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Winter Combustion School Madras December 15, 2015
Combustion Kinetics (4)
Solid Fuel Combustion
Eliseo Ranzi
Dipartimento di Chimica, Materiali e Ingegneria Chimica “G. Natta”Politecnico di Milano
Winter Combustion School Madras December 15, 2015
Outline 2
Combustion of solid fuels, characterization of solid fuel (plastics, coal, biomass, RDF), multistep kinetics of devolatilization and pyrolysis, secondary gas phase reactions, particle and reactor scale.
Winter Combustion School Madras December 15, 2015
3Solid Fuel Pyrolysis, Gasification and Combustion
Yin, C , Rosendahl , LA , Kaer , SK Prog. Energy Comb. Science 34 (2008) 725
A complex multi-componentmulti-phase
and multi-scale problem.
Biomass Travelling Grate Combustor
Winter Combustion School Madras December 15, 2015
AbstractDetailed chemistry of thermal treatments of solid fuels (large numbers ofspecies and reactions) requires careful simplifications.This multi-component and multi-phase problem requires to apply
chemical lumping procedures at four different levels:
1- Characterization of the Solid Fuel in terms of Reference Components2- Multistep Kinetic Models of Devolatilization of Reference Components3- Heterogeneous Gas-Solid Reactions of Char with O2/H2O/CO2
4- Secondary Gas-Phase Reactions of Tars and Volatile Components
The comprehensive description of coupled transport and kinetic processes, bothat particle and reactor scale, increases the mathematical complexity of solid fuelgasification and combustion.
Two application examples at the reactor scale:Countercurrent Coal or Biomass GasifierBiomass Combustor on a Travelling Grate
illustrate the viability of this approach.
A compromise needs to be found between computation efforts and prediction accuracy.
4
Winter Combustion School Madras December 15, 2015
5Mathematical Modeling of a Travelling Grate Combustor
Requires at least to analyse the three following features:- Solid Fuel Characterization- Kinetics
Pyrolysis of Solid Fuel (release of volatile components)Heterogeneous Reactions (char gasification and combustion)Homogeneous Reactions of gases and tars
- Mathematical Model Balance EquationsParticle and Reactor Scale
Courtesy Garioni-Naval_2012
Winter Combustion School Madras December 15, 2015
Solid Fuel Combustion 6
Coal
Plastics
Biomasses
MSW and RDF
Fuel Characterization
Kinetic schemes ofSolid Fuel DevolatizationChar GasificationSecondary Gas Phase Reax
Balance equations at the particle and reactor scale
Winter Combustion School Madras December 15, 2015
Outlines
•Solid Fuels Characterization•Biomass (Cellulose, Hemicellulose, Lignins, and Extractives)•Coal, Plastic and Refuse Derived Fuels
•Kinetic Models•Solid Fuel Pyrolysis and Devolatilization•Char Gasification and Combustion•Secondary Gas-Phase Reactions
•Comprehensive Multi-Scale and Multi-Phase Model •Balance Equations at Particle and Reactor Scale
•Application Examples•Countercurrent Coal and Biomass Gasifier •Biomass Combustor on a Travelling Grate
7
Winter Combustion School Madras December 15, 2015
8SOLID FUELS
Coal Plastics Biomasses
MSWMunicipal Solid
Wastes
Solid fuels
Mechanical selections
Refuse Derived Fuel (RDF)
Plastics(PE, PP, PET, PS)
Biomass(Wood, Tissue and Lignocellulosic..)
Winter Combustion School Madras December 15, 2015
straw
cellulosehemicellulose
agriculturalresidues
miscanthus
lignins
0 0.25 0.5 0.75 10
0.5
1.5
1
2
O/C atomic
H/C
atom
ic
Anthracite
lignitebituminous
coals
After: R.H. Hurt (1998) "Structure, properties, and reactivity of solid fuels." 27th Symposium on Combustion. 2887-2904
Solid Fuels in Van Krevelen Diagram.
MSWRDF
PMMA
PE/PP
PS
ABS
naylon-6
Plastics
9
Winter Combustion School Madras December 15, 2015
Solid Fuels in Van Krevelen Diagram. 10
0
0.5
1
1.5
2
0 0.2 0.4 0.6 0.8
H/C
Ato
mic
Rat
io
O/C Atomic Ratio
Van Krevelen Diagram
RDF
Coal
BiomassPlastics
Winter Combustion School Madras December 15, 2015
11
Physical structure of Biomass spans several orders of magnitude, from the atomic level of biopolymers (10-10 to 10-9 m) to the microstructured cellular network (10-5 to 10-3 m) to the macrostructures of thick particles and pellets (10-3 to 10-2 m) and finally to trees and grasses.
Multi-Scale Nature of Biomass.
Mettler et al., Energy Environ. Sci., 2012, 5, 7797
Winter Combustion School Madras December 15, 2015
Himmel et al., Biomass Recalcitrance: Engineering Plants and Enzymes for Biofuel Production. Science 2007 (2) 315; 804-807
Multi-Scale Nature of Cellulose.
Corn stover (scale 1 m) Scanning electron micrograph of the cross section of maize stem
(scale 50 μm)
Atomic force micrograph of the cellwall surface. The diameter of microfibril is 3-5 nm (scale 50 nm)
Winter Combustion School Madras December 15, 2015
Biomass composition:Cellulose, Hemicellulose and Lignin
Cellulose is the structural component of the primary cell wall of green plants. Cellulose is a linear polymer of up to 10,000 D-glucose molecules (C6H10O5)n
13
H-bonds between polymer chains
Winter Combustion School Madras December 15, 2015
Microfibril of Cellulose Cristallyte
Himmel et al., Biomass Recalcitrance: Engineering Plants and Enzymes for Biofuel Production. Science 2007 (2) 315; 804-807
Pectin (poly-galacturonic acid)forms a gel that glues the cell-wall components together.
Winter Combustion School Madras December 15, 2015
Biomass composition:Cellulose, Hemicellulose and Lignin
15
Hemicellulose is a complex mixture of different sugar monomers (xylose, mannose, galactose, arabinose,..)being xylose the most abundant. It is the biomass component with a high char formation tendency
Winter Combustion School Madras December 15, 2015
16Molecular Composition of Biomass
http://digital.library.okstate.edu/oas/oas_image_files/v72/p51_56Fig1.jpg
Cellulose and hemicellulose chains are embedded in lignin.
