413 topic iv-3 (fossil fuels and boiler efficiency)

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    ISAT 413 - Module IV:

    Combustion and Power Generation

    Topic 3: Fossil Fuels and Boiler Efficiency

    Fossil Fuels

    Fluid-Moving SystemsCombustion Methods and Systems

    Steam Generators

    Boiler Types and Classifications

    Primary Boiler Heat-Transfer Surfaces

    Secondary Boiler Heat-Transfer Surfaces

    Boiler Ratings and Performance

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    2

    Fossil Fuels

    The three general classes of fossil fuels are coal, oil,

    and natural gas.

    Hydrocarbon Chemistry

    There are three major groups of hydrocarboncompounds the aliphatic hydrocarbons, the alicyclic

    hydrocarbons, and the aromatic hydrocarbons.

    The aliphatic or chain hydrocarbons are further

    divided into three subgroups the alkane, the alkene,and the alkyne hydrocarbons.

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    The alkanehydrocarbons, also called paraff in series,

    are the saturated group of chain hydrocarbons. The

    general chemical formula for this group is CnH2n+2. suchas Methane (CH4), Ethane (C2H6), Propane (C3H8), Butane

    (C4H10), Pentane (C5H12), Hexane (C6H14), Heptane

    (C7H16), Octane (C8H18), Nonane (C9H20), Decane (C10H22),

    etc. As the number of atoms in the alkane molecules

    increase, the hydrogen fraction decreases and thehydrocarbons become less volatile. Figure below shows

    the chemical structure of n-Octane.

    HC

    H

    H

    C

    H

    H

    C

    H

    H

    C

    H

    H

    C

    H

    H

    C

    H

    H

    C

    H

    H

    C

    H

    H

    H

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    The alkenehydrocarbons, also called olef in series,

    have one double bond between two of the carbon atoms

    in the chain. The general formula for this group is CnH2n,

    and some of the typical compounds are ethylene (C2H4),propylene (C3H6) (left), butene (C4H8), pentene (C5H10),

    and hexene (C6H12).

    HC

    H

    H

    C

    H

    H

    C

    H

    The alkynehydrocarbons, also called acetylene series,

    have one triple bond in the hydrocarbon chain. Thegeneral formula for this group is CnH2(n-1), and some of

    the typical compounds are acetylene (C2H2), and

    ethylacetylene (C4H6) (r ight).

    HC

    H

    H

    CH C C

    H

    H

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    The alicyclichydrocarbons are composed of saturated

    carbon-atom rings and have a general formula that is

    identical to that of the alkene subgroup of aliphatic

    hydrocarbons, i.e., CnH2n, some of the typicalcompounds are cyclopropane (C3H6), cyclobutane (C4H8),

    (top), and cyclopentane (C5H10).

    The aromatichydrocarbons are

    composed of the basic benzenering or rings. The ring is a six-atom

    carbon ring with double bonds

    between every other carbon atom.

    The general formula for this groupis CnH2n-6, some of the typical

    compounds are benzene (C6H6)

    (bot tom), toluene (C7H8), xylene

    (C8H10), and naphthalene (C10H8).

    HC

    H

    H

    C

    H

    H

    HC C

    H

    H

    HC

    H

    H

    C

    HC C

    H

    H

    C

    C

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    Standard Fuels

    The 100-octane fuel standard for in ternal-combust ion-

    engineis 2,2,4-trimethylpentane, C8H18(isooctane),while 0-octane fuel standard is n-heptane, C7H16. The

    unknown fuel is burned in the engine and the

    compression ratio is slowly increased until a certain

    knock or detonation reading is obtained from a

    vibration detector. The octane ratings of most regulargasolines range from 85 to 95.

    The 100-cetane fuel standard for compression- ign i t ion

    ordiesel fuelsis n-hexadecane (C16H34), while 0-cetane

    fuel standard is alpha-methylnaphthalene (C11H10). Thecetane ratings of most diesel fuels range between 30

    and 60.

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    Coal

    American Society for Testing Materials (ASTM) has

    developed a method that ranks coal into four

    classifications:

    Class I coals: Anthracitic coals, the oldest.

    Class II coals: Bituminous coals.

    Class III coals: Subbituminous coals.Class IV coals: Lignitic coals.

    Coal Analyses

    The two common coal analyses are the proximateanalysis and the ul t imate analysis.

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    Proximate Analysis

    The prox imate analysisis the simplest coal analysis

    and gives the mass fractions of f ixed carbon(FC),

    vo lat ile matter(VM), ash(A ), and moisture (M) in the

    coal.

    This analysis can be determined by simply weighing,

    heating, and burning a small sample of powdered coal.

