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assignment 1

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GREEN AMONIA PROCESS
OPTIMISATION
CHE4173 – SUSTAINABLE
ENGINEERING
NGOC GIA HAN NGUYEN
ATIQAH NOOR HISHAM
01/04/2022
1
Question 1 – Stream Table
The heat capacity (CP) can be calculated by:
π»π‘’π‘Žπ‘‘ 𝑑𝑒𝑑𝑦
𝑄
𝑄
𝐢𝑃 =
=
=
πΆβ„Žπ‘Žπ‘›π‘”π‘’ π‘œπ‘“ π‘‡π‘’π‘šπ‘π‘’π‘Ÿπ‘Žπ‘‘π‘’π‘Ÿπ‘’
βˆ†π‘‡
π‘‡π‘œπ‘’π‘‘ − 𝑇𝑖𝑛
The min temperature difference is βˆ†π‘‡π‘šπ‘–π‘› = 20℃ so the
βˆ†π‘‡π‘šπ‘–π‘›
2
= 10℃
The shifting rule is:
For hot stream, the shifted temperature would be 𝑇 ∗ = π‘‡β„Žπ‘œπ‘‘ π‘ π‘‘π‘Ÿπ‘’π‘Žπ‘š −
βˆ†π‘‡π‘šπ‘–π‘›
For cold stream, the shifted temperature would be 𝑇 ∗ = π‘‡π‘π‘œπ‘™π‘‘ π‘ π‘‘π‘Ÿπ‘’π‘Žπ‘š +
2
βˆ†π‘‡π‘šπ‘–π‘›
2
Based on above calculation, the stream table is shown in Table 1.
Table 1 shows the stream table in the base case scenario (dry recycle, no heating) with βˆ†π‘‡π‘šπ‘–π‘› = 20℃
Stream Type
No.
Mass
P
Tin
Flowrate (bara) (oC)
(kg/hr)
1a
Cold 8858.1
40
25
1b
Cold 8858.1
40
250.3
1c
Cold 8858.1
40
251.3
2
Cold 2118.7
40
222.9
3
Cold 9545.7
40
379.9
4
Hot
8925.4
39.3
800
5
Hot
8925.4
39
195
6
Hot
2739.1
39.3
800
7
Hot
687.6
40
35
* T* was denoted as shifted temperature
Tout
(oC)
Q (kW)
CP
(kW/oC)
T*in
(oC)
T*out
(oC)
250.3
251.3
420
550
610
195
35
35
35
2453.15
4215.79
1133.54
207.20
1409.70
3854.80
5176.30
602.30
0
10.89
4215.79
6.72
0.63
6.13
6.37
32.35
0.79
0
35
260.3
261.3
232.9
389.9
790
185
790
25
260.3
261.3
430
560
620
185
25
25
25
Question 2
To be able to find the hot and cold utility targets, and process pinch temperature, the
problem table algorithms was carried out, as shown in Table 2:
2
Table 2 shows the problem table cascade in the base case scenario (dry recycle, no heating) with βˆ†π‘‡π‘šπ‘–π‘› = 20℃
Stream 1a
Ti (oC)
790
620
560
430
389.9
261.3
260.3
1b
1c
6.72
6.72
4215.7
9
232.9
10.89
185
10.89
35
10.89
25
*(i) was denoted as interval
2
0.63
0.63
0.63
0.63
0.63
3
6.13
6.13
6.13
6
CPc CPh
Ti
(oC)
Hi
(kW)
6.37
6.37
6.37
6.37
6.37
6.37
0.79
0.79
0.79
0.79
0.79
0.79
170.00
60.00
130.00
40.10
128.60
1.00
6.37
6.37
0.79
0.79
0.79
0.79
-7.16
-1.03
-0.40
6.32
0.19
4209.2
7
4.36
3.73
-22.25
-33.14
27.40
47.90
150.00
10.00
4
5
32.35
32.35
-1217.01
-61.95
-51.87
253.44
24.93
4209.27
Total
H (kW)
0.00
1217.01
1278.96
1330.82
1077.38
1052.45
-3156.81
Hadjust
(kW)
3455.00
4672.01
4733.96
4785.82
4532.38
4507.45
298.19
119.54
178.64
-3337.62
-331.39
-3276.36
-3455.00
-117.38
214.02
178.64
0.00
3337.62
3669.01
As we can see from the table, the shifted pinch temperature is 185 oC, where is equal to 0. Therefore,
βˆ†π‘‡
ο‚· The pinch temperature for hot stream would be π‘‡π‘π‘–π‘›π‘β„Ž π‘“π‘œπ‘Ÿ β„Žπ‘œπ‘‘ π‘ π‘‘π‘Ÿπ‘’π‘Žπ‘š = 𝑇 ∗ π‘π‘–π‘›π‘β„Ž + 2π‘šπ‘–π‘› = 185℃ + 10℃ = 195℃.