Winter Combustion School Madras December 15, 2015
Building blocks of lignin 17
lignin structure:chemical bonds and functional groups
Custodis, V. B., Bährle, C., Vogel, F., & van Bokhoven, J. A. (2015). Phenols and aromatics from fast pyrolysis of variously prepared lignins from hard-and softwoods. Journal of Analytical and Applied Pyrolysis, 115, 214-223.
There are three main alcohol monomers, with different methoxylation degree.
Coniferyl Synapyl Coumaryl
Lignin is a complex macromolecule with a high molecular mass (>10,000 uma)
It confers mechanical strength to the plant.
Winter Combustion School Madras December 15, 2015
18
F. Streffer (2014) Lignocellulose to Biogas and other Products. JSM Biotechnol Bioeng 2(1): 1023
Winter Combustion School Madras December 15, 2015
19
Wood species Cellulose Hemicellulose Lignin
SoftwoodsPicea glauca 41 31 27Abies balsamea 42 27 29Pinus strobes 41 27 29Tsuga canadensis 41 23 33Norway spruce 46 25 28Loblolly pine 39 25 31Thuja occidentalis 41 26 31
HardwoodsEucalyptus globulus 45 35 19Acer rubrum 45 29 24Ulmus americana 51 23 24Populus tremuloides 48 27 21Betula papyrifera 42 38 19Fagus grandifolia 45 29 22Agricultural residuesCorn stover 40 17 25Wheat straw 30 20 50
Switchgrass 45 12 30
Fengel D, Wegener G. Wood. Chemistry, ultrastructure, reactions. Walter de Gruyter: Berlin, 613 pp (1984).Zhang YP. Reviving the carbohydrate economy via multi-product lignocellulose biorefineries. J Ind Microbiol Biot 35:367-375 (2008).
Biochemical Analysis of Biomasses
Extractives:The biomass material that is soluble in either water or ethanol during exhaustive extraction.
Winter Combustion School Madras December 15, 2015
Water soluble extractives Phenolic Compounds
-H2O
Flavonoids
Condensed Tannins
Phenolic Acids
-H2O
Hydrolysable Tannins
+ Sugar
Winter Combustion School Madras December 15, 2015
Resin Acids
Fatty acids
-H2O
Water insoluble extractives
Resins
+ Glycerol
Fats/OilsTriglycerides
Terpens Monoterpens
Carotenoids
Winter Combustion School Madras December 15, 2015
Biomass Characterization: Proximate Analysis and TGA23
TGA is a recording of mass changes, as a function of a combination of temperature with time.
Devolatilization(300-600 °C)
100
80
60
40
20
0
Ashes
Time/Temperature
100
80
60
40
20
0
100
80
60
40
20
0
Drying(100°C)
Char Gasificationor Combustion(800-1200 °C)
Volatiles
Fixed Carbon and Ash
Humidity
Proximate Analysis is derived from Thermo Gravimetric Analysis (TGA)
The proximate analysis gives moisture, volatile content VM (when heated to 950 C), the remaining fixed carbon FC , the Ash (mineral) together with the high heating value (HHV).
Winter Combustion School Madras December 15, 2015
Proximate Analysis of typical Biomasses
25
A. Williams, J.M. Jones, L. Ma, M. Pourkashanian ‘Pollutants from the combustion of solid biomass fuels’ Progress in Energy and Combustion Science 38 (2012) 113-137
Winter Combustion School Madras December 15, 2015
Biomass Composition and Proximate Analysis 26
http://www.ieabcc.nl/workshops/task32_Lyon/full%20page/04%20David%20Baxter.pdf
The proximate analysis gives moisture, volatile content VM (when heated to 950 C), the fixed carbon FC remaining at that point, the Ash (mineral) together with the high heating value (HHV).
Proximate Analysis
Wt%
Coal
Biomass
Winter Combustion School Madras December 15, 2015
27Biomass Composition
http://www.ieabcc.nl/workshops/task32_Lyon/full%20page/04%20David%20Baxter.pdf
The ultimate analysis gives the composition of the biomass in weight percentage of Carbon, Hydrogen and Oxygen as well as Sulfur and Nitrogen.
Ultimate /Elemental Analysis (wt%)
Coal
Biomass
Winter Combustion School Madras December 15, 2015
Proximateand Ultimate (Elemental) Analysis
of typical Biomasses
28
A. Williams, J.M. Jones, L. Ma, M. Pourkashanian ‘Pollutants from the combustion of solid biomass fuels’ Progress in Energy and Combustion Science 38 (2012) 113-137
C/H/O atomic balances allow to define biomasscomposition in terms of three Reference Components
Winter Combustion School Madras December 15, 2015
Ultimate Analysis allows to derive
Biomass composition in terms of
Cellulose, Hemicellulose and Lignins Cotton
% Cellulose % Lignins
% Hemicellulose
Birch Bark
Biomass Characterization
Biomass is considered as a linear combination of Cellulose, Hemicellulose and Lignins
29
Ranzi, E., Cuoci, A., Faravelli, T., Frassoldati, A., Migliavacca, G., Pierucci, S., & Sommariva, S. (2008).Chemical kinetics of biomass pyrolysis. Energy & Fuels, 22(6), 4292-4300
Winter Combustion School Madras December 15, 2015
Biomass Characterization
5 reference species
3 elemental balances (C, H, O)
3 reference mixtures
BIOMASS
Winter Combustion School Madras December 15, 2015
Ultimate Analysis allows to derive
Biomass composition in terms of
Cellulose, Hemicellulose and Lignins Cotton
% Cellulose % Lignins
% Hemicellulose
Birch Bark
Biomass Characterization
Biomass is considered as a linear combination of Cellulose, Hemicellulose and Lignins
31
Ranzi, E., Cuoci, A., Faravelli, T., Frassoldati, A., Migliavacca, G., Pierucci, S., & Sommariva, S. (2008).Chemical kinetics of biomass pyrolysis. Energy & Fuels, 22(6), 4292-4300
Weight fraction of reference components:(daf basis)
Cellulose -C6H10O5- 0.329Hemicellulose -C5H8O4- 0.179LIGH -C22H28O9- 0.253LIGO -C20H22O10- 0.175LIGC -C15H14O4- 0.064
The biomass is described as a linear combination of 5 reference species.