    The coal sample is carefully weighed and then heatedto 110oC for 20 min. The sample is then weighed again

    and the mass loss is divided by the original mass to

    obtain the moistu re fract ion.

    The remaining sample is heated to 954oC in a closedcontainer for 7 min. The sample is then reweighed and

    the resulting mass loss in this heating process is

    divided by the original mass to obtain the fraction of

    thevo lat ile matter

    in the sample.

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    The sample is then heated to 732oC in an open crucible

    until it is completely burned. The residue is then

    weighed and the final weight is divided by the original

    weight to obtain the ash fract ion.

    The mass fraction of f ixed carbonis obtained by

    subtracting the moisture, volatile matter, and ash

    fractions from unity.

    In addition to the FC, VM, M, and A, most proximateanalyses list separately the su l fur mass fract ion(S)

    and the higher heat ing value(HHV) of the coal.

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    Ultimate Analysis

    The ult im ate coal analys isis a laboratory analysis that

    lists the mass fractions of carbon, C, hydrogen (H2

    ),

    oxygen (O2), nitrogen (N2), and sulfur (S) in the coal

    along with the higher heating value.

    Most ultimate analyses include the moisture and ash

    separately, but some analyses include the moisture as

    part of the hydrogen and oxygen mass fractions.

    The ultimate analysis is required to determine the

    combustion-air requirements for a given combustion

    system and this, in turn, is used to size the draft

    system for the furnace.These calculations should be based on the as-burned,

    ultimate coal analysis, if possible.

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    Coal Properties

    There are a number of properties that should be

    considered when selecting a coal for a given application.

    Among these are its sulfur content, its burning

    characteristics, its weatherability, its ash-softening

    temperature, its grindability index, and its energy

    content.

    It is desirable to use a coal with a low sul fur con tent.

    If the coal i s bu rnedin a stationary bed with little

    agitation, the coal should be a free-burning coal, not a

    caking coal; caking coals must be mechanically agitated

    when they are burned to break up the fused-coal masses.The weatherabil i ty of a coal is a measure of its ability

    to withstand exposure to atmospheric conditions without

    excessive crumbling.

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    The gr indabi l i ty index is another important property

    that should be considered when selecting a coal. This is

    particularly true for the common pulverized-coal power

    system where the coal is ground up finer than facepowder.

    The ash-so ftening temperatureis an important

    consideration in the choice of coals for a particular

    power plant. The ash-softening temperature is thetemperature where the ash becomes very plastic,

    somewhat below the melting point of the ash. Slagging

    occurs as ash deposits build up on the heat-transfer

    surfaces.The energy content or heating valueof a coal is a very

    important property. The heating value represents the

    amount of chemical energy in a given mass or volume of

    fuel. HHV = LHV + hfg,fuel

    .

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    Petroleum

    Although crud e oi lis a composition of many organic

    compounds, the ultimate analyses of all crude oils are

    fairly constant. The carbon mass fraction ranges from 84to 87%, the hydrogen mass fraction ranges from 11 to

    16%, the sum of oxygen and nitrogen mass fractions

    range from 0 to 7%, and the sulfur mass fraction ranges

    from 0 to 4%.There are six grades of commercial fuel oil. No. 1 is the

    lightest, least viscous, for vaporizing burners. No. 2 is a

    distillate oil and is the general-purpose domestic heating

    oil. No. 3 is no longer available. No. 4 is a relatively lightheating oil. No. 5 is a heavy, viscous, commercial-grade

    heating oil, and No. 6, or bunker-C oil, is the heaviest

    and most viscous of the residual fuel oils. Both Nos. 5

    and 6 oils require heating before they can be pumped.

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    Petroleum Properties

    The important properties of petroleum and petroleum

    products are the heating value, the specific gravity, the

    flash point, and the pour point.

    The speci f ic gravi ty,s,of any liquid is the density of

    that liquid divided by the density of water at 15.6oC.

    The f lash pointof a liquid fuel is the minimum fluid

    temperature at which the vapors coming from a free

    surface of the liquid will just ignite, producing a flash.

    The pour po in tof a liquid fuel is the lowest fluid

    temperature at which an oil or oil product will flow under

    standard conditions.

    The combustion of crude-oil products has some ash,

    sulfur, and vanadium oxidizes (V2O5) problems. They are

    expensive to remove.

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    Gaseous Fuels

    Almost all gaseous fuelsare either fossil fuels or

    byproducts of fossil fuels. These fuels can be divided

    into three general groups including natural gases,manu factured fuel gases, and byp rodu ct fuel gases.

    The composition of a fuel gasis commonly expressed in

    terms of the moleor vo lumefractions of the chemical

    compounds found in it.The heating value of any fuel gas is commonly expressed

    in units of energy per uni t vo lume(kJ/m3) but this value

    is directly proportional to the gas density, which in turn is

    directly proportional to the absolute pressure andinversely proportional to the absolute temperature.

