n j
d t
F j0
F j þ
n ji r i V
¼
(3.131)
i
¼1
Equation (3.127) can be rearranged to give
V X
N R
d n j
d t H j
F j H j ¼
F j0
H j þ
n ji r i H j
(3.132)
i
¼1
Thus,
P
N S
H j0 P
N S
F j H j ¼ P
N S
H j0 P
N S
V P
N R
r i P
N S
n ji H j þ P
N S
d n j
d t H j
F j0
F j0
F j0
H j
j
¼1
j
¼1
j
¼1
j
¼1
i
¼1
j
¼1
j
¼1
(3.133)
H j0
H j
¼ P
N S
V P
N R
r i DH Ri þ P
N S
d n j
d t H j
F j0
j
¼1
i
¼1
j
¼1
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