It is then necessary to describetheir pyrolysis behavior
Winter Combustion School Madras December 15, 2015
Biomass Characterization 32
P. Debiagi et al (2015) Energy & Fuels, 22(6), 4292-4300.
Hydrophilic (Tannins) and hydrophobic (triglycerides)
extractives allow to extend the applicability of the
characterization method.
Winter Combustion School Madras December 15, 2015
Pyrolysis and Devolatilization of Biomass33
http://www.biomasstorrefaction.org/torrefaction/
Torrefied biomass has several benefits over untreated biomass:•Higher calorific value•More homogeneous product•Higher bulk density•Excellent grindability•Durability•Hydrophobic nature/water resistance•No biological activity
Winter Combustion School Madras December 15, 2015
Torrefaction 34
Torrefied biomass shows better transportation characteristics (lower handling and storage costs) compatible properties to coal (bulk energy density , heating value) grindability, and hydrophobicity.
Torrefaction reduces investment for co-firing application
Thermal pre-treatment technology, which produces a solid biofuel product with a superior handling, milling and co-firing capabilities compared to other biomass fuels.
Winter Combustion School Madras December 15, 2015
35
http://news.mongabay.com/bioenergy/2008/07/torrefaction-gives-biomass-20-energy.html
Winter Combustion School Madras December 15, 2015
Van Krevelen diagram for coals, biomass and torrefied biomass.
T.G. Bridgeman , J.M. Jones , I. Shield , P.T. Williams (2008 ) ‘Torrefaction of reed canary grass, wheat straw and willow to enhance solid fuel qualities and combustion properties’ Fuel 87(6) 844 - 856
Torrefaction is the first step of Biomass Pyrolysis Process
Torrefied biomass devolatilises and burns over a shorter temperature range.
Devolatisation profiles of untreated and treated reed canary grass (RCG).
Torrefied biomass has a higher combustion heat (higher fixed carbon).
The advantages are more pronounced at higher torrefaction temperatures.
36
Winter Combustion School Madras December 15, 2015
Torrefaction and Pyrolysis are the first steps in Thermal Treatments of Solid Fuels.
MSW
straw
cellulosehemicellulose
agriculturalresidues
miscanthus
lignins
0 0.25 0.5 0.75 10
0.5
1.5
1
2
O/C atomic
H/C
atom
ic
Anthracite
lignitebituminous
coals
RDF
PMMA
PE/PP
PS
ABS
naylon-6
Plastics
It is thus necessary to describethe chemical evolution of the solidfuels (i.e. the reference species )
towards the residual Char
37
Winter Combustion School Madras December 15, 2015
Cellulose Pyrolysis.Concerted Reactions and Mechanism of Glucose Pyrolysis and Implications for Cellulose Kinetics
38
V. Seshadri and P. R. Westmoreland ‘Concerted Reactions and Mechanism of Glucose Pyrolysis and Implications for Cellulose Kinetics’ J. Phys. Chem. A 2012, 116, 11997−12013
Formation of levoglucosan from β-D-glucose by dehydration.
Retro-aldol condensation of xylose
Winter Combustion School Madras December 15, 2015
Mechanism of formation of C1–C6 organic compounds from glucose
39
Intermediates produced from glucose via concerted reactions in the condensed phase. Glucose is short-lived and rapidly transforms to various melt phase and vapor phase species.
R. Vinu and L. J. Broadbelt (2012) ‘A mechanistic model of fast pyrolysis of glucose-based carbohydrates to predict bio-oil composition’ Energy Environ. Sci., 2012
Winter Combustion School Madras December 15, 2015
Ab initio molecular dynamics simulations are performed with α-cyclodextrin to reveal the pathways of cellulose pyrolysis.Homolytic cleavage of glycosidic linkages and furan formation directly from cellulose without
any small-molecule (e.g., glucose) intermediates are obtained.
M. S. Mettler, S. H. Mushrif, A. D. Paulsen, A. D. Javadekar, D. G. Vlachos and P. J. Dauenhauer ‘Revealing pyrolysis chemistry for biofuels production: Conversion of cellulose to furans and small oxygenates’ Energy Environ. Sci., 2012, 5, 5414-5424
Contrary to previous pyrolysis work using mm-scale cellulose samples, thin-film pyrolysis enables the study of condensed-phase pyrolysis chemistry under isothermal conditions and minimizes the breakdown of volatile products.
This work combines thin-film technology with first-principles computations to elucidate major condensed-phase pyrolysis paths.
Conversion of cellulose to furans and small oxygenates
α-cyclodextrin is an appropriate surrogate of cellulose.
40
Winter Combustion School Madras December 15, 2015
Reaction Pathways of α-cyclodextrin Pyrolysis.
M. S. Mettler et al., Energy Environ. Sci., 2012, 5, 5414-5424
41
Winter Combustion School Madras December 15, 2015
Oxygenated species from pyrolysis of cellulose and hemicellulose
42
Shen, D., Jin, W., Hu, J., Xiao, R., & Luo, K. (2015). An overview on fast pyrolysis of the main constituents in lignocellulosic biomass to valued-added chemicals: Structures, pathways and interactions. Renewable and Sustainable Energy Reviews, 51, 761-774.
Winter Combustion School Madras December 15, 2015
Average values are shown for thin-film pyrolysis at 500 C with 90% mean confidence intervals.
Compounds from thin-film pyrolysis experiments 43
Winter Combustion School Madras December 15, 2015
44
Shen, D., Jin, W., Hu, J., Xiao, R., & Luo, K. (2015). An overview on fast pyrolysis of the main constituents in lignocellulosic biomass to valued-added chemicals: Structures, pathways and interactions. Renewable and Sustainable Energy Reviews, 51, 761-774.