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    Gaseous Fuels Heating Values

    T

    T

    P

    P r

    rrT,rPvT,Pv

    HHVHHV

    If the volumetric heating values of the gas components at

    some reference pressure Pr

    and reference temperature Tr

    are known, the volumetric heating vale of the gas

    mixture, HHVvis obtained from the following equation:

    Where (HHVv)iand Viare the volumetric high heating

    value and the volumetric fraction of thei thgaseous

    component, respectively. The following equation can be

    used to convert the volumetric higher heating value atthe reference pressure and temperature to some other

    pressure and temperature:

    irT,rP,i

    ni

    ivrT,rPv

    VHHV

    1

    mixtureofHHV

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    P

    T

    MW

    R

    P

    RT

    m

    V

    v u

    A volumetric heating value HHVvat some temperature T

    and pressure Pcan be converted into a gravimetric

    heating value HHVmby multiplying the volumetric value

    by the specific volume vof the gas at the same pressureand temperature:

    The specific volume of a gas mixture can be determinedfrom the molecular weight (MW) of the gas and the ideal-

    gas equation of state, as follows:

    T,PT,Pvm vHHVHHV

    where Ruis the universal gas constant.

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    Example IV-3.1

    Calculate the higher heating value, in kJ/m3and kJ/kg,

    at 10oC and 3 atm for gas mixture with the following

    composition: 94.3% CH4, 4.2% C2H6, and 1.5% CO2.

    3

    3

    3

    3

    6453700150910640420030379430

    0521701440150071300420043169430

    0

    91064

    03037

    m

    kJ,.,.,.

    C

    kmol/kg.......

    m/kJ

    m/kJ,

    m/kJ,

    :Solution

    mixturev

    v

    v

    v

    HHV

    :atm1and20At

    MW

    COforHHV

    HCforHHV

    CHforHHV

    :atm1andC20At

    o

    2

    62

    4

    o

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    kg

    kJ,

    kg

    m.kg/m,vHHVHHV

    kg

    m

    .kPa.

    K.

    kmol

    kg.

    K.kmol

    m.kPa.

    P

    T

    MW

    R

    v

    m

    kJ,

    .

    .,

    T

    T

    P

    P

    kg

    kJ,

    kg

    m.kg/m,vHHVHHV

    kg

    m.

    kPa.

    K.

    kmol

    kg.

    K.kmol

    m.kPa.

    P

    T

    MW

    Rv

    vm

    u

    r

    rrT,rPvmixturev

    vm

    u

    1205345430920116

    454303251013

    15283

    0517

    3148

    92011615283

    1293

    1

    364537

    12053411164537

    4111325101

    15293

    0517

    3148

    33

    3

    3

    3

    33

    3

    3

    HHVHHV

    :atm3andC10At o

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    Typical Fuel Gases

    There are two types of natural gas that produced fromthe decay of organic matter and that which has been

    trapped deep in the earths crust since the earth was

    formed.

    Natural gas has the highest gravimetric heating value ofall fossil fuels, about 55,000 kJ/kg, or 37,000 kJ/m3at 1 atm

    and 20oC.

    Natural gas is commonly sold in units of therms( 1 therm

    = 100,000 Btu)

    Natural gas can be converted to liquified natural gas

    (LNG) at -127oC. Some companies use large underground

    cavities, including domed, sealed aquifers to store LNG.

    Natural Gas

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    Liquified petroleum gas (LPG), sometimes called refinery

    gas, is composed of the light distillates of petroleum,primarily propane and butane.

    Water gas is a manufactured fuel gas that is produced by

    alternately passing steam and air through a bed of

    incandescent coke.

    There are many proposed processes for producing

    high-Btu and medium-Btu fuel gases from coal. The

    high-Btu gas is commonly called synthetic natural gas or

    simply SNG.

    There are several fuel gases are called producer gas,which are produced normally by burning low-grade coal

    seams in the ground (in situ) with insufficient air for

    complete combustion.

    Manufactured Fuel Gases

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    Coke-oven gas is an excellent fuel gas with a high

    heating value. The gas is essentially composed of thevolatile matter of a caking coal. The gas is a byproduct of

    the industry that supplies coke to the steel industry.

    Blast-furnace gas was a low-quality fuel gas resulting

    from the steel industry. It was produced by burning natural

    gas or other fuel with insufficient air.

    Sewage gas has been used as a heating fuel in several

    cities in the eastern U.S. since colonial times. Most of the

    interest in sewage gas involves the utilization of animal

    and vegetable wastes (biomass), particularly the wastefrom large cattle feed lots, to generate the gas. Sewage

    gas is almost pure methane, which is produced in the

    decay process.

