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www.ijemr.net ISSN (ONLINE): 2250-0758, ISSN (PRINT): 2394-6962
173 Copyright © 2018. IJEMR. All Rights Reserved.
Volume-8, Issue-5, October 2018
International Journal of Engineering and Management Research
Page Number: 173-176
DOI: doi.org/10.31033/ijemr.8.5.07
Analysis of Steady State Cryogenic Air Separation Unit and Simulation of
Fixed Bed Adsorption Separation of Air
Siddharth Ranjan Mohanty1
and Dr. A.M. Mohanty2
1
M.Tech Scholar, Department of Designing and Manufacturing Mechanical, Centurion University, INDIA
2
Professor, Department of Mechanical Engineering, Centurion University, INDIA
3
Corresponding Author: mohantysiddharth087@gmail.com
ABSTRACT
Atmospheric dry air contains approximately 78%
nitrogen, 21% oxygen, and 1% argon plus low concentrations
of noble gases like carbon dioxide, hydrocarbons and other
impurities. An air separation unit divides atmospheric air
into the three pure gaseous components (nitrogen, oxygen
and argon). Nitrogen, oxygen and argon are used by industry
in large quantities and hence termed industrial gases. The
current work aim is to simulate the cryogenic air separation
unit including adsorber and cryogenic distillation. Simulation
of absorber is carried out using ADSIM of Aspen Tech to
remove carbon dioxide (CO2) and water vapour (H2O). The
breakthrough curves of carbon dioxide (CO2) and water
vapour on 5A molecular sieve and activated alumina
respectively are found at different Reynolds number. The
study helps to find out schedule time adsorber/desorber unit.
ASPEN Plus simulator is used to simulate cryogenic air
separation into nitrogen, oxygen and argon.
Keywords— Cryogenic, Distillation Column, Pressure
Swing Adsorption, Aspen Plus, Aspen Dynamics, Aspen
Adsim, Steady State Simulation, Composition, Molecular
Sieve, Activated Alumina, Isotherm Parameter
I. INTRODUCTION
The first application of computer control an air
separation plant was done in the early 1970s. Since that
time, best advanced control technologies have been useful
to improve the productivity and efficiency of air separation
plant [1].
The components presented in air (Oxygen,
Nitrogen, Argon etc.) are very often useful components in
chemical technology. The biggest marketplaces for oxygen
are in primary metals production, gasification and
chemicals, petroleum refineries, concrete and glass
products, clay and welding. Gaseous nitrogen (N2) is used
in the petroleum and chemical industries and it is also used
widely by the metals industries and electronics for its inert
properties. Liquid nitrogen (LN2) is used in applications
ranging from food freezing to cryogenic grinding of
plastics. Argon, the third key constituent of air, uses as
mostly in steelmaking, heat treating, welding, and
manufacturing procedures for electronics.
Techniques such as Membrane, PSA (Pressure
Swing Adsorption) and VPSA (vacuum Pressure Swing
Adsorption), are normally used to separate a single
constituent from normal air. The only possible sources of
the rare gases krypton, xenon, and neon are the distillation
of air using at least two distillation columns.
II. EXPERIMENTAL WORK
Process of Cryogenic Air Separation
The process is shown on the attached process
flow sheet.
Air compression
In the mechanical air filter the process air is
cleaned from dust and other particles. It is then
compressed to the required process pressure by a
multistage, intercooled turbo compressor.
Pre-cooling
The process air cooler cool down and washes the
compressed air in counter flow with water. There are two
streams of water injected into air cooler, cooling water at
normal temperature at the lower section and chilled water
from evaporation cooler and refrigeration units at the top
of air cooler.
The descending cooling water also scrubs the
water-soluble chemical impurities from the process air. A
wire mesh on top of the process air cooler removes the
water mist from the process air. In the evaporation cooler
the dry and pressure less nitrogen absorbs part of the
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174 Copyright © 2018. IJEMR. All Rights Reserved.