Primary Reaction Paths of Cellulose Pyrolysis
Levoglucosane
5-hydroxy-methyl-furfural
hydroxy-acetaldehyde
Winter Combustion School Madras December 15, 2015
Multistep Kinetic Model of Cellulose Pyrolysis
Cellulose
Levoglucosane
DecompositionProducts
Active Cellulose
Char + H2OReaction Kinetic constant
[s-1]Reaction
Heat [kj/kg]
Cellulose → Active Cellulose 8×1013 exp (-45000/RT) 0
Active Cellulose → Acetic Acid + 0.2 Glyoxal + 0.2 CH3CHO + 0.25 HMFU + 0.2 C3H6O + 0.22 CO2 + 0.16 CO + 0.83 H2O + 0.1 CH4 + 0.01 HCOOH + 0.01G{H2} + 0.61 Char
1×109 exp (-30000/RT)
650
Active Cellulose → Levoglucosane 4×T exp (-10000/RT) 490
CELL → 5 H2O + 6 Char 8×107 exp (-31000/RT) -1800
45
Bradbury, A. G., Sakai, Y., & Shafizadeh, F. (1979). A kinetic model for pyrolysis of cellulose. Journal of Applied Polymer Science, 23(11), 3271-3280.Ranzi, E., Cuoci, A., Faravelli, T., Frassoldati, A., Migliavacca, G., Pierucci, S., & Sommariva, S. (2008). Chemical kinetics of biomass pyrolysis. Energy & Fuels, 22(6), 4292-4300. Energy & Fuels, 2008, 4292-4300
These reactions not only describe the residual char (Broido-Shafizadeh model), but also give a guess
of the composition of released tar and gases.
Winter Combustion School Madras December 15, 2015
Validation of Cellulose Pyrolysis ModelComparisons with experimental TG data
Temperature °C300 400 500 600
0.1
0.2
0.3
0.4
0.5
.
Levoglucosano
HAA
300 400 500 600
0.1
0.2
0.3
0.4
0.5
Mol
e Fr
actio
n
Levoglucosane
C2H4O
Dati: Radlein D., Piskorz J. (1991)
Low Heating Rates
Antal M.J. et al.(1995-1998)
High Heating Rates
Milosavljievic I., Suuberg E.(1995)
46
250 300 350 400 450 500 550
0.2
0.4
0.6
0.8
1
Resi
duo
• Exp.Modello
1°C/min 80°C/min
10°C/min
250 300 350 400 450 500 550
0.2
0.4
0.6
0.8
1
Resi
duo
• Exp.Modello
1°C/min 80°C/min
10°C/min
600
• ExperimentalPrediction
250 300 350 400 450 500 550
0.2
0.4
0.6
0.8
1
Temperatura °C
Resi
duo
100°C/min
1000°C/min
• Exp.Modello
600
• ExperimentalPrediction
• ExperimentalPrediction
250 300 350 400 450 500 550
0.2
0.4
0.6
0.8
1
Temperatura °C
Resi
duo
100°C/min
1000°C/min
250 300 350 400 450 500 550
0.2
0.4
0.6
0.8
1
Temperatura °C
Resi
duo
100°C/min
1000°C/min
• Exp.Modello
Similar multistep kinetic models are alsodeveloped and validated for
hemicellulose and lignins.
Winter Combustion School Madras December 15, 2015
47Multistep Kinetic Model of Cellulose Pyrolysis
Ranzi, E., Cuoci, A., Faravelli, T., Frassoldati, A., Migliavacca, G., Pierucci, S., & Sommariva, S. (2008). Chemical kinetics of biomass pyrolysis. Energy & Fuels, 22(6), 4292-4300. Energy & Fuels, 2008, 4292-4300
The peculiarity of this pyrolysis scheme is the attempt to describe not only solid residue, but also a detailed
composition of released gas and tar species.
Winter Combustion School Madras December 15, 2015
48
Validation of Biomass Pyrolysis ModelComparisons with experimental TG data
Biomass devolatilization is then the combination of the pyrolysis of cellulose,
hemicellulose, and lignin
Winter Combustion School Madras December 15, 2015
From Biomass to Coal 49
The same approach is used for:
- Coal Characterization
- Multistep Kinetic Model of Coal Devolatilization
Winter Combustion School Madras December 15, 2015
50
Nine ‘Reference’ Coals wereselected in a narrow area
by Zhao et al. (1994)
Zhao, Y., Serio, M. A., Bassilakis, R., & Solomon, P. R. (1994). A method of predicting coal devolatilization behavior based on the elemental composition. ‘25th Symposium on Combustion’ 25(1): 553-560. Elsevier.Sommariva, S., Maffei, T., Migliavacca, G., Faravelli, T., & Ranzi, E. (2010). A predictive multi-step kinetic model of coaldevolatilization. Fuel, 89(2), 318-328.
Three reference coals are selected: COAL1 anthraciteCOAL2 bituminousCOAL3 lignite
Again, Elemental Analysis and C/H/O balances allow to define actual coal as a
mixture of three Reference Coals
Coal Characterization
Winter Combustion School Madras December 15, 2015
Characterization of the Solid Fuel
5 reference species
3 elemental balances (C, H, O)
3 reference mixtures
BIOMASS COAL
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
60 65 70 75 80 85 90 95 100Carbon (wt %)
Hydr
ogen
(wt%
)
Tomita
Solomon
Fletcher
IFRF
References
COAL3
COAL2
COAL1
CHAR
H
CHARc
COAL
Winter Combustion School Madras December 15, 2015
Multistep Kinetic Model of Coal Devolatilization 52
Sommariva, S., Maffei, T., Migliavacca, G., Faravelli, T., & Ranzi, E. (2010). A predictive multi-step kinetic model of coal devolatilization. Fuel, 89(2), 318-328.
A multistep kinetic model was alsodeveloped and validated for the three
reference coals.
Initially the coal forms a metaplastic phase, then, with different mechanisms at low and high temperatures, gas and tar species are released.