    Byproduct Fuel Gases

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    Fluid-Moving Systems

    Two basic fluid moving systems are employed in almost

    all steam-generator systems. These are the pumps

    needed to supply the working fluid to the steam

    generator and the air compressors or fans needed to

    supply combustion air to the furnace. An important

    parameter for these systems is the mechanical eff ic ienc y

    mech, which is a measure of the machines ability totransmit mechanical work to the fluid flowing through the

    device. The mechanical efficiency for fluid-moving

    systems is given by:

    inputworkactual

    inputworkidealmechh

    For a primer mover, such as a turbine, the mechanical

    efficiency is:

    outputworkideal

    outputworkactualmechh

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    The speci f ic speed of a given pump is defined as theangu lar veloc i ty, in r/min , of a geometr ically sim i lar

    pump, reduced in s ize, wh ich w i l l prod uce a volumetr ic

    f low rate of 1 gal/m in against a total pressu re rise of 1

    lb/in

    2

    . The specific speed of a given pump can bedetermined from a known volumetric flow rate of Q

    gal/min over a pressure rise of Plb/in2at an angular

    velocity of Nr/min:

    413

    21

    /

    /

    s

    P

    NQN

    D

    The boiler feed pump supplies high-pressure liquid

    water to the boiler and commonly operates over a wide

    range of pressures. The centrifugal pump is commonlyused for this purpose and the performance of these

    systems is usually expressed in terms of the speci f ic

    speed Nsof the pump.

    Boiler Feed Pumps

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    A condition that should be avoided during the operation of

    any liquid pump. This condition is called cavitat ion.

    Cavitation occurs when the liquid pressure on the surface ofthe impeller falls below the vapor pressure of the liquid. This

    causes vapor bubbles to form on the surface of the impeller

    and these bubbles collapse as they move into a region of

    higher pressure. The sudden collapse of these bubbles

    causes severe impact loads on the impeller and this actioncan cause severe erosion of the impeller surface. Not only

    can cavitation physically damage the pump but it also

    drastically lowers the mechanical efficiency of the pump and

    makes it noisy.

    Cavitation can be alleviated by increasing the fluid pressure

    at the pump inlet. This pressure, minus the vapor pressure of

    the liquid, is called the net positive suction head or NPSH,

    which is commonly specified by the pump manufacturer.

    Cavitation

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    There are two general types of air compressors

    posi t ive displacementair compressors and dynamicair

    compressors.

    In the positive-displacement compressor, the impeller

    or piston forcibly displaces the air volume to compress

    it. Common positive-displacement air compressors are

    the reciprocating and rotary compressors.In the dynamic air compressor, the high-velocity

    impeller transfers momentum from the impeller to the

    air. The two categories of dynamic air compressors are

    the axial-flow (gas turbine) and centrifugal (fossil-fuel)compressors.

    Combustion-air fans (centrifugal) usually have very

    high flow rates but total pressure rises of less than 15

    to 20 kPa (2 to 3 psia).

    Combustion Air Systems

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    Since the pressure across any fan is relatively small,

    the air flow through the fan can be assumed to be

    incompressible. The so-called fan or pump lawsapply,

    that is, for geometrically similar centrifugal machines,operating at the same efficiencies, the pressure rise P

    across the device, the volumetric flow rate Qthrough

    the device, and the input power requirements Pare

    related by the following equations:

    Where ris the fluid density, Nis the angular velocity,and Dis the diameter of the impeller.

    5343

    222

    31 DNkPQkPDNkPNDkQ rDrD ;;

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    There are two basic types of mechanical-draft systems,

    the forced-draft and the induced-draft systems.

    In the induced-draft (i-d) system, the fan draws

    combustion products from the combustion chamber

    and discharge them into the stack.

    In the forced-draft (f-d) system, the fan pumps only

    combustion air into the furnace.

    For the f-d fan, we should consider both the air and

    the water vapor separately. The volumetric flow rate for

    f-d fan can be calculated as:

    Volumetric Flow Rate of Forced-Draft Systems

    016189728

    1

    ..P

    TR

    F

    AQ

    Q

    u

    D.G.AFD

    FD

    ratefuel

    fand-fforrateflowVolumetric

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    Example IV-3.2

    A 600-MWepower plant burns Lafayette County ,

    Missouri, coal with average moisture and ash fractions

    of 14 and 11%, respectively. This plant operates with a

    heat rate of 8863 Btu/kWh. An analysis of the refuse pit

    gives a higher heating value of 2605 kJ/kg. An orsat

    analysis of the flue gas gives 13.78% CO2, 4.9% O2, and

    0.75%CO. Find (a) The thermal efficiency of the powerplant. (b) The coal rate. C) The capacity of the f-d fan, in

    kg/min and ft3/min, if atmospheric conditions are 50oC,

    0.93 atm, and a relative humidity of 50%.