injected cool water. The required heat for the evaporation
is provided by the water which is cooled down by this
effect. This water is called chilled water. The water losses
of this system due to evaporation will be recovered by
cooling water out of the cooling water system.
Purification with molecular sieve
The air purification system comprises two cyclic
operating adsorber vessels passing through an adsorber
vessel, the molecular sieve retains the remaining moisture,
CO2 and potentially hazardous hydrocarbons from the air
steam.
While one adsorber is purifying the air, the other
adsorber is regenerated. During the heating cycle the
regeneration gas (waste nitrogen gas from the coldbox) is
heated by an electric heater and desorbs water and CO2
from the molecular sieve. During the cooling cycle the
heater is switched off and the adsorbent is cooled down
with cold dry waste nitrogen gas. After the completion of
the regeneration sequence, the adsorber is pressurized
before being switched over to the adsorption cycle.
The regeneration cycle consist mainly heating,
cooling, pressurizing and depressurizing.
The regeneration gas coming from the
rectification unit as waste gas is heated up in the
regeneration gas electrical heater at heating period. At the
cooling period the heater is bypassed. An important
indication for sufficient regeneration is the regeneration
peak temperature which appears during the cooling cycle.
At the end of the regeneration cycle the regenerated
adsorber is set into operation and the other one starts with
a new regeneration cycle.
Process refrigeration
The main stream of the purified air enters the
coldbox. It is cooled down in the main heat exchanger to
about liquefaction temperature while the cold gaseous
oxygen and nitrogen streams cooling from the column are
heated up. The air is feed to the bottom section of the
pressure column.
A side steam of the purified air is channelled
through the booster heat exchanger. Afterward the stream
is split in two. One fraction is further compressed by a
multistage intercooled turbo-type air booster compressor
while the second one is compressed by the turbine coupled
booster compressors with after cooler. Both streams are
cooled down in the booster heat exchanger and in the main
heat exchanger. The turbine boostered stream leaves the
main heat exchanger in the middle section and is expanded
in the expansion turbine. The gaseous air is fed into the
middle section of the low pressure column. A second
turbine is on stand-by and can be used during start up to
accelerate the cooling down process [33]. The air stream
passes the booster heat exchanger. This side stream is then
cooled in the main heat exchanger, where it serves as
heating medium to evaporate and warm up the internally
compressed product (LOX). Downstream the heat
exchanger this side stream is expanded into the pressure
column by an expansion valve.
Air separation
In the pressure column the air is separated into
pure N2 at the top, and oxygen enriched liquid air at the
bottom. The required reflux for the rectification is
provided by condensing the gaseous nitrogen in the
condenser/reboiler. The condensation heat of the nitrogen
is transferred to the boiling oxygen. Part of the liquid
nitrogen serves as reflux for the pressure column. The
other part is used as reflux for the low pressure column
[32, 34]. Part of the N2 is withdrawn from the top of the
pressure column and passes the main heat exchanger
before it serves as sealgas for the plant. In the low pressure
column the final separation takes place into pure oxygen at
the bottom and pure nitrogen at the top. Liquid oxygen
from the bottom of the low pressure column evaporates in
the condenser/reboiler and rises in the low pressure
column. The gaseous oxygen product originates at the
bottom of the low pressure column. The oxygen internal
compression pump increases the pressure to the required
value. The pressurized liquid evaporates and warms up in
the main heat exchanger while high pressure air coming
from the booster air compressor cools down and liquefies.
The oxygen leaves the coldbox as high pressure gaseous
