process design for coal liquefaction
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I S H A R U S T A G I ( 2 0 0 9 C H 7 0 7 2 1 )
M A T T H E W G E O R G E ( 2 0 0 8 C H 7 0 1 1 7 )
N I K H I L G O Y A L ( 2 0 0 9 C H 7 0 1 4 7 )
Process Design for Coal
Liquefaction1
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Different Routes for Coal to Liquid2
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World Oil and Coal Reserves3
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Coal Liquefaction
Portion of Organic Coal Substance converted toliquid products
Key Objectives: Producing liquids by chemically altering the coal structure
Increasing the content of hydrogen relative to carbon
Simultaneous Removal of nitrogen, sulfur, oxygen, and
mineral matter
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Liquefaction Methods
Pyrolysis: Coal conversion at a T> 400 deg. C in a non-oxidizing atmosphere to
gases, liquids, and char.
Indirect: Coal reaction with O2 & H2O high T to produce a mixture of CO &
H2 (synthesis gas), which can be catalytically converted to liquidproducts.
Direct: Coal reacts at high P & T with gaseous H2 and a solvent (Hydrogen-
donor) followed by conversion to liquids using or without addedcatalysts.
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Indirect Liquefaction
Step-1: Coal Gasification
Includes the endothermic reactions of carbon with steam andcarbon dioxide and the exothermic reaction of carbon with
oxygen.
Additional reactions include coal de-volatilization, the watergas shift reaction and the methanation reaction
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Coal Gasification
Important Considerations:
H2/CO ratio in the exit gas- an important parameter in FTsynthesis (step-2)
WGS Catalysts:
High T (440-700oC): Cr/Fe oxide or Zn/Cr oxide
Low T (230-350oC): Cu/Cr Oxide
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Importance of Catalysts in Coal Liquefaction
Stabilization of Free-Radicals formed during thermaldecomposition takes place by hydrogen abstraction fromeither hydrogen donor substances or molecular hydrogenactivated by a catalyst
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Catalyst Functions
Activate molecular hydrogen and transfer it to coalfragment radicals
Increase hydrogen transfer to the coal by hydrogenatingsolvent species to produce H-donor compounds
Increase coal conversion and yield of oil fractions
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Step 2: Syn-Gas Catalytic Conversion
Fischer-Tropsch Synthesis Wide range of products hydrocarbons, alcohols, aldehydes,
ketones, and acids
Common catalytic route: High Temperature Fischer Tropsch (HTFT): 330-350 0C
Fused Iron catalysts used*
Product fraction gasoline and light olefins
Low Temperature Fischer Tropsch (LTFT): 220-250 0C Precipitated alkali promoted Iron catalyst or supported Cobalt catalyst
used*
Product fraction waxes, diesel fuel
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Reaction Mechanism11
H2 adsorption:
Dissociative in nature with heats of adsorption in the orderCo> Ni > Fe
Alkali metals and oxides used as promoters affect hydrogen-
metal bond strength
CO adsorption:
Both dissociative (on Cr, Mn, Fe) and molecular (Co, Ni, Ru) On Ni, CO easily dissociates, forming methane while on Co and
Fe, strong metal-carbon bonds lead to C2+ compounds
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Carbide Mechanism for Fischer Tropsch SynthesisRef: A. T. Bell, Catal. Rev.Sci. Eng., 23, 203 (1981)
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Reaction Mechanism
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Advantages of Coal based liquid fuels14
Energy independence: Consumption = 14 MB-liquid fuels/day
Import = 55% Oil
Recoverable Coal Reserves = 270 billion tons
Potential Oil Production = 2 MB/day
Use in gasoline engines
ICTL process plants can easily be converted tohydrogen fuel cell production plants, once fuel celltechnology becomes more viable.
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Process Flow Sheet15
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Exergy Analysis
For the quantification of the environmentalperformance and comprehensive energy efficiencyof the system
Based on the second law analysis of the system
Maximum efficiency is attained for a process inwhich exergy is conserved
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Exergy Analysis
The process was divided into 5 CVs including:
ASU
Gasifier
Gas Cooling and scrubbing section
WGS and gas leaning
Fuel synthesis, and steam cycle.
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Calculation Steps20
The sum of the work in and out of a control volume is calculated.
The heat that crosses a control volume and the averagetemperature related to the heat streams are calculated.
Mass Conservation is verified to confirm that the system isoperating at steady state.
The flow rates that cross a control volume are identified andcalculated.
The specific exergy of each flow crossing a control volume iscalculated.
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Definitions21
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Results
Flow Streams/ ParametersSingle-Stage 2-Stage
Consumables
Coal Fed (ton/day) 11,400 10,800
O2 Fed (ton/day) 8800 7560
Water Consumption (ton/day) 1890 2230
Power
Steam Turbine (MW) 210 266
Parasitic Load -201 -236
ASU -130 -124
Acid Removal -8 -8
Others -63 -104
Net Power Output 0 30
Products
FT-Oil (m3/hr) 146 146
Energy Efficiency (LHV) 43 47
Exergy Efficiency 41 44
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F-T Unit
Consists of: F-T Reactor
Water Separation Unit
Tail Gas Recycle Loop
F-T YieldF-T Selectivity
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F-T Reactor Mass Balance24
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According to the Mass Balance, CO conversion = 50%
H2 conversion = 60 %
Also, a large amount of water is produced.