    38500

    8863

    34123412.

    a

    :Solution

    th

    rateheat

    plantofefficiencythermalThe

    Btu/kW3412Btu/kWrateheatThe

    th

    h

    h

    h

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    ton/h248.7tonne/h225.6kg/h225,600

    kW600,000

    fuelofHHVburned-as

    powerthermalrateCoal

    kJ/kg.2605refuseofHHV:analysisRefusekJ/kg.33,160HHV

    S,5.2%,N1.3%,O9.3%,H5.6%C,78.6%:analysisultimateCoal

    e

    222

    11014011603338510

    36001

    5800095011014017860

    0095011011950

    1195092050

    110

    92050079500101

    0795077832

    2605

    ..kg/kJ,kJ/kJ.

    h/ss.kW/kJ

    coalkg/burnedCkg.....CCC

    coalkg/Ckg...ARC

    coalkg/Rkg..

    .

    R/A

    AR

    Rkg/Akg...R

    C.

    R

    A

    Rkg/Ckg.,HHV

    HHV

    R

    C

    b

    ththe

    ee

    rul tb

    rr

    ul t

    r

    rC

    Rr

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    32

    min

    kg,..

    ,

    F

    Am

    .

    ...../...

    .

    NCO%CO%/CN%.

    F

    A

    %....N%

    ...P

    P.

    ..PP

    c

    D.G.Adf

    ul t,b

    A.G.D

    airdry

    v

    x,Co@satv

    460388039043550160

    600225

    1

    7680

    11014010130781375058098803322

    7680

    3322

    98807504947813100

    89460930714

    6220

    7891150

    222

    2

    050

    ratecoalfand-fforrateflowmassGas

    coalair/kgkg9.803

    orsatfrom

    airdryO/kgHkg0.043550.89440.622

    lb/in0.8946

    0.5;humidityrelative:aircmbustiontheinMoisture

    2

    2

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    33

    min

    ft,,

    .

    .

    .

    ft

    inatm.

    atm

    in/lbf.

    RR.lbmol

    lbf.ft

    coallbm

    airlbm.

    h

    min

    ton

    lbm

    h

    ton.

    ..P

    TR

    F

    AV

    V

    in

    u

    D.G.A

    df

    df

    3

    2

    22

    0003711

    0218

    043550

    7928

    1

    144930714

    4601221545

    8039

    60

    20007248

    02187928

    1

    ratecoal

    fand-fforrateflowvolumetricGas

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    Combustion Methods and Systems

    Gaseous fuels, including natural gas, are the easiestfossil fuels to burn. The fuel gas needs little or no

    preparation before combustion. It must be simply

    proportioned, mixed with air, and ignited. This can be

    accomplished in the following ways:The atmospher icgas burner: The momentum of the

    incoming gas is used to draw the primary air into the burner in

    a process called aspiration.

    The refractorygas burner: Commonly used in steam

    generators. The combustion air is drawn in around the burner,

    which has multiple gas jets that produce good mixing.

    The fan-mixburner: The fuel gas is introduced from nozzles

    mounted at the angle in a rotating spider burner.

    Gas-Fired Systems

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    Oil is somewhat more difficult to burn than natural gas

    because the burner must prepare the fuel for combustion

    as well as proportion it, mix it with air, and burn it. There

    are several ways to prepare the fuel oil for combustion:

    Oil-Fired Systems

    Vaporization or gasification:

    The vaporization technique is

    particularly well suited for thelight fuel oils.

    Atomization of the oil droplets

    can be accomplished with the

    use of high-pressure air orsteam, or the liquid oil film can

    be torn apart by centrifugal force.

    Figure at right shows a common

    rotary-cup (mechanical

    atomization) burner.

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    The pu lver ized-coal furn aceburns finely powdered coal

    and air in a gaseous torch. This combustion system can

    produce much higher capacities than the stokerfurnaces, it gives fast response since there is little

    unburned fuel in the combustion chamber, it reduces the

    amount of excess air required for combustion and this

    reduces the NOxemissions, it can burn all ranks of coalfrom anthracitic to lignitic, and it permits combination

    firing (refers to the capacity of burning coal, oil, or

    natural gas in the same burner). Normally, only one type

    of fuel is burned at a time although two different fuels

    can be simultaneously burned for short periods of time.

    The pulverized-coal furnace finds widespread application

    in coal-fired power plants.