Winter Combustion School Madras December 15, 2015
53
Pittsburg TARS
0.00
0.10
0.20
0.30
0.40
0 10 20 30 40 50(min)
Wei
ght f
ract
ion
Pittsburg H2O
0.00
0.04
0.08
0.12
0 10 20 30 40 50(min)
Wei
ght f
ract
ion
Pittsburg CO2
0.00
0.01
0.02
0.03
0 10 20 30 40 50(min)
Wei
ght f
ract
ion
Pittsburg CO
0.00
0.01
0.02
0.03
0.04
0 10 20 30 40 50(min)
Wei
ght f
ract
ion
Pittsburg TAR
0.0E+00
2.0E-02
4.0E-02
6.0E-02
8.0E-02
1.0E-01
0 10 20 30 40 50(min)
Evol
utio
n ra
te (w
t/min
)
Pittsburg TG
0.40
0.60
0.80
1.00
0 10 20 30 40 50(min)
Wei
ght l
oss
300
600
900
1200
T (K)
Pittsburg C2H4
0.000
0.002
0.004
0.006
0 10 20 30 40 50(min)
Wei
ght f
ract
ion
Pittsburg H2O
0.0E+00
5.0E-03
1.0E-02
1.5E-02
0 10 20 30 40 50(min)
Evol
utio
n ra
te (w
t/min
)
Pittsburg CH4
0.00
0.02
0.04
0.06
0 10 20 30 40 50(min)
Wei
ght f
ract
ion
Pittsburg CO2
0.0E+00
1.0E-03
2.0E-03
3.0E-03
0 10 20 30 40 50(min)
Evol
utio
n ra
te (w
t/min
)
Pittsburg CO
0.0E+00
2.0E-03
4.0E-03
6.0E-03
8.0E-03
0 10 20 30 40 50(min)
Evol
utio
n ra
te (w
t/min
)
Pittsburg C2H4
0.0E+00
4.0E-04
8.0E-04
1.2E-03
0 10 20 30 40 50(min)
Evol
utio
n ra
te (w
t/min
)
Pittsburg CH4
0.0E+00
2.0E-03
4.0E-03
6.0E-03
8.0E-03
0 10 20 30 40 50(min)
Evol
utio
n ra
te (w
t/min
)
Extensive Validation of Coal Pyrolysis ModelTG Experiments of Solomon et al. (1990)
Solid residue, Tar , COx , H2O, CH4 , C2H4 and their evolution rates
Sommariva, S., Maffei, T., Migliavacca, G., Faravelli, T., & Ranzi, E. (2010). A predictive multi-step kinetic model of coal devolatilization. Fuel, 89(2), 318-328.
Winter Combustion School Madras December 15, 2015
56
https://www.google.it/url?sa=i&rct=j&q=&esrc=s&source=images&cd=&cad=rja&uact=8&ved=0ahUKEwij2q7G067JAhXHXhoKHR08B24QjRwIBw&url=http%3A%2F%2Fepthinktank.eu%2F2013%2F11%2F07%2Fplastic-waste%2Fplastics-production-plastic-waste-treatment-of-plastic-waste%2F&psig=AFQjCNHVE6nw8_4TJWLDrSwD97a0J6KNRw&ust=1448646520408459
Winter Combustion School Madras December 15, 2015
57
0
0.2
0.4
0.6
0.8
1
250 300 350 400 450 500 550 600
PS PP PE
Temperature °C
Resi
due
Pyrolysis of Plastic PolymersTG depolymerization of Poly-Styrene (PS), Poly-Propylene (PP), and Poly-Ethylene (PE)follows the Bond Dissociation Energies. Residual char is negligible.
PVC
Dehydrochlorination of Poly-Vinyl-Chloride (PVC) is the fastest step.The formation of (-CH=CH-)n is the reason for the successive residual char.Ranzi, E., Dente, M., Faravelli, T., Bozzano, G., Fabini, S., Nava, R., ... & Tognotti, L. (1997). Kinetic modeling of polyethylene and polypropylene thermal degradation. Journal of Analytical and Applied Pyrolysis, 40, 305-319.
Winter Combustion School Madras December 15, 2015
Elemental H/C/O Characterization of RDF
4
6
8
10
12
14
50 60 70 80 90% C [w/w]
% H
[w/w
]
RDF elemental composition
LigninCellulose
Plastics
H2O
240
4
6
8
10
12
14
50 60 70 80 90% C [w/w]
% H
[w/w
]
RDF elemental composition
LigninCellulose
Plastics
H2OH2O
240
RDF (on daf basis) are simply characterized in terms of Plastics, Cellulose and Lignin on the basis of H/C/O balances and heating value.
58
Sommariva, S., Grana, R., Maffei, T., Pierucci, S., & Ranzi, E. (2011). A kinetic approach to the mathematical model of fixed bed gasifiers. Computers & Chemical Engineering, 35(5), 928-935.
Winter Combustion School Madras December 15, 2015
59
Sommariva, S., Grana, R., Maffei, T., Pierucci, S., & Ranzi, E. (2011). A kinetic approach to the mathematical model of fixed bed gasifiers. Computers & Chemical Engineering, 35(5), 928-935.
Effect of Particle Size on RDF pyrolysis
Plastic content is higher in coarse particlesand it is responsible of the seconddevolatilization step at 400–500 ◦C.Ash and inert materials are moreabundant in fine particles.(Buah et al., 2007)
This dependence of RDF composition on the particle size was also observed in terms of different heating value by Skodras et al. (2008).
coarseparticles
(dp=1-35mm)
fineparticles
(dp<.5mm)
Winter Combustion School Madras December 15, 2015
Solid Fuels and Reference (Lumped) Species 60
The peculiarity of this approach is that all these schemes consist of a limited number ofdevolatilization reactions, which are able to describe not only the solid residue, but alsothe detailed composition of released gas and tar species.
A few lumped or reference species, togetherwith their pyrolysis models, allow to describe
the devolatilization process of the different fuels
The overall kinetic model of Solid Fuel Pyrolysis is simply the combination of the multistep kinetic models of Biomass , Plastics, and Coals.
Winter Combustion School Madras December 15, 2015
61
Importance of Secondary Gas-Phase Reactions
in Solid Fuel Pyrolysis Process.
Winter Combustion School Madras December 15, 2015
Transport Phenomena and Gas Phase Kinetics in Biomass Pyrolysis.
6262
The pyrolysys of biomasses occurs through the thermal degradation of solid cellular wall material to form an intermediate liquid (metaplast).
Subsequent high temperature decompositions generate volatile organic compounds (VOCs -Tar ) which exit the particle, through the wood pore (cellular lumen).
Gas-Phase Reactions need to be considered
Mettler et al., Energy Environ. Sci., 2012, 5, 7797
Winter Combustion School Madras December 15, 2015
M. S. Mettler, S. H. Mushrif, A. D. Paulsen, A. D. Javadekar, D. G. Vlachos and P. J. Dauenhauer ‘Revealing pyrolysis chemistry for biofuels production: Conversion of cellulose to furans and small oxygenates’ Energy Environ. Sci., 2012, 5, 5414-5424
The initial thermal decomposition of coal and biomass generates a short-lived liquid phase (metaplast). Further heating of the liquid intermediate produces tar/bio-oil species which can further react in the gas phase.
Multi-Component and Multi-Phase Nature of Coal and Biomass Pyrolysis Process.
Thousands of solid, liquid, gas-phase reactions are involved in
Coal and Biomass pyrolysis.
