Biomedical Engineering Reference
In-Depth Information
Since the conversionofAmust be between 0 (no conversion) and1 (100%conversion) inorder
for it to be physically possible, we discard the value that is greater than unit and obtain
f
A
¼ 20
3
20
3
p
p
1
1199
¼ 0:97194
(E5-4.14)
Next, we check if indeed this conversion gives the maximum gross profit. We can either
plot out the variation of GP$ vs
f
A
to see if we indeed having a maximum GP$ at this
f
A
value or checking the second derivative of GP$,
d
2
GP$
d
f
A
¼
2
$
A
F
B
f
A
2
$
V
F
B
kC
A
0
1 f
A
3
(E5-4.15)
Plug in the values we know up until this step, we obtain
d
2
GP$
d
f
A
¼
2 2ð
$
=
mol
Þ100ð
mol
=
h
Þ
0:97194
3
2 0:03½
$
=ð
lh
Þ 100ð
mol
=
h
Þ
3
0:15ðmin
1
Þ60ð
min
=
h
Þ2ð
mol
=
l
Þð1 0:97194Þ
Þ< 0
A negative second-order derivative means that the value of GP$ is lower for either higher
or lower
f
A
. Thus, we indeed have obtained a maximum value of the gross profit at the
conversion of
f
A
¼
¼15527ð
$
=
h
0.97194. This confirms that the optimum conversion is
f
A
¼
0.97194.
The reactor size can be computed from
Eqn (E5-4.4)
F
B
100
0:15 60 2 ð1 0:97194Þ
V ¼
kC
A
0
1 f
A
¼
¼ 197:99
l
l
3. The cash flow based on the optimum conversion:
$
B
F
B
F
A
0
F
B
f
A
F
A
0
F
B
GP$
F
A
0
¼
kC
A
0
1 f
A
F
A
0
$
A
$
V
$
V
f
A
¼
$
B
f
A
$
A
kC
A
0
1 f
A
0:03 0:97194
0:15 60 2 ð1 0:97194Þ
¼ 5 0:97194 2
$
=
mol
A
¼
$
2:802=
mol
A
4. At breaking even point, the net profit (or in this case the gross profit) is zero. Therefore,
at the break-even point, operating cost and the value of product are equal.
The value of product is,
$
B
F
B
¼ 5 100
$
=
h
¼ 500
$
=
h
which is also the operating cost at break-even.
Search WWH ::
Custom Search