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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