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    Modeling the Gasification Based Biomass

    Co-firing in a 600MW Pulverized Coal BoilerDalong Jiang, Changqing Dong*, RuiYang, Junjiao Zhang, and Yongping Yang

    Abstract--Gasification based biomass co-firing was an

    attractive technology for utilizing biomass as an additional

    fuel in utility boilers. Compared to directly co-firing biomass

    and coal, it showed following benefits: (1) avoiding biomass

    delivery into the boiler, (2) reduced boiler slagging, (3)

    avoiding altered ash characteristics. In co-firing

    demonstration project, higher percentage of biomass gas for

    co-firing was expected. But the effect of percentage of biomass

    gas on combustion efficiency, boiler efficiency and pollutant

    emission was not clear. In the study, numerical simulation of

    co-firing producer gas from biomass gasification and coal in a

    600MWe tangential PC boiler was carried out with CFD

    method. Combustion behavior and pollutant emission for the

    coal fired only case and six co-firing cases were compared.

    The results showed that The effect of co-firing on combustion

    efficiency was slight, the reduction of NOx emission can be

    achieved. The NO removal rate was between 45% and 71%.

    In addition, slagging can be reduced for the temperature

    decreasing. And the convection heat transfer area should be

    increased or the biomass gas should be limited to a low

    percentage to achieve higher boiler efficiency.

    Key words--biomass gas, co-firing, nitrogen monoxide

    I.NOMENCLATURE

    Symbol Meaning expression

    Gk

    the generation of turbulence kinetic energy due to the mean

    velocity gradients

    Gb

    the generation of turbulence kinetic energy due to buoyancy

    YM

    the contribution of the fluctuating dilatation in compressible

    turbulence to the overall dissipation rate

    This work was supported by the National Basic Research Program

    (2009CB219900), and the National High Technology Research and

    Development of China (2008AA05Z302).

    D.L. Jiang, C.Q. Dong*, R. Yang, J.J. Zhang, and Y.P. Yang are all with

    the National Engineering Laboratory of Biomass Power Generation

    Equipment, Key Laboratory of Condition Monitoring and Control for

    Power Plant Equipment, Ministry of Education, North China Electric

    Power University, China, 102206 (*Corresponding author:

    [email protected]).

    1C constant=1.44

    2C constant=1.92

    3C constant=0.09

    k turbulent Prandtl numbers for k

    turbulent Prandtl numbers for

    Sk

    user-defined source term

    S user-defined source term

    ( )m tv

    volatile yield up to time t

    ,0m

    p initial particle mass at injection

    1 ,

    2 yield factors

    ma

    ash content in the particle

    H the total height of the boiler

    z the ratio of the actual elevation to the total height of the boiler

    II.INTRODUCTION

    Biomass co-firing, the practice of supplementing a base

    fuel with biomass fuels which include wood waste, short

    rotation woody crops, short rotation herbaceous crops (e.g.,

    switchgrass), alfalfa stems, various types of manure,

    landfill gas and wastewater treatment gas, began in the

    1980s, and become the normal power generation

    technology in Europe and the United States.

    With minimum modifications to the existing boiler

    systems, co-firing was generally viewed as the most cost

    effective approach to biomass utilization by the electric

    utility industry. It was a family of technologies [1]. These

    included: (1) blending biomass with coal on the fuel pile,

    then pulverizing and injecting the mixture into the boiler,

    (2) preparing the biomass separately from coal, and

    injecting it into the boiler without impacting the

    conventional coal delivery system, (3) feeding the biomass

    into the gasifier to generate producer gas, and injecting the

    biomass gas into the boiler through the gas burner.

    Reviews of co-firing experiences identified over 100

    successful field demonstrations in 16 countries that used

    essentially major type of biomass (herbaceous, woody,

    animal waste, anthropomorphic wastes) combined with

    essentially every rank of coal and combusted in major type

    of boiler (tangential, wall, and cyclone fired) [2,3]. The

    technical evaluations showed the potential project

    benefits:(1) reduced fossil CO2 emissions, (2)reduced other

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    airborne emissions including NOx, SO2 and trace

    metals,(3)potential for reduced fuel cost,(4) supporting

    economic development among wood products and

    agricultural industries in a given service area. So co-firing

    was a low-cost, low-risk, environment friendly technology

    to biomass utilization by the electric utility industry.

    However, while biomass was directly co-fired with coal,

    some technical challenges appeared, including [4]:

    Limited percentage of biomass for co-firing (e.g.