oxygen product. Liquid oxygen product is withdrawn at
the top of the main condenser and channeled to the oxygen
storage system.
Liquid nitrogen product is withdrawn at the top of
the low pressure column and transferred to the nitrogen
storage system. Impure gaseous nitrogen (GAN) from the
top of the low pressure column warms up in the sub-cooler
and in the main heat exchanger and split into two streams.
One stream passes the evaporation cooler in order to
produce chilled water for the process air cooler. The
remaining part is used as regeneration gas and passes the
regeneration gas heater and molecular sieve adsorbers.
Argon production by rectification
In the crude argon column the oxygen is removed
from the crude argon by means of cryogenic rectification.
Argon enriched gas from the low pressure column is used
as a feed for the crude argon column. The oxygen free
crude argon on the top of the crude argon column
condenses in the crude argon condenser exchanging heat
with oxygen enriched liquid from the pressure column.
The liquid crude argon serves as reflux. After passing the
crude argon condenser part of the oxygen free crude argon
is withdrawn at the top of the crude argon column and fed
to the middle section of the pure argon column. In the pure
argon column the remaining nitrogen is removed by
cryogenic rectification. The top gas of the pure argon
column liquefies in the condenser against boiling, oxygen
rich liquid from the pressure column. The liquid argon
serves as reflux for the rectification.
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175 Copyright © 2018. IJEMR. All Rights Reserved.
The remaining nitrogen does not condense and is
vented from the outlet of the pure argon condenser to
atmosphere. Liquid argon from the sump of the pure argon
column is evaporated in the pure argon evaporator and fed
back to the column. Pure liquid argon is withdrawn as
product from the sump of the pure argon column and
transferred to the argon liquid storage tank.
Table No. 1 : Observation Table
Parameters Quantity
HP Column Pressure 535kpa to 549kpa
LP column pressure 133kpa to 140kpa
Crude argon column pressure 123kpa to 138kpa
Pure argon column pressure 115kpa to 120kpa
No. of stage in HP column 62
No. of stage in LP column 80
No. of stage in crude argon column 175
No. of stage in pure argon column 50
Input air temperature 28.790
C
Input air pressure 101.3kpa
Input air molar flow rate 4521kgmole/h
Input air composition Nitrogen78.12%,
Oxygen20.95%,
Argon 0.93%
Figure No.1 Testing Lab
III. RESULT
The liquid oxygen product withdrawn from the
cold box is stored in an atmospheric flat bottom tank. This
liquid storage serves as a backup supply of oxygen in case
of a plant shut down. The liquid oxygen withdrawn from
the tank pressurizes to the required value by means of the
backup pumps, evaporates in the hot water bath vaporizer
and is fed to the high pressure gaseous oxygen buffer
vessels. Additionally a truck filling pump is available to
fill liquid oxygen into a truck.
The liquid nitrogen is stored in an atmospheric
flat bottom tank from where it is pressurized with the
backup pumps and evaporated in the hot water bath
vaporizer and is feed to the pressure reducing station
where the desired amounts of high- mid- and low pressure
GAN can be regulated. A buffer vessel for high pressure
gaseous nitrogen is available. The liquid storage serves for
backup the supply of pressure nitrogen in case of a
nitrogen compressor shut down. Additionally a truck
filling pump is available to fill liquid nitrogen into a truck.
The liquid argon is stored in a pressure tank from
where it is further pressurized with the backup pumps,
evaporated in the LAR backup evaporators and fed to the
pressure reducing station. A buffer vessel for high pressure
gaseous argon is available. The liquid storage with
evaporators serves as gaseous argon supply to the
customer. A truck filling pump is available to fill liquid
argon into a truck. Additionally liquid argon from the tank
can be pressurized, evaporated and bottled into gas
cylinders at the available station.
Gas purifications