    Pulverized-Coal Furnace

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    The f lu idized-bed furnaceis a radically new type of

    combustion system that has been under development

    and testing during the last 30 years. In this unit, crushedcoal and either crushed dolomite or limestone are mixed

    in a bed that is then levitated by the combustion air

    entering the bottom of the furnace. The boiler evaporator

    tubes are immersed directly in the fluidized bed and thedirect contact between the burning coal particles and the

    water tubes produces very high heat-transfer rates,

    reducing the size of the unit. This arrangement (see Culp

    text Figure 4.18 on your course pack) also produces very

    low combustion temperatures, and traps the sulfur in the

    furnace, thereby permitting the utilization of high-sulfur

    coal.

    Fluidized-Bed Combustion System

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    Steam Generators

    The steam generatoror boi leris a combination of

    systems and equipment for the purpose of converting

    chemical energy from fossil fuels into thermal energy

    and transferring the resulting thermal energy to a

    working fluid, usually water, for use in high-temperature

    processes or for partial conversion to mechanical energy

    in a turbine.In most modern large power plants, one boiler is used

    to supply steam to one steam-turbine generator unit. The

    bo i ler complexincludes the ductwork and air-handling

    equipment, the fuel-handling and processing equipment,the furnace, the water supply and treatment system, the

    steam drums and piping, the exhaust gas system, and

    the pollution control systems including scrubber and

    electrostatic precipitator or baghouse filter.

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    The heat transfer sections of a large boiler include the

    prim ary heat trans fer su rfaces(the evaporator,

    superheater, and the reheater) and thesecondary heat

    transfer surfaces(the air preheater and the economizer).An energy flow diagram for a typical large steam

    generator is shown in the figure below.

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    Steam boilers can be classified many ways but there are

    actually two basic types of steam generators, depending

    on the orientation of the water-steam and hot-gas flowpaths. These two general classifications are the f i re-tube

    boilers and the water-tubeboilers.

    The common f ire-tubeboiler is essentially composed of a

    water-filled pressure vessel containing a number of tubeswhich are the passage-ways for the hot exhaust gas and

    through which heat is transferred from the hot gas to the

    water in the vessel. This system is the simplest and probably

    the least expensive of all the steam generators.

    In the f ire-tubesystem, the high-pressure water is placed onthe external surface of the tubes. Since most pressure-vessel

    codes will limit the external pressure on a tube to half that for

    internal pressure, the fire-tube systems are limited to relatively

    low steam pressures.

    Boiler Types and Classifications

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    The f i re-tube steam generatoris commonly employed in

    small industrial plants, and these systems can be

    purchased in the form of complete operation package.

    Figure below shows a typical two-pass, packaged, fire-tube steam generator.

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    The water-tube boilers are best suited for high-

    pressure, high-capacity steam generators. The high-

    pressure water and the steam flows from tube headers or

    drums through tubes in the furnace walls or in the tubebundles mounted in the exhaust gas duct.

    The water-tube steam generators may be classified as either

    natural-circulation systems or forced-circulation boilers.

    In a natural-circulation boiler the saturated water flows fromthe steam drum high in the boiler, through the downcomer

    tubes to the bottom or mud drum.

    In a forced-circulation boiler, the fluid is pumped through the

    evaporator section of the boiler.

    The most widely used forced-circulation boiler system in theU.S. is the universal-pressure or Benson boi ler.

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    Benson Boiler

    In the Benson boiler, the

    water is pumped to about

    35 MPa (5000 psia) in the

    main feed pump. The

    compressed water is then

    piped to the economizer

    section, through heevaporator tubes, through a

    transition section, and

    finally through a convection

    superheater, where it isexhausted to the turbine at

    a pressure around 24 Mpa

    (3500 psia).

    CS convection superheater

    E economizerFP feed pump

    O steam to service

    T tube evaporating sections

    TS transition section

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    The primary heat-transfer surfaces in the boiler include the

    evaporator section, the superheater section, and the reheat

    section if the power cycle employs reheat.The evaporat ivesurface is usually located in the hottest part of

    the boiler near the combustion zone because the boiling water in

    the tubes protects the tube material from excessive

    temperatures.Superheatersections are the heat-transfer surfaces in which

    heat is transferred to the saturated steam to increase its

    temperature and available energy. Superheaters are particularly

    important in the production of turbine steam to reduce the

    moisture content of the steam as it passes through the turbine.The reheat section of a large boiler is that portion of the boiler

    in which all of the steam exhausting from the high-pressure

    turbine is returned for additional superheat before it is sent to

    the intermediate-pressure turbine or turbine section.

    Primary Boiler Heat-Transfer Surfaces

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    The secondary heating surfaces recover heat from the

    flue gas after it has passed over the primary heat-transfer

    surfaces. In order to achieve a high boiler efficiency, it isdesirable to lower the temperature of the exhaust gas as

    much as possible. There are two kinds of secondary

    heat-transfer surfaces, the economizer and the air

    preheater.The economizer(normally a cross-flow heat exchanger)

    transfers heat from the flue gas to the incoming boiler

    water. It has been estimated that an increase of 6 to 7oC

    in the temperature of the feedwater produced from the

    heat recovery in the economizer will increase the boiler

    efficiency about 1%.