They deoxygenate and volatilize solid fuel to generate liquids and
gases.
It is then necessary to account for Gas-Phase Secondary ReactionsHeterogeneous Char reactions
63
Winter Combustion School Madras December 15, 2015
Secondary Gas Phase Reactions : PAH and Soot Formation in Coal Pyrolysis (Sarofim et al., 1987)
64
Mitra, A., Sarofim, A. F., & Bar-Ziv, E. (1987). The influence of coal type on the evolution of polycyclic aromatic hydrocarbons during coal devolatilization. Aerosol science and technology, 6(3), 261-271.
Similarly, it is necessary to account for the successive pyrolysis and oxidation reactions of all the volatiles
(gas and tar) released by the solid fuels.
Winter Combustion School Madras December 15, 2015
65
T.F. Lu, C.K. Law ‘Toward accommodating realistic fuel chemistry in large-scale computations’Progress in Energy and Combustion Science 35 (2009) 192–215
65
Methyl decanoateis a biomass fuel surrogate. Detailed kinetic mechanism consists of 3036 species and
8555 reactions.
Automatic Generation of kinetic mechanisms easily produces
Large Kinetic Models
Size of Gas-Phase Kinetic Mechanisms
POLIMISemi-detailedlumped
Winter Combustion School Madras December 15, 2015
66Gas Phase Reactions
Detailed Kinetics of Pyrolysis and Combustion(hundreds of species and thousands of reactions)
Hierarchy and Modularityare the main features of Detailed Kinetic Schemes
• GRI Kinetics for Gases
• PRF and additives for Gasolines
• Diesel and Jet Fuels
•Tar and Oxygenated Species• NOx
• PAH and Soot formation
CO-CO2
Ethers
CH4C2-C4
nC7-isoC8
H2 - O2
Heavy FuelsMe-Esters
Alcohols
Due to the hierarchical and modular structure of detailed kinetic schemes, the extension to new
tars or released species only requires the additionof their primary propagation reactions.
Winter Combustion School Madras December 15, 2015
67
Tran, L. S., Sirjean, B., Glaude, P. A., Fournet, R., & Battin-Leclerc, F. (2012). Progress in detailed kinetic modeling of the combustion of oxygenated components of biofuels. Energy, 43(1), 4-18.
Oxygenated components of biofuels
Winter Combustion School Madras December 15, 2015
68
Liu, D., Togbé, C., Tran, L. S., Felsmann, D., Oßwald, P., Nau, P., ... Battin-Leclerc,F. and Kohse-Höinghaus, K. (2014). Combustion chemistry and flame structure of furan group biofuels using molecular-beam mass spectrometry and gas chromatography, Combustion and flame,161(3), 748-765.
Decompositions of dihydrofuryl radicals(C4H5O-2 and C4H5O-3)
Winter Combustion School Madras December 15, 2015
Secondary Gas-Phase Reactions: 2,5-dimethylfuran Pyrolysis (Lifshitz et al., 1998)
69
Fi 5 Di h lf l i i 99 5% A 3 C i f
2,5-dimethylfuran pyrolysis in 99.5% Ar at 3 atm.
Lifshitz, A., Tamburu, C., Shashua, R., ‘Thermal Decomposition of 2,5-Dimethylfuran. Experimental Results and Computer Modeling’, J. Phys. Chem. A 102: 10655-10670 (1998)
Comparisons of model predictions and experimental data
Winter Combustion School Madras December 15, 2015
70Cellulose Pyrolysis Products (Norinaga et al. 2013)
Norinaga, K., Shoji, T., Kudo, S., & Hayashi, J. I. (2013). Detailed chemical kinetic modelling of vapour-phase cracking of multi-component molecular mixtures derived from the fast pyrolysis of cellulose. Fuel 103 (2013) 141–150.
Volatile released by cellulose pyrolysis
Winter Combustion School Madras December 15, 2015
71
Vapour-phase cracking of molecular mixtures derived from the fast pyrolysis of cellulose
Secondary Gas-Phase Reactionsof Cellulose Pyrolysis Products at 700-800 °C
Norinaga, K., Shoji, T., Kudo, S., & Hayashi, J. I. (2013). Detailed chemical kinetic modelling of vapour-phase cracking of multi-component molecular mixtures derived from the fast pyrolysis of cellulose. Fuel 103 (2013) 141–150.
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74
Heterogeneous Gas-Solid Reactions
Multi-Phase Model at the Particle Scale
Winter Combustion School Madras December 15, 2015
Heterogeneous Gas-Solid ReactionsMulti-Phase Model at the Particle Scale (Wen, 1968)
75
Particle Model consists of mass and energy balances for solid and gas phase
Wen, C. Y. (1968). Noncatalytic heterogeneous solid-fluid reaction models. Industrial & Engineering Chemistry, 60(9), 34-54.
Two asymptotic regimes are usually defined:a kinetic controlled regime for low temperatures and small particles
(Heat and Mass Transport are faster than Kinetics)a transport controlled regime for high temperatures and big particles
(Transport rates become lower than the kinetic rates)
Shrinking Model (unreacted core)General Model (reacting volume)
Winter Combustion School Madras December 15, 2015
76Particle Model 76
,,
,1, 1 , ,
, ,1
1 1 1 1, 1, , ,1 1
Sj i
j j i
j ij i j j i j j j i
NCPS Sj i p j i j NCP NCP
ij j j j j j i j i j j i j i j j
i i
dmV R
dtdm
J S J S V Rdt
d m c TJC S JC S S J h S J h V HR
dt
− −
=− − − − −
= =
= ⋅ = ⋅ − ⋅ + ⋅ = ⋅ − ⋅ + ⋅ − ⋅ + ⋅
∑∑ ∑
Particle Model consists of mass and energy balances
Rj,i is the net formation rate of ith species in the jth sector
Conduction Diffusion Reaction
The density distribution is the sum of the densities of different species in each particle sector.Similarly, the shrinking and porosity of each sector inside the particle is calculated.
Winter Combustion School Madras December 15, 2015
Thermally Thick Particles: Biot and Pyrolysis Numbers
Py Numbers decrease with increasing temperatures
Paulsen et al. Energy Fuels 2013, 27, 2126−2134
Biot relates conduction and convection times.
Pyrolysis Numbers relate thermal and kinetic times.