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    B. Mathematical Models

    The combustion in the furnace was a very complicated

    process that included gas turbulent flow, turbulent

    combustion, particle movement, volatile devolatilization,

    particle combustion, radioactive heat transfer, and these

    interacted. In the paper, standard k was selected for

    simulating the gas turbulent flow field. The turbulence

    kinetic energy kand its rate of dissipationwere obtained

    from the following transport equations[6]:

    ( ) ( ) [( ) ]ti k b M k i j k j

    kk ku G G Y S

    t x x x

    + = + + + +

    (1)

    2

    1 3 2( ) ( ) [( ) ] ( )t

    i k b

    i j j

    u C G C G C S t x x x k k

    + = + + + +

    (2)

    / /uj

    G u uk i j u

    i

    =

    Pr

    ttG gb i x

    t i

    =

    2kC

    t

    = (3)

    22Y Mt

    =2

    kM

    ta

    = (4)

    Two mixture fraction/PDF (Probability Density Function)

    was selected as the gas turbulent combustion model. The

    PDF modeling approach involves the solution of transport

    equations for one or two conserved scalars (the mixture

    fractions). Equations for individual species are not solved.

    Instead, species concentrations are derived from the

    predicted mixture fraction fields. The thermo-chemistry

    calculations are preprocessed in prePDF and tabulated for

    look-up in FLUENT. Interaction of turbulence and

    chemistry is accounted for with a probability density

    function.

    *

    sec( , , )

    i i fuel f p H =

    *

    sec( , , )

    i i fuel f p H =

    / 2 / 2 *

    s ec s ec, , , ,fuel fuelf p p H

    i

    *

    sec( , , )i i fuel f p H =

    1( )

    fuelp f

    2 sec( )p p

    Fig.3. Computational tasks between FLUENT and prePDF for a

    Two-Mixture-Fraction case

    The dispersion of particles due to turbulence in the fluid

    phase was predicted using the stochastic tracking model.

    The two competing rates Kobayashi model was selected as

    the devolatilization model. The kinetic devolatilization rate

    expressions of the form proposed by Kobayashi:

    1( )

    1 1PE RTR A e

    = (5)

    2( )

    2 2PE RTR A e= (6)

    Where1

    R and2

    R are competing rates that may

    control the devolatilization over different temperature

    ranges. The two kinetic rates are weighted to yield an

    expression for the devolatilization as:

    1 1 2 2 1 20 0

    ,0 ,0

    ( )( )exp( ( ) )

    (1 )

    t tv

    w p a

    m tR R R R dt dt

    f m m = + +

    (7)

    The Kobayashi model requires input of the kinetic rate

    parameters1

    A ,1

    E ,2

    A ,2

    E ,1

    ,2

    . These parameters

    recommended by the literature [7] were used.

    The Kinetic/Diffusion surface reaction rate model was

    selected as the surface combustion model and the P1 as the

    radioactive heat transfer model. Segregated solution

    method was used and the standard pressure scheme was

    chosen. First-Order Upwind Scheme was used in the

    discretization of governing equations and simple algorithm

    for pressure-velocity coupling [8].

    IV.SIMULATIONRESULTSANDDISCUSSION

    Seven cases including coal fired only and six producer

    gas co-firing cases were calculated with Fluent software

    package. For co-firing cases, the percentage of biomass gas

    was 3%, 5%, 8%, 10%, 15%, 50% separately. The velocity

    vector, coal particles mass, temperature, the concentration

    of CO, CO2, O2 and NO emissions in seven conditions

    were compared. The excess air ratio at the outlet of furnace

    was kept as 1.125. The initial parameters were showed in

    table IV. The heat transfer area above the furnace arch was

    not considered.

    Fig 4 Velocity vectors distribution in the first layer of primary air injection

    Fig.5. Velocity vectors distribution in the fourth layer of primary air

    injection

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    TABLE IV

    THE MAIN INLET PARAMETERS OF THE SEVEN CASES

    Parameters Coal combustion 3% co-firing5%

    co-firing8% co-firing 10% co-firing 15% co-firing 50% co-firing

    The layer of the coal

    burner

    123456

    7

    1234

    567

    1234

    567

    1234

    567

    1234

    567

    1234

    567

    1234

    567

    The layer of the biomass

    gas burner/ 1 1 1 1 1 1234

    Coal quantity(t/h) 419 406.43 398.05 385.48 377.1 356.15 209.5

    The flow rate of

    biomass(m3/s)/ 9.18 15.3 24.48 30.6 45.92 153.01

    Outlet velocity of

    biomass gas(m/s)/ 10.67 17.79 28.46 35.58 26.69 25.41

    Outlet velocity of primary

    air(m/s)23.73 23.73 23.73 23.73 23.73 23.73 23.73

    Outlet velocity of

    secondary air(m/s)