ο‚·
The pinch temperature for cold stream would be π‘‡π‘π‘–π‘›π‘β„Ž π‘“π‘œπ‘Ÿ π‘π‘œπ‘™π‘‘ π‘ π‘‘π‘Ÿπ‘’π‘Žπ‘š = 𝑇 ∗ π‘π‘–π‘›π‘β„Ž −
βˆ†π‘‡π‘šπ‘–π‘›
2
= 185℃ − 10℃ = 175℃.
The hot utility target is 3455 kW, and the cold utility target is 3669.01 kW
3
For the flue gas required, from the problem table cascade in Table 2, a grand composite
curve was plotted, as shown in Figure 1.
Figure 1: Grand Composite Curve of the process in the base case scenario (dry recycle, no heating) with βˆ†π‘‡π‘šπ‘–π‘› = 20℃
The flue gas temperature will start at the theoretical flame temperature (1800 oC).
βˆ†π‘‡
This corresponds to a shifted temperature of 1800 ℃ − min −2𝑓𝑙𝑒𝑒 π‘”π‘Žπ‘  = 1800 ℃ −
25 ℃ = 1775℃ on the grand composite curve. The heat duty of the flue gas is equal to
the utility target of 3455 kW.
The flue gas profile is not restricted above the pinch, so it can be cooled to the pinch
temperature of 185 oC before venting to the atmosphere.
βˆ†π‘‡
The actual stack temperature would be 185 ℃ + min −2𝑓𝑙𝑒𝑒 π‘”π‘Žπ‘  = 185 ℃ + 25 ℃ = 210℃.
The actual stack temperature is above the acid dew point of 125 oC.
The Grand Composite Curve with the Hot Utility is shown in Figure 2.
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Figure 2: Grand Composite Curve of the process and flue gas as hot utility in the base case scenario (dry recycle, no heating)
with βˆ†π‘‡π‘šπ‘–π‘› = 20℃
For the fuel consumption,
πΆπ‘ƒπΉπΏπ‘ˆπΈ 𝐺𝐴𝑆
π‘„π»π‘šπ‘–π‘› = 3455 π‘˜π‘Š
π‘„π»π‘šπ‘–π‘›
3455
=
=
= 2.17 π‘˜π‘Š/𝐾
βˆ†π‘‡
1775 − 185
The fuel consumption is calculated for flue gas from theoretical flame temperature to
ambient temperature
π‘„πΉπΏπ‘ˆπΈ 𝐺𝐴𝑆 π‘Ÿπ‘’π‘žπ‘’π‘–π‘Ÿπ‘’π‘‘ = πΆπ‘ƒπΉπΏπ‘ˆπΈ 𝐺𝐴𝑆 × βˆ†π‘‡ = 2.17 × (1800 − 20) = 3867.86 π‘˜π‘Š
πΉπ‘’π‘Ÿπ‘›π‘Žπ‘π‘’ 𝑒𝑓𝑓𝑖𝑐𝑖𝑒𝑛𝑐𝑦 =
π‘„π»π‘šπ‘–π‘›
π‘„πΉπΏπ‘ˆπΈ 𝐺𝐴𝑆 π‘Ÿπ‘’π‘žπ‘’π‘–π‘Ÿπ‘’π‘‘
× 100 =
3455
× 100 = 89.33%
3867.86
The flow rate of flue gas required is:
𝐹𝑙𝑒𝑒 π‘”π‘Žπ‘  π‘“π‘™π‘œπ‘€ π‘Ÿπ‘Žπ‘‘π‘’ = π‘„πΉπΏπ‘ˆπΈ 𝐺𝐴𝑆 π‘Ÿπ‘’π‘žπ‘’π‘–π‘Ÿπ‘’π‘‘ × π»π‘’π‘Žπ‘‘π‘–π‘›π‘” π‘£π‘Žπ‘™π‘’π‘’
1 π‘€π‘Š
𝑀𝐽
= 3867.86 π‘˜π‘Š ×
× 47.1
= 0.082 π‘˜π‘”/𝑠
1000 π‘˜π‘Š
π‘˜π‘”
For the CO2 stack emissions:
The stack loss is calculated for flue gas from stack temperature to ambient air temperature
π‘„π‘†π‘‘π‘Žπ‘π‘˜ π‘™π‘œπ‘ π‘  = πΆπ‘ƒπΉπΏπ‘ˆπΈ 𝐺𝐴𝑆 × βˆ†π‘‡ = 2.17 × (210 − 20) = 412.86 π‘˜π‘Š
The CO2 stack emissions are
𝐢𝑂2 π‘ π‘‘π‘Žπ‘π‘˜ π‘’π‘šπ‘–π‘ π‘ π‘–π‘œπ‘› = π‘„π‘†π‘‘π‘Žπ‘π‘˜ π‘™π‘œπ‘ π‘  × πΈπ‘šπ‘–π‘ π‘ π‘–π‘œπ‘› πΉπ‘Žπ‘π‘‘π‘œπ‘Ÿ
1 πΊπ‘Š
𝐢𝑂2
π‘˜π‘” 𝐢𝑂2 3600𝑠
= 412.86 π‘˜π‘Š × 6
× 58.3 π‘˜π‘”
= 0.024
×
10 π‘˜π‘Š
𝐺𝐽
𝑠
1β„Žπ‘Ÿ
= 86.65 π‘˜π‘” 𝐢𝑂2 /β„Žπ‘Ÿ
The design scenarios will produce 281 kg/hr H2. Therefore, CO2 footprint of SOEC process is
5
𝐢𝑂2 π‘“π‘œπ‘œπ‘‘π‘π‘Ÿπ‘–π‘›π‘‘ =
𝐢𝑂2 π‘ π‘‘π‘Žπ‘π‘˜ π‘’π‘šπ‘–π‘ π‘ π‘–π‘œπ‘›
86.65 π‘˜π‘” 𝐢𝑂2 /β„Žπ‘Ÿ
=
= 0.31 π‘˜π‘” 𝐢𝑂2 /π‘˜π‘” 𝐻2
𝐻2 π‘π‘Ÿπ‘œπ‘‘π‘’π‘π‘‘π‘–π‘œπ‘›
281 π‘˜π‘” 𝐻2 /β„Žπ‘Ÿ
Question 3
Above Pinch