77
Winter Combustion School Madras December 15, 2015
78Pyrolysis of Thermally Thick Biomass Particle‘Exotic’ behavior of the center temperature profile
Wood sphere at 688 K.
dp=2.54 cm
Experimental center temperature overshoots the external temperature,due to the exothermic reactions of char formation
Park, W. C., Atreya, A. and Baum, H. R. (2010) 'Experimental and theoretical investigation of heat and mass transfer processes during wood pyrolysis', Combustion and Flame, 157(3), 481-494.
The flat Temperature plateau at ~650 K is due to endothermic tar devolatilization.
Comparisons of experimental and predicted (red lines) results.
Winter Combustion School Madras December 15, 2015
Pyrolysis of Thick Biomass Particle
Park, W. C., Atreya, A. and Baum, H. R. (2010) 'Experimental and theoretical investigation of heat and mass transfer processes during wood pyrolysis', Combustion and Flame, 157(3), 481-494.
The ‘endothermic’ release of tar component and ‘exothermic’ charification process are responsible
for this behavior of the temperature profiles
Comparisons of experimental and predicted (red lines) Center Temperature Profiles.
79
Winter Combustion School Madras December 15, 2015
Pyrolysis of Thick Biomass Particle:time-resolved gas phase composition (Bennadji et al., 2013)
80
648 K
*Acetic Acid (CH3COOH) and Hydroxy-Acetaldehyde (CH2OH-CHO) are lumped together
Bennadji, H., Smith, K., Shabangu, S., & Fisher, E. M. (2013). Low-temperature pyrolysis of woody biomass in the thermally thick regime. Energy & Fuels, 27(3), 1453-1459.
Secondary gas phase reactions are not important in these conditions.
Winter Combustion School Madras December 15, 2015
Secondary Gas-Pase Reactions at the
Elemental Reactor Scale
81
Reactor LayerReactor Layer
Gas Stream
The dynamic model of the ideal Gas-Solid Reactor accounts for the
exchanges and for kinetics both in the solid and the gas phase.
Fuel Particle
Particle Model consists of mass and heat balances
Secondary Gas-Phase Reactionstake place in the elemental reactor
Winter Combustion School Madras December 15, 2015
Elemental Reactor Model (Gas-phase) 82
Reactor LayerReactor Layer
Gas Stream
The dynamic Mass and Energy Balances of the Perfectly Stirred Reactor accounts for
Gas-Solid exchanges
Devolatilization Kinetics Heterogeneous Combustion/Gasification
Secondary Gas-Phase Reactions
, ,
, , , ,
1, , , ,
1 1 1
i
IN i OUT i
iIN i OUT i N i R g i
NCP
i p g NCP NCP NCPi
IN i g OUT i g N i N i N RAD gi i i
dg G G J V Rdt
d g C TG h G h J h JC J HR
dt
η
η η=
= = =
= − + + ⋅
= ⋅ − ⋅ + + + +
∑∑ ∑ ∑
ConvectionGas-Solid Exchange
RadiativeHeat Flux
ReactionHeat
η is the number of fuelparticles in the reactorvolume (VR)
Winter Combustion School Madras December 15, 2015
83
Without considering secondary gas-phase reactions, the model
overestimate the production of tars above
500 °C (dashed line)
Effect of Secondary Gas-Phase Reactions
Winter Combustion School Madras December 15, 2015
0%
20%
40%
60%
450 650 850 1050Temperature [°C]
Corbetta, M., Frassoldati, A., Bennadji, H., Smith, K., Serapiglia, M. J., Gauthier, G., Melkior, T., Ranzi, E., & Fisher, E. M. (2014). Pyrolysis of centimeter-scale woody biomass particles: kinetic modeling and experimental validation, Energy & Fuels.
Effect of Secondary Gas-Phase Reactions
BIO-OIL(TAR) GAS
RESIDUE
Without considering secondary gas-phase reactions, the model
overestimate the production of tars above
500 °C (dashed line)
84
Winter Combustion School Madras December 15, 2015
BIO OIL from Fast Pyrolysis of Biomass 85
Bridgwater, A. V. (2003). Renewable fuels and chemicals by thermal processing of biomass. Chemical Engineering Journal, 91(2), 87-102.Calonaci, M., Grana, R., Barker Hemings, E., Bozzano, G., Dente, M., & Ranzi, E. (2010). Comprehensive kinetic modeling study of bio-oilformation from fast pyrolysis of biomass. Energy & Fuels, 24(10), 5727-5734.
Optimal temperature for bio-oil production Reactor LayerReactor Layer
Gas Stream
Winter Combustion School Madras December 15, 2015
86
The heat needed for the pyrolysis is provided by the CHP plant fluidized-bed boiler by feeding hot sand to the CFB pyrolysis unit (800oC). Cold sand together with the char (at around 500oC) is send back to the fluidized-bed boiler, in which also the non-condensablesare fired. The combination allows lower investment costs when integrating into existing boilers
Winter Combustion School Madras December 15, 2015
Biomass Thermochemical Conversion Processes 87
European Biomass Industry Association http://www.eubia.org
Winter Combustion School Madras December 15, 2015
Gasification Regime of Thick Particles 88
A single reactor layer is fed with thick Fuel particles and Air at 300 K and a nominal Φ = 3.
Below a critical contact time there is a sudden shut down of the system.
Gasification regime requires high contact times to homogeneously heat
up the biomass particle.Volatiles form CO and H2.
At low contact time of solid particles a combustion regime
can prevail on gasification. Gas phase temperature rises,
while the center of the particle remains unreacted.
There is only a partial release of tar and volatiles, and the complete combustion to CO2
and H2O.
Winter Combustion School Madras December 15, 2015
Multi-Phase Model at Particle and Reactor Scale
89
Gas Stream
Grate
Gas Stream
Grate
Gas Stream
Grate
A fixed bed of solid particlesis considered as a cascade of several Elemental Reactors
Reactor LayerReactor Layer
Gas Stream
The dynamic model of the ideal Gas-Solid Reactor
accounts for the exchanges and for kinetics both in the solid and the gas phase.