Removal of CO2 from natural gas

Removal of organics from vent streams

Removal of NOx from N2


Removal of solvents and odors from air

Removal of water vapour from air and other gas
streams

Removal of SO2 from vent streams

Removal of sulphur compound from gas streams
Liquid purifications

Removal of water from organic solutions

Removal of organic from water

Removal of sulfur compounds from organic
solutions

Decolorization of solutions
This chapter discusses the simulated result of air
separation plant in steady state, purity level of product
gases, performance of column, carbon dioxide (CO2) and
water vapour (H2O) adsorption in adsorber.
IV. CONCLUSION
From the present work we can summarize the
followings;
In this thesis report, we conclude that an air
separation plant processing 4702 kmol/hr of air to the basic
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176 Copyright © 2018. IJEMR. All Rights Reserved.
air components Nitrogen (3667.4037 kmol/hr), Oxygen
(985.26 kmol/hr) and Argon (42.39 kmol/hr) was
designed. Purity of produced Nitrogen is 99.6%, Oxygen is
99.4% and purity of Argon is 99.5%. But Rourkela steel
plant purity of product nitrogen is 99.99%, oxygen is
99.55% - 99.8% and argon is 99.9%.
To simulate cryogenic air separation unit, ASPEN
Plus software is used.
At stable states, the breakthrough time of CO2 is
about 267 minute and H2O is about 67 minute. But
Rourkela steel plant breakthrough time of CO2 and H2O
are 240 minute.
To adsorb carbon dioxide (CO2) and water vapour
(H2O), molecular sieve and activated alumina bed are used.
Adsorber is simulated through ADSIM of Aspen Tech.
REFERENCES
[1] Vinson D. R. (2006). Air separation control
technology, Computers and Chemical Engineering, 30,
1436-1446.
[2] Smith A.R. & Klosek J. (2001). A review of air
separation technologies and their integration with energy
conservation processes. Fuel Processing Technology, 70,
115-134.
[3] Uma H. & Tomas P. (2009). Steady state and dynamic
simulation of crude oil distillation using aspen plus and
aspen dynamics. Petroleum & Coal, 51(2), 100-109.
[4] Liwei Y., Yunsong Y., Yun L., & Zaoxiao Z. (2010).
Energy saving opportunities in an Air separation process.
International Refrigeration and Air Conditioning
Conference, Purdue University. Available at:
https://pdfs.semanticscholar.org/7528/2e677cd18f740ad50
82c7e01cb566aeb579b.pdf.
[5] Agrawal. R. & Thorogood R. M. (1991). Production of
medium pressure nitrogen by cryogenic air separation.
Butterworth Heinemann Ltd., 5, 203.
[6] Manjare S. D. & Ghoshal A. K. (2005). Studies on
dynamic adsorption behavior of ethyl acetate from air on
5A and 13X Molecular Sieves. The Canadian Journal of
Chemical Engineering, 83, 233.

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Analysis of Steady State Cryogenic Air Separation Unit and Simulation of Fixed Bed Adsorption Separation of Air