    The air p reheatertransfers thermal energy from the

    exhaust gas to the cold combustion air.

    Secondary Boiler Heat-Transfer Surfaces

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    47

    There are twobroad classes of air p reheater, the

    regenerative heaters and the recuperative heaters.

    The recuperat ive heater is a plate-type or tubular heat

    exchanger operating as either a counteflow or crossflow unit.A shot-cleaning system, rather than a soot-blower system, is

    commonly used to clean the flue-gas side of these heat

    exchangers.

    The regenerativeair preheater, or Ljungstrum heater,

    employs a large rotor assembly with approximately half of the

    element mounted in the exhaust gas duct and the other half in

    the supply air duct. The rotating element, which usually turns

    2 to 4 r/min, contains many corrugated laminas that are

    alternately heated by the flue gas and cooled by thecombustion air.

    The air preheaters are useful in other ways than just

    improving the overall efficiency of the unit, it reduces the time

    required for fuel ignition, thereby improving fuel combustion.

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    One problem associated with any coal-fired boiler

    system, particularly a pulverized-coal system, is the ash

    content of the flue gas and the resulting buildup of ash or

    slag deposits on the heat-transfer surfaces of the boiler,both the primary and the secondary surfaces. It is

    common practice in coal-fired boilers to incorporate

    devices, called soot blowers, to remove the ash deposits

    from the tubes (as shown in the figure below).

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    49

    Most of the modern steam generators are rated in terms

    of steam capacity (usually lbm/h) along with the steam

    outlet pressure and temperature.The figure of merit for operation of a boiler is the boiler

    or steam-generator efficiency sg. This quantity is defined

    as the fraction the input chemical energy that is

    transferred to the working fluid. The boiler efficiencycommonly ranges from 70 to 90%.

    There are two ways to calculate the boiler efficiency, the

    direct method and the indirect method.

    Boiler Rating and Performance

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    It is assumed that the total fuel-input energy is either

    transferred to the working fluid or is lost in a number of

    ways. There are a total s ixboiler heat losses and all ofthem are calculated in terms of energy lost per unit mass

    of fuel (kJ/kg). Using this system, the steam-generator

    efficiency becomes:

    Indirect Method to Calculate Boiler Efficiency

    %HHV

    HHV

    %

    fuel

    fuel100

    100

    lossestotal

    fuelofvalueheatinghigher

    lossestotal-fuelvalueofheatinghigherEfficiencyBoiler sgh

    1 The Dry Gas Loss (DGL)

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    The dry-gas loss (DGL) is that portion of the boiler losses

    that can be attributed to the combustion air supplied to

    the steam generator.

    1. The Dry-Gas Loss (DGL)

    analyses.ultimateburned-asandrefusethefromdetermined

    asfractionmasshydrogenandmoisture,refuse,theareand,,and

    Ce,temperaturgas-flueoutlet

    Ce,temperaturairinlet

    air)ofasthesamebeto(assumedgasflueofheatspecific

    fuel/kggasfluedryofkg,

    where

    DGL

    o

    o

    2

    2

    2

    00351

    901

    901

    HMR

    T

    T

    CkJ/kg..c

    HMR.F

    Aw

    TTcHMR.F

    A

    TTcw

    out,g

    in,g

    op

    D.G.A

    g

    in,gout,gpD.G.A

    in,gout,gpg

    2 The Moisture Loss (ML)

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    53

    The moisture loss (ML) includes the loss due to

    vaporizing the moisture in the fuel and the loss due to the

    latent heat of the moisture produced from the combustionof the hydrogenin the fuel:

    2. The Moisture Loss (ML)

    in,gout,gws

    oout,g

    in,gout,gws

    oout,g

    in,gw

    out,gs

    ws

    T.T..hh

    T

    T.T.hh

    T

    kg/kJTh

    kg/kJ

    Th

    hhHM

    1874926162492

    300

    187409322442

    300

    9 2

    C,toequalorthanlessisIf

    C,exceedsIf

    ,e,temperaturgasinlettheatwaterofenthalpyspecific

    gas),fluetheinvaporwatertheofpressurepartialeapproximat(the

    kPa7ofpressureaandatsteamdsuperheateofenthalpyspecific

    where

    ML

    3 The Moisture in Combustion air Loss (MCAL)

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    54

    Another but much smaller moisture loss is the moisture-

    in-combustion-air loss (MCAL), it is at least an order of

    magnitude lower than the moisture and dry-gas losses formost fuels.