Fuel Particle
Particle Model consists of mass (solid and gases) and
heat balances
Winter Combustion School Madras December 15, 2015
Gasifier is a Stack of Elemental Reactor Layers(counter-current and co-current configuration)
90
syngas
solid fuel
SteamAir/Oxidizer Ash
Fuel
ash
Syngas
Steam/Oxidizer
Top
Bottom
Temperature
Winter Combustion School Madras December 15, 2015
91
Fuel Particle
Reactor LayerReactor Layer
Gas Stream
Gas Stream
Solid Particles
Solid Particles
PARTICLE SCALE REACTOR LAYER SCALE
COUNTERCURRENT GASIFIER REACTOR SCALE
Multi-Scale Nature of Solid Fuel Gasifier
Winter Combustion School Madras December 15, 2015
92
15-30 solid phase species, 100-200 gas-phase components,
5-10 reactor layers, and 3-5 discretization sectors in the solid particle.
Several Thousands of Balance Equations
The resulting Stiff System of Differential Algebraic Equations (DAE) is solved by using the BZZMATH Library.
The Jacobian matrix is structured in Sparse Diagonal Blocks.
Mathematical Model of the Counter-Current Gasifier
Buzzi-Ferraris, G. (1993). Scientific C++; Building Numerical Libraries the Object-Oriented Way. Addison-Wesley Longman Publishing Co., Inc..Buzzi-Ferraris, G., & Manenti, F. (2010). Fundamentals and linear algebra for the chemical engineer: Solving numerical problems. Wiley-vch.
Winter Combustion School Madras December 15, 2015
93
Solid speciesGas-solid
interactions
Sector 1
Sector N
Migration of gas species
Layer 1
Layer NR
Migration of gas species
PARTICLE SCALE REACTOR LAYER SCALE REACTOR SCALECOUNTERCURRENT GASIFIER
∼30 elements
∼100 elements
∼30 elements
Solid species (NCS)
Gas-solid interactions
(NCg)
∼30 elements
∼30 elements
Gas-phase species(NCG)
Solid Fuel GasifierBlock Sparse Structure of the Jacobian
External Sector
Internal Sector
Winter Combustion School Madras December 15, 2015
95Counter-Current Coal Gasifier
Empirical correlations are required to account for the morphological changes of the coal particles and the fixed bed.
Shrinking and swelling, porosity and density, diffusivity….
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96
2D Models: Anisotropic particles
Comminution of fuel particleduring conversion
Gómez-Barea, A., & Leckner, B. (2010). Modeling of biomass gasification in fluidized bed. Progress in Energy and Combustion Science, 36(4), 444-509.
Anisotropy and Morphological Changes
Winter Combustion School Madras December 15, 2015
300 800 1300 1800Temperature [K]
solid
gas
exp
Leucite Sub-bitum.
Validation of the Coal Gasifier Model
AIR
/H2O
SYN
GAS
FUEL
RESID
UE
PYROLYSIS
GASIFICATION
CHAR COMBUSTION
DRYING
ASH ZONE
Grieco, E. M., & Baldi, G. (2011). Predictive model for countercurrent coal gasifiers. Chem. Eng. Sci., 66(23), 5749-5761.
C78%
H5%
O14%
N2%
S1%
Leucite Sub-bitum.
Moisture 17.4 %
F = 0.1 kg/s/m^2
F = 0.25 kg/s/m^2xO2 = 16.5 %xN2 = 63 %xH2O = 20.5 %
Steady-stateTemperature
Profiles
Steady-stateSyngas
Composition
98
Winter Combustion School Madras December 15, 2015
99Simplified Structureof a Travelling Grate Combustor
Winter Combustion School Madras December 15, 2015
100
The biomass bed on the grate is assumed as several stacks of elemental reactor layers.
The grate movement determines the effective contact times of the biomass on the grate.
The steady problem is thus transformedinto a dynamic problem of a travelling ‘Slice’ of the fuel bed.
Steady and Dynamic Problem
Winter Combustion School Madras December 15, 2015
101
Decomposition and CombustionReactions in the Freeboard
Integral closure of mass and energy balances :Pyrolysis products with primary and secondary air are involved in gas-phase reactions.Flue gases heat up the radiating walls of the furnace.
Travelling Grate Biomass Combustor
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102
Top LayerIgnition
CharCombustion
Front
E. Ranzi, S. Pierucci, P. C. Aliprandi, S. Stringa (2011)‘Comprehensive and detailed kinetic model of a traveling grate combustor of biomass’ Energy & Fuels 25:4195 - 4205
Detailed predictions of Temperatures and Reactivityinside the Travelling Grate Combustor.
Winter Combustion School Madras December 15, 2015
103Detailed simulations allow to derive a Control Model of the Travelling Grate Combustor.
E. Ranzi, S. Pierucci, P. C. Aliprandi, S. Stringa (2011)‘Comprehensive and detailed kinetic model of a traveling grate combustor of biomass’ Energy & Fuels 25:4195 - 4205
0
1
2
3
4
13 14.75 16.5 18.25 20
Posi
tion
on th
e tr
avel
ing
grat
e [m
]
Grate velocity [m/h]
Ignition
Combustion front
0
1
2
3
4
0.12 0.14 0.16 0.18
Posi
tion
on th
e tr
avel
ing
grat
e [m
]
Bed thickness [m]
Ignition
Combustion front
Grate velocity and bed thicknesseffect on ignition and combustion front.
Similarly, the effect of Biomass Composition, Fuel Size, Radiating Temperature, Primary and Secondary Air Flowrate
is investigated.
Winter Combustion School Madras December 15, 2015
104Control Model of the Travelling Grate Combustor.(12 MW biomass combustor operating in Belgium)
Summary of operating conditions, biomass characteristics, and model predictions.
E. Ranzi, S. Pierucci, P. C. Aliprandi, S. Stringa (2011)‘Comprehensive and detailed kinetic model of a traveling grate combustor of biomass’ Energy & Fuels 25:4195 - 4205
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105
• Solid fuel pyrolysis and combustion processes are intrinsically more difficultto describe than gas-phase processes on a fundamental mechanistic leveland present major challenges to combustion scientists.
• The morphological changes during fuel conversion require to account forcontinuous modifications of physical and transport properties.
• For this reason, lumping procedures need to be applied at different levels.• Once lumped models are available, it is always feasible and useful to increase
the description level and to improve model predictions
• For several solid fuels, the simple knowledge of the C/H/O content issufficient to understand their pyrolysis and combustion behavior.
• Of course, the catalytic effect of ashes is only one of the further complicatingaspects of this problem
Conclusion
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106
CRECK Modeling Group at Politecnico di Milano
Thanks for the attention