A steam system is installed.
F-T Reactor Mass Balance25
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Exergy Analysis
Exergetic efficiency for the reference case (taking theyield to be 90%) comes out to be 62%
Output energy is contained in the hydrocarbonproduct (95%) as well as the tail gases that are usedto derive power through the steam system (5%)
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Lost Work
Gasifier FT-Unit Power PlantASU
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Process Simulation using ASPEN Plus28
Gasification Process:
Chemical reactions in coal gasification (adapted from Perry et al., 2008)
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Gasification29
Reaction Sequence
Reaction sequence for the gasification of coal (adapted from Higman et al., 2003)
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ASPEN PFD31
OXYGEN
GASIFIER SYNGAS
MIXER
COAL
WATER
SLURRY
B1
SYNAPP
F
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Yield as a function of P & T32
Yield: No. of k-moles of Syn-gas per kg of MAF-Coal
0.0000
0.0100
0.0200
0.0300
0.0400
0.0500
0.0600
0.0700
800.00 1000.00 1200.00 1400.00 1600.00
Syn-Gasyield
Temperature (K)
P=30
P=10
P=50
P=70
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Assumptions: Equilibrium Operation
of the reactor undergiven T/P conditions
H2/CO ratio = 2 atT= 670 K (400 oC)
WGS Reactor: H2/CO ratio as a function of T
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0
0.5
1
1.5
2
2.5
3
3.5
400 600 800 1000 1200
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WGS Reactor Model35
Mass Balance: Equilibrium conversion (Xe) in terms of equilibrium constant (Keq)A: H2O, B: CO
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WGS Reactor: Non-Isothermal Adiabatic Model
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Assumptions: Specific heat (cP) of species and reaction heat (HRX) is
independent of pressure at which reaction takes place.
cP of species remain constant at the average of the reactor feed
temperature and calculated equilibrium (or reactor outlet)temperature.
Adiabatic reactor: Q = 0.
No work in reactor: W = 0.
All reactants enter the reactor at the same temperature,therefore Ti0 = T0
No phase changes occurs in reactor
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Non-Isothermal Adiabatic Model (contd..)37
Energy Balance: Relationship between temperatureand equilibrium conversion (XEB)
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Maximum Conversion38
Intersection of the Mass & Heat Balance curves
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WGS reactor model results39
Comparison of model results for different H2O/COfeed ratios
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WGS Reactor Model Results40
Comparison of model results for different feedtemperatures
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LTFT vs. HTFT41
LTFT Flow-sheet
HTFT Flow-sheet
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LTFT vs. HTFT43
FT step is marginally more expensive for the HTFTtechnology and nearly double the cost for the LTFTroute when compared to natural gas conversion
Comparison between the HTFT and LTFT options, itis clear that the LTFT route is more efficient
The main reason for the lower efficiency of the HTFT
option is that the acid gas removal step becomesmore utility intensive.
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Poly-generation System in FT process44
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MEB, Electricity produced and Utilities balance
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Items Units FT-100 FT-70 FT-30 FT-00Feedstocks
Coal t/h 1180 1180 1180 1180
Limestone t/h 130 130 130 130
Oxygen for the gasification t/h 984 986 984 984
Steam for the gasification t/h 142 142 142 142
CO2 for coal feeding in the gasification t/h 185 185 185 185
Scrubbing water in the gasification t/h 325 325 325 325
Steam into the WGS reactor t/h 139 432 821 1114
Air used in the Claus process t/h 6 6 6 6
Air used in the gas turbine t/h 1130 6495 13557 18878
Main products
Diesel t/h 242 170 73 0
Naphtha t/h 86 61 26 0
LPG t/h 47 33 14 0
Sulfur recovered t/h 3 3 3 3
Utilities
Making-up water t/h 4474 5066 6005 6710Electricity consumption MW 601 595 586 579
Electricity
Generated by the gas turbine MW 136 830 1749 2435
Generated by the steam turbine MW 458 833 1209 1494
Sub-total of electricity MW -8 1068 2374 3350
EFF % 48.3 44.9 39 34.6
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References
F. Fischer and H. Tropsch, Brennst. Chem., 4, 276 (2003).
J. M. Fox III, Catal. Rev.Sci. Eng., 35, 169 (1998).
J. H. Gregor, Catal. Lett., 7, 317 (1990). O.P.R. van Vliet et al. FischerTropsch diesel production in a well-to-wheel
perspective: A carbon, energy flow and cost analysis. Energy Conversion andManagement 50 (2009) 855876.
M. E. Dry and J. C. Hoogendoorn, Catal. Rev.-Sci. Eng., 23, 265 (1981).
B. Jager and R. Espinoza, Catal. Today, 23, 17 (1995).
Andre P. Steynberg, Herman G. Nel. Clean coal conversion options using FischerTropsch technology. Fuel 83 (2004) 765770
G.W. Yu et al. Process analysis for polygeneration of FischerTropsch liquids andpower with CO2 capture based on coal gasification. Fuel 89 (2010) 1070-1076.
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