    3. The Moisture-in-Combustion-air Loss (MCAL)

    in,gsat

    satatm

    sat

    w,p

    in,gout,gw.pD.G.A

    TP

    PP

    P.

    c

    TTcF

    A

    atvaporwatertheofpressuresaturationtheis

    humidityrelativetheis

    and

    CkJ/kg.1.926orvaor,waterofheatspecifictheis

    airdry/kgOHkginair,enteringtheofratiohumiditythewhere

    MCAL

    o

    2

    6220

    4 The Unburned Carbon Loss (UCL)

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    The unburned-carbon loss (UCL) is the boiler loss

    associated with the appearance of carbon in the refuse.

    This loss is equal to the product of the mass of unburnedcarbon per unit mass of fuel in the refuse (Cr) and the

    higher heating value of the carbon (HHV)carbon:

    4. The Unburned-Carbon Loss (UCL)

    carbonofvalueheatinghighertheis

    refusetheinfuelofmassunitpercarbonunburnedofmasstheis

    where

    UCL

    carbon

    r

    carbonr

    HHV

    C

    HHVC

    5 The Incomplete Combustion Loss (ICL)

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    The incomplete-combustion loss (ICL) is the energy lost

    as the result of the formation of carbon monoxide instead

    of carbon dioxide in the combustion process. The ICL canbe determined from the following equation:

    5. The Incomplete-Combustion Loss (ICL)

    analysisorsatthefromdirectlyvaluetheis

    analysisorsatthefromdirectlyvaluetheis

    fuelofmassperburnedcarbonofmasstheiswhere

    12.01ICL

    2

    22

    236300128

    CO%

    CO%

    C

    kg/kJCO%CO%

    CO%C

    CO%CO%

    HHVCCO%.

    b

    bCOb

    6 The Radiation Loss (RL)

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    The radiation and unaccounted loss (RL) cannot be

    explicitly calculated, but is estimated from the data

    presented in the Figu re 4.31 below. The data from thisgraph give the radiation loss as a function of the actual

    steam output and the maximum design output, in MBtu/h,

    as well as the number of cooled walls in the furnace.

    fuelHHV

    RL

    4.31Figurefromfactor

    6. The Radiation Loss (RL)

    E l IV 3 3

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    Example IV-3.3

    Using the data from Example IV-3.2 perform an energy

    balance for the system and calculate the boiler

    efficiency. Assume that the boiler has three sides thatare water-cooled and the system is operating at 10% of

    full power during the boiler test.

    fuelkgkJ

    TTcHMRF

    ADGL

    CTcoalkgkgHkgkJHHV

    coalkgkgCai rdrykgOHkgcoalkgkgC

    M WPRMCT

    Solution

    i nou tp

    DGA

    oou tfuel

    br

    eoi n

    /.

    ......

    .

    .,/./,

    ,/.,/.,/.

    ,,.,.,

    :

    ..

    92427

    50288003510420914011950018039

    901

    :(DGL)lossgas-Dry

    2880420and;87024

    58004355000950

    60011950140503.2,-IVExampleFrom

    2

    2

    2

    :(ML)lossMoisture

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    59

    h

    MBtu

    kWh

    Btu

    fuelkg/kJ...

    ..,C,ICL

    fuelkg/kJ..,C,UCL

    fuelkg/kJ....

    TTcF

    AMCAL

    fuelkg/kJ.

    .....

    T.T..HM

    hhHMML

    b

    r

    inoutw,pD.G.A

    inout

    ws

    5318

    47077813750

    7505806302363023

    4311009507783277832

    71955028892610435508039

    11470

    50187428892616249204209140

    18749261624929

    9

    2

    2

    8863kW600,000powerinputboiler(max.)Design

    :(RL)lossRadiation

    %CO%CO%CO

    :(ICL)losscombustion-Incomplete

    :(UCL)losscarbon-Unburned

    :(MCAL)lossair-combustion-in-Moisture

    :(ML)lossMoisture

    2

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    %.%,

    .,

    fuelkg/kJ.,.,

    H H V

    fuelkg/kJ.......

    fuelkg/kJ.,.H H V.

    ...

    h/MBtu..

    h/MBtu.

    sg

    fuel

    fuel

    67710078024

    922519efficiencygeneratorSteam

    9225191555478024

    lossestotalsteamthefer toheat transUseful

    1555464414707431171951147092427

    RLICLUCLMCALMLDGLlossesTotal

    :balanceEnergy

    6441780240178001780RL

    017808100220

    wallscooled-water3forfactorcorrection

    wallscooled0forfactor4.31FigurefromFactor

    4425425410poweroutputboilerActual

    4254532080poweroutputboiler(max.)Design

    Then80%.efficiencyboilerthat theAssume

    h