  • 1. www.ijemr.net ISSN (ONLINE): 2250-0758, ISSN (PRINT): 2394-6962 173 Copyright © 2018. IJEMR. All Rights Reserved. Volume-8, Issue-5, October 2018 International Journal of Engineering and Management Research Page Number: 173-176 DOI: doi.org/10.31033/ijemr.8.5.07 Analysis of Steady State Cryogenic Air Separation Unit and Simulation of Fixed Bed Adsorption Separation of Air Siddharth Ranjan Mohanty1 and Dr. A.M. Mohanty2 1 M.Tech Scholar, Department of Designing and Manufacturing Mechanical, Centurion University, INDIA 2 Professor, Department of Mechanical Engineering, Centurion University, INDIA 3 Corresponding Author: mohantysiddharth087@gmail.com ABSTRACT Atmospheric dry air contains approximately 78% nitrogen, 21% oxygen, and 1% argon plus low concentrations of noble gases like carbon dioxide, hydrocarbons and other impurities. An air separation unit divides atmospheric air into the three pure gaseous components (nitrogen, oxygen and argon). Nitrogen, oxygen and argon are used by industry in large quantities and hence termed industrial gases. The current work aim is to simulate the cryogenic air separation unit including adsorber and cryogenic distillation. Simulation of absorber is carried out using ADSIM of Aspen Tech to remove carbon dioxide (CO2) and water vapour (H2O). The breakthrough curves of carbon dioxide (CO2) and water vapour on 5A molecular sieve and activated alumina respectively are found at different Reynolds number. The study helps to find out schedule time adsorber/desorber unit. ASPEN Plus simulator is used to simulate cryogenic air separation into nitrogen, oxygen and argon. Keywords— Cryogenic, Distillation Column, Pressure Swing Adsorption, Aspen Plus, Aspen Dynamics, Aspen Adsim, Steady State Simulation, Composition, Molecular Sieve, Activated Alumina, Isotherm Parameter I. INTRODUCTION The first application of computer control an air separation plant was done in the early 1970s. Since that time, best advanced control technologies have been useful to improve the productivity and efficiency of air separation plant [1]. The components presented in air (Oxygen, Nitrogen, Argon etc.) are very often useful components in chemical technology. The biggest marketplaces for oxygen are in primary metals production, gasification and chemicals, petroleum refineries, concrete and glass products, clay and welding. Gaseous nitrogen (N2) is used in the petroleum and chemical industries and it is also used widely by the metals industries and electronics for its inert properties. Liquid nitrogen (LN2) is used in applications ranging from food freezing to cryogenic grinding of plastics. Argon, the third key constituent of air, uses as mostly in steelmaking, heat treating, welding, and manufacturing procedures for electronics. Techniques such as Membrane, PSA (Pressure Swing Adsorption) and VPSA (vacuum Pressure Swing Adsorption), are normally used to separate a single constituent from normal air. The only possible sources of the rare gases krypton, xenon, and neon are the distillation of air using at least two distillation columns. II. EXPERIMENTAL WORK Process of Cryogenic Air Separation The process is shown on the attached process flow sheet. Air compression In the mechanical air filter the process air is cleaned from dust and other particles. It is then compressed to the required process pressure by a multistage, intercooled turbo compressor. Pre-cooling The process air cooler cool down and washes the compressed air in counter flow with water. There are two streams of water injected into air cooler, cooling water at normal temperature at the lower section and chilled water from evaporation cooler and refrigeration units at the top of air cooler. The descending cooling water also scrubs the water-soluble chemical impurities from the process air. A wire mesh on top of the process air cooler removes the water mist from the process air. In the evaporation cooler the dry and pressure less nitrogen absorbs part of the
  • 2. www.ijemr.net ISSN (ONLINE): 2250-0758, ISSN (PRINT): 2394-6962 174 Copyright © 2018. IJEMR. All Rights Reserved. injected cool water. The required heat for the evaporation is provided by the water which is cooled down by this effect. This water is called chilled water. The water losses of this system due to evaporation will be recovered by cooling water out of the cooling water system. Purification with molecular sieve The air purification system comprises two cyclic operating adsorber vessels passing through an adsorber vessel, the molecular sieve retains the remaining moisture, CO2 and potentially hazardous hydrocarbons from the air steam. While one adsorber is purifying the air, the other adsorber is regenerated. During the heating cycle the regeneration gas (waste nitrogen gas from the coldbox) is heated by an electric heater and desorbs water and CO2 from the molecular sieve. During the cooling cycle the heater is switched off and the adsorbent is cooled down with cold dry waste nitrogen gas. After the completion of the