Figure 3: Heat exchange network design for the above pinch region
The heat exchange network is designed such that the hot utility target of 3455 kW is
supplied by the cooling of flue gas in the above pinch region, as represented by the red
“heat exchangers” in Figure 3. The boiler is divided into three parts namely the boiler
feedwater (BFW) pre-heater, the steam generator, and the superheater and are given by
streams 1a, 1b and 1c respectively. Figure 3 shows the heat exchange network design for
the above pinch region which treats flue gas as a hot stream in order to show how heat is
exchanged from the flue gas to the boiler. Heat exchange between the flue gas and the
steam generator (Stream 1b) principally relies on radiant heat as the steam generator will
typically operate at a very high pressure, whereby the CP of steam is high enough for
cooling the flue gas at its hottest end. The pre-heater (Stream 1a), as it operates at the
lowest pressure in the boiler, is placed at the colder end of the flue gas stream and the
superheater (Stream 1c) in between the two. Since the CPs of streams 1a and 1c are
significantly lower, both the pre-heater and superheater will rely on convective heat from
the flue gas.
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Below Pinch
Figure 4: Heat exchange network design for the below pinch region
Figure 4 shows the heat network design for the below pinch region, whereby cold utilities
are placed in streams 5 and 6, totalling up to 3669.01 kW which matches the cold utility
target that has been calculated in question 2.
Question 4
The heat exchanger which exchanges heat between Stream 1a and Stream 6 has the heat
duty of 66.9 kW. The heat duty is well below 100 kW, which is the standard of a normal
small heat exchanger. Therefore, if possible, this heat duty should be removed for the fact
that it is not efficient to invest capital in such a small duty heat exchanger.
The CP of flue gas in this scenario (dry recycle, no heating) is 2.17 kW/K. However, in other
cases with dry recycling and moderate heating, the CP of flue gas is slightly lower at 2.11
kW/K. It is expected that with more heating, the lower the CP of flue gas. With heating, the
feed temperature is higher, the temperature difference smaller, and thus the CP is lower
𝑄
since 𝐢𝑃 = βˆ†π‘‡.
A higher CP means that more energy is required to raise or lower its temperature and there
is a higher number of heat transfer units. This is not cost-effective considering the capital
expenditure. Additionally, flue gas with a higher CP will take a longer time to be cooled
down, and hence the heat exchange with the boiler will also take a longer time. Therefore,
various improvements could be made to lower the CP of the flue gas as seen in the other
scenarios which include a recycling stream and heating.
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