    54.712345

    6

    69.6154.723

    456

    65.97154.723

    456

    60.09154.7234

    56

    56.16154.7234

    56

    67.47154.7234

    56

    71.1612354.74

    56

    Outlet velocity of

    OFA(m/s)45.44 45.44 45.44 45.44 45.44 45.44 45.44

    (In the option of outlet velocity of secondary air, the number in the bracket represented the layer of the secondary air)

    Figure 4, 5 showed the velocity vector distribution in the

    first and the fourth layer of primary air injection. Four jet

    streams interacted and formed good corner tangential firing.

    This suggested that the aerodynamic field was proper and

    the air distribution mode meet the demand of corner

    tangential firing. The diameter of the tangential circle did

    not changed in all cases, which suggested that co-firing did

    not impact the field in the furnace.

    Fig.6. The mass history of the coal particles

    Figure 6 showed the particle traces colored by particle

    mass. For co-firing 3%,5%,8%,10%,15% biomass gas and

    coal combustion case, some particles fell into the cold ash

    hopper under gravity action, which caused solid

    incomplete combustion heat loss. However, most particles

    moved upward with flow gas and burned out. When

    co-firing 50% biomass gas, pulverized coal was injected

    from the upper layer of burners, no particle fell into the

    cold ash hopper.

    0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8

    800

    1000

    1200

    1400

    1600

    1800

    2000

    T/K

    z/H

    coal combustion

    3% co-firing

    5% co-firing

    8% co-firing

    10% co-firing

    15% co-firing

    50% co-firing

    Fig 7 Mean temperature distribution along with the height of the furnace

    The mean temperature distribution along the height of

    furnace was similar for the seven cases as showed in Fig 7.

    There were two peak temperatures which were

    representing the burner region and the area in the upper

    reaches of OFA injection. For the co-firing cases, the mean

    temperature was lower than that of the coal combustion,

    and decreased with the percentage of the biomass gas

    increased. The gas volume was higher for co-firing cases

    than that of the coal fired only case, thus, the temperature

    thereupon decreased. When the percentage of biomass gas

    increased to 50% the temperature of outlet flue gas

    decreased by 300K.

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    0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8

    0

    1

    2

    3

    4

    5

    6

    7

    CO/mo

    lefraction

    z/H

    coal combustion

    3% co-firing

    5% co-firing

    8% co-firing

    10% co-firing

    15% co-firing

    50% co-firing

    a

    b

    cd

    Fig 8 Mean CO concentration distribution along with the height of

    furnace

    The mean CO concentration was similar for all the cases.

    There are two maximum and two minimum which were

    marked by a, b, c and d in figure 9. a and b

    were present to near the first and the fifth layer of burner

    separately. c was present to the space between the first

    group burner and second group burner. With the feeding of

    the over-fire air, the second minimum d appeared. For

    co-firing cases, the CO level decrease with the increasing

    proportion of the biomass gas. When the percentage of

    biomass gas was increased to 50%, the CO level was lower

    than that of coal combustion case.