regeneration sequence, the adsorber is pressurized before being switched over to the adsorption cycle. The regeneration cycle consist mainly heating, cooling, pressurizing and depressurizing. The regeneration gas coming from the rectification unit as waste gas is heated up in the regeneration gas electrical heater at heating period. At the cooling period the heater is bypassed. An important indication for sufficient regeneration is the regeneration peak temperature which appears during the cooling cycle. At the end of the regeneration cycle the regenerated adsorber is set into operation and the other one starts with a new regeneration cycle. Process refrigeration The main stream of the purified air enters the coldbox. It is cooled down in the main heat exchanger to about liquefaction temperature while the cold gaseous oxygen and nitrogen streams cooling from the column are heated up. The air is feed to the bottom section of the pressure column. A side steam of the purified air is channelled through the booster heat exchanger. Afterward the stream is split in two. One fraction is further compressed by a multistage intercooled turbo-type air booster compressor while the second one is compressed by the turbine coupled booster compressors with after cooler. Both streams are cooled down in the booster heat exchanger and in the main heat exchanger. The turbine boostered stream leaves the main heat exchanger in the middle section and is expanded in the expansion turbine. The gaseous air is fed into the middle section of the low pressure column. A second turbine is on stand-by and can be used during start up to accelerate the cooling down process [33]. The air stream passes the booster heat exchanger. This side stream is then cooled in the main heat exchanger, where it serves as heating medium to evaporate and warm up the internally compressed product (LOX). Downstream the heat exchanger this side stream is expanded into the pressure column by an expansion valve. Air separation In the pressure column the air is separated into pure N2 at the top, and oxygen enriched liquid air at the bottom. The required reflux for the rectification is provided by condensing the gaseous nitrogen in the condenser/reboiler. The condensation heat of the nitrogen is transferred to the boiling oxygen. Part of the liquid nitrogen serves as reflux for the pressure column. The other part is used as reflux for the low pressure column [32, 34]. Part of the N2 is withdrawn from the top of the pressure column and passes the main heat exchanger before it serves as sealgas for the plant. In the low pressure column the final separation takes place into pure oxygen at the bottom and pure nitrogen at the top. Liquid oxygen from the bottom of the low pressure column evaporates in the condenser/reboiler and rises in the low pressure column. The gaseous oxygen product originates at the bottom of the low pressure column. The oxygen internal compression pump increases the pressure to the required value. The pressurized liquid evaporates and warms up in the main heat exchanger while high pressure air coming from the booster air compressor cools down and liquefies. The oxygen leaves the coldbox as high pressure gaseous oxygen product. Liquid oxygen product is withdrawn at the top of the main condenser and channeled to the oxygen storage system. Liquid nitrogen product is withdrawn at the top of the low pressure column and transferred to the nitrogen storage system. Impure gaseous nitrogen (GAN) from the top of the low pressure column warms up in the sub-cooler and in the main heat exchanger and split into two streams. One stream passes the evaporation cooler in order to produce chilled water for the process air cooler. The remaining part is used as regeneration gas and passes the regeneration gas heater and molecular sieve adsorbers. Argon production by rectification In the crude argon column the oxygen is removed from the crude argon by means of cryogenic rectification. Argon enriched gas from the low pressure column is used as a feed for the crude argon column. The oxygen free crude argon on the top of the crude argon column condenses in the crude argon condenser exchanging heat with oxygen enriched liquid from the pressure column. The liquid crude argon serves as reflux. After passing the crude argon condenser part of the oxygen free crude argon is withdrawn at the top of the crude argon column and fed to the middle section of the pure argon column. In the pure argon column the remaining nitrogen is removed by cryogenic rectification. The top gas of the pure argon column liquefies in the condenser against boiling, oxygen rich liquid from the pressure column. The liquid argon serves as reflux for the rectification.
  • 3. www.ijemr.net ISSN (ONLINE): 2250-0758, ISSN (PRINT): 2394-6962 175 Copyright © 2018. IJEMR. All Rights Reserved. The remaining nitrogen does not condense and is vented from the outlet of the pure argon condenser to atmosphere. Liquid argon from the sump of the pure argon column is evaporated in the pure argon evaporator and fed back to the column. Pure liquid argon is withdrawn as product from the sump of the pure argon column and transferred to the argon liquid storage tank. Table No. 1 : Observation Table Parameters Quantity HP Column Pressure 535kpa to 549kpa LP column pressure 133kpa to 140kpa Crude argon column pressure 123kpa to 138kpa Pure argon column pressure 115kpa to 120kpa No. of stage in HP column 62 No. of stage in LP column 80 No. of stage in crude argon column 175 No. of stage in pure argon column 50 Input air temperature 28.790 C Input air pressure 101.3kpa Input air molar flow rate 4521kgmole/h Input air composition Nitrogen78.12%, Oxygen20.95%, Argon 0.93% Figure No.1 Testing Lab III. RESULT The liquid oxygen product withdrawn from the cold box is stored in an atmospheric flat bottom tank. This liquid storage serves as a backup supply of oxygen in case of a plant shut down. The liquid oxygen withdrawn from the tank pressurizes to the required value by means of the backup pumps, evaporates in the hot water bath vaporizer and is fed to the high pressure gaseous oxygen buffer vessels. Additionally a truck filling pump is available to fill liquid oxygen into a truck. The liquid nitrogen is stored in an atmospheric flat bottom tank from where it is pressurized with the backup pumps and evaporated in the hot water bath vaporizer and is feed to the pressure reducing station where the desired amounts of high- mid- and low pressure GAN can be regulated. A buffer vessel for high pressure gaseous nitrogen is available. The liquid storage serves for backup the supply of pressure nitrogen in case of a nitrogen compressor shut down. Additionally a truck filling pump is available to fill liquid nitrogen into a truck. The liquid argon is stored in a pressure tank from where it is further pressurized with the backup pumps, evaporated in the LAR backup evaporators and fed to the pressure reducing station. A buffer vessel for high pressure gaseous argon is available. The liquid storage with evaporators serves as gaseous argon supply to the customer. A truck filling pump is available to fill liquid argon into a truck. Additionally liquid argon from the tank can be pressurized, evaporated and bottled into gas cylinders at the available station. Gas purifications  Removal of CO2 from natural gas  Removal of organics from vent streams  Removal of NOx from N2   Removal of solvents and odors from air  Removal of water vapour from air and other gas streams  Removal of SO2 from vent streams  Removal of sulphur compound from gas streams Liquid purifications  Removal of water from organic solutions  Removal of organic from water  Removal of sulfur compounds from organic solutions  Decolorization of solutions This chapter discusses the simulated result of air separation plant in steady state, purity level of product gases, performance of column, carbon dioxide (CO2) and water vapour (H2O) adsorption in adsorber. IV. CONCLUSION From the present work we can summarize the followings; In this thesis report, we conclude that an air separation plant processing 4702 kmol/hr of air to the basic
  • 4. www.ijemr.net ISSN (ONLINE): 2250-0758, ISSN (PRINT): 2394-6962 176 Copyright © 2018. IJEMR. All Rights Reserved. air components Nitrogen (3667.4037 kmol/hr), Oxygen (985.26 kmol/hr) and Argon (42.39 kmol/hr) was designed. Purity of produced Nitrogen is 99.6%, Oxygen is 99.4% and purity of Argon is 99.5%. But Rourkela steel plant purity of product nitrogen is 99.99%, oxygen is 99.55% - 99.8% and argon is 99.9%. To simulate cryogenic air separation unit, ASPEN Plus software is used. At stable states, the breakthrough time of CO2 is about 267 minute and H2O is about 67 minute. But Rourkela steel plant breakthrough time of CO2 and H2O are 240 minute. To adsorb carbon dioxide (CO2) and water vapour (H2O), molecular sieve and activated alumina bed are used. Adsorber is simulated through ADSIM of Aspen Tech. REFERENCES [1] Vinson D. R. (2006). Air separation control technology, Computers and Chemical Engineering, 30, 1436-1446. [2] Smith A.R. & Klosek J. (2001). A review of air separation technologies and their integration with energy conservation processes. Fuel Processing Technology, 70, 115-134. [3] Uma H. & Tomas P. (2009). Steady state and dynamic simulation of crude oil distillation using aspen plus and aspen dynamics. Petroleum & Coal, 51(2), 100-109. [4] Liwei Y., Yunsong Y., Yun L., & Zaoxiao Z. (2010). Energy saving opportunities in an Air separation process. International Refrigeration and Air Conditioning Conference, Purdue University. Available at: https://pdfs.semanticscholar.org/7528/2e677cd18f740ad50 82c7e01cb566aeb579b.pdf. [5] Agrawal. R. & Thorogood R. M. (1991). Production of medium pressure nitrogen by cryogenic air separation. Butterworth Heinemann Ltd., 5, 203. [6] Manjare S. D. & Ghoshal A. K. (2005). Studies on dynamic adsorption behavior of ethyl acetate from air on 5A and 13X Molecular Sieves. The Canadian Journal of Chemical Engineering, 83, 233.