    0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8

    13

    14

    15

    16

    17

    18

    CO2/molefraction

    z/H

    coal combustion

    3% co-firing

    5% co-firing

    8% co-firing

    10% co-firing

    15% co-firing

    50% co-firing

    Figure 9 Mean CO2 concentration distribution along with the height of

    furnace

    Figure 9 presented the CO2 level. The peak value was

    nearby the space between the first group burner and second

    group burner. The CO2 level decrease for the co-firing

    cases but the difference of the outlet value was not

    significant. Figure 10 presented the O2 concentration. The

    trends were similar and two peak values were present to

    the burner area and the OFA injection area separately. The

    0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8

    -0.5

    0.0

    0.5

    1.0

    1.5

    2.0

    2.5

    3.0

    3.5

    4.0

    O2/molefraction

    z/H

    coal combustion

    3Data1_Co-firing

    5% co-firing

    8% co-firing

    10% co-firing

    15% co-firing

    50% co-firing

    Figure 10 Mean O2 concentration distribution along with the height

    of furnace

    0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8

    0

    00

    00

    00

    00

    z/H

    coal combustion3% co-firing5% co-firing8% co-firing10% co-firing

    15% co-firing50% co-firing

    Figure 11 Mean NO concentration distribution along with the height

    of furnace

    O2 level increased with the increasing proportion of the

    biomass gas. Figure 11 presented the effect of the co-firing

    on NO emission. There are two peak values, one was

    present to the burner area, and the other was present to the

    OFA injection area. Table V showed NO emission at outlet

    and NO removal rate of co-firing. The NO removal rates

    were between 45% and 71% for co-firing cases. As

    compared to coal, producer gas was characterized by low

    nitrogen content and can reduce the NO formation, thus,

    the NO level decreased dramatically when co-firing.

    TABLE V

    THE NO EMISSION AT OUTLET AND NO REMOVAL RATE OF

    CO-FIRING

    ConditionOutlet NO mole

    fraction/ppm

    Removal rate of

    NO/%

    Coal combustion 149.697 /

    3% Co-firing 82.246 45%

    5% Co-firing 60.707 59%

    8% Co-firing 60.065 60%

    10% Co-firing 51.792 65%

    15% Co-firing 50.631 66%

    50% Co-firing 44.138 71%

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    For all the co-firing cases, the CO, CO2 and O2

    concentration distributions were similar to that of the coal

    fired only case. The differences of the outlet values of these

    parameters were slight. Aerodynamic field was proper and

    coal particles burned completely in all cases. The

    temperature level was lower when co-firing, this can relief

    the slagging problem. These analyses showed that the

    effect of co-firing on combustion efficiency was slight. The

    NO emission was reduced when co-firing.

    V.CONCLUSIONS

    In this study, 3%, 5%, 8%, 10% 15%, 50% by heat basis

    producer gas from biomass gasification was co-fired with

    coal in the 600MW tangential PC boiler. The results

    showed that:

    NO emission decreased with the percentage of the

    biomass gas increased. The removal rate was between

    45% and 71%.

    The effect of co-firing on combustion efficiency was

    slight. The flue gas temperature was lower and the

    flue gas quantity was higher when co-firing, and

    decreased with the percentage of the biomass gas

    increased. The convection heat transfer area should be

    increased or the biomass gas should be limited to a

    low percentage to achieve higher boiler efficiency.

    The slagging can be reduced for lower co-firing

    temperature.

    VI.REFERENCES

    [1]D.A.Tillman, Biomass co-firing: the technology, the experience, the

    combustion consequences, Biomass and Bioenergy , 2000,19: 365-384.

    [2] Baxter L., Biomass co-firing overview, Second world conference

    and exhibition on biomass for energy, industry and climate protection.

    Rome, Italy, 2004.

    [3] Koppejan J., Introduction and overview of technologies applied

    worldwide, Second world conference and exhibition on biomass for

    energy, industry and climate protection. Rome, Italy, 2004.

    [4] Larry Baxter, Biomass-coal co-combustion: opportunity for

    affordable renewable energy, Fuel, 2005, 84: 1295-1302.

    [5] Magn Lapuerta, Juan J. Hernndez, Amparo Pazo, et al., Gasification

    and co-gasification of biomass wastes: Effect of the biomass origin and

    the gasifier operating conditions, Fuel processing technology. 2008,

    89(9): 828-837.

    [6] Fujun Wang, Computational Fluid Dynamic Analysis: Principle and

    Application of CFD Software, Beijing, China, 2004.120-123.

    [7] Luis I. Dez, Cristbal Corts, Javier Pallars, et al., Numerical

    investigation of NOx emissions from a tangentially-fired utility boiler

    under conventional and overfire air operation, 2007, 87(7):1259-1269.

    [8] Ryan Zarnitz, Sarma V. Pisupati, Evaluation of the use of coal

    volatiles as reburning fuel for NOx reduction, Fuel, 2007, 86(4):

    554-559.

    VII.BIOGRAPHIES

    Dalong Jiang was majoring PH.D. program

    in North China Electric Power University. He was

    the chairman of Dragon Power Corp.( China). His

    special fields of interest are the clean utilization of

    Biomass energy.

    Rui Yang was born in Shaanxi province in

    china on November 30, 1983. She is studying at

    North China Electric Power University. Her

    special fields of interest are efficient and clean

    utilization of biomass.