lectures - gas emissions - b&w

Upload: anonymous-m2wqfyr

Post on 03-Jun-2018

225 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/12/2019 Lectures - Gas Emissions - b&w

    1/36

    ENVIRONMENTAL MANAGEMENTENGINEERING

    Gas emissions

    Prof. Fulvia CHIAMPO

    Academic Year 2013-14

  • 8/12/2019 Lectures - Gas Emissions - b&w

    2/36

    CHARACTERISTIC PARAMETERSFOR FLUE GASES

    Composition (% by volume)

    Temperature (C)

    Pollutants (mg/Nm3)

    Micropollutants (g/Nm3)

    State of the pollutants (solid, vapor, gas)

    Dust (mg/Nm3)

    Particle size distribution

    Boiling point of the pollutants (C)

  • 8/12/2019 Lectures - Gas Emissions - b&w

    3/36

    ELEMENTS OF LEGISLATIONFOR FLUE GAS EMISSIONS

    The legislation considers the main pollutants emitted with flue gases.

    The limits of pollutant concentration change according to theindustrial activity that produces the pollutants themselves.

    Normally, the main pollutants considered by legislations are:

    - DUST-SO2

    -NOx(NO and NO2)

    -CO

    -HCl and HF (hydrogen chloride and hydrogen fluoride ! Not ACIDS)

    -METALS

    ..

  • 8/12/2019 Lectures - Gas Emissions - b&w

    4/36

    .....

    -Gas and vapor organic substances, expressed as total organiccarbon (TOC)

    -PCDD and PCDF (polychlorodibenzodioxins andpolychlorodibenzofurans).

    Taking into account that the emissions are gas, the limits must bedefined at a fixed temperature and at a fixed pressure, very often at a

    empera ure o , an a a pressure o , a.The emission limits, also those of gases (for example, SO2) arealways expressed in mass/ volume.

    The modern legislations contain also:

    -the monitoring plan-the control plan

    and of course

    - penalties (fine and/or arrest).

  • 8/12/2019 Lectures - Gas Emissions - b&w

    5/36

    PCDDs and PCDFsDIBENZODIOXIN STRUCTURE

    75 congeners ofPOLYCHLORODIBENZODIOXINS

    DIBENZOFURAN STRUCTURE

    135 congeners of

    POLYCHLORODIBENZOFURANS

  • 8/12/2019 Lectures - Gas Emissions - b&w

    6/36

    REMOVAL/SEPARATION

    In general, a force must be applied to separate two systems; it canbe:

    -gravitational (it is FREE but its efficiency is satisfactory just for

    large and heavy particles)

    -mechanical (centrifugation, filtration)

    -

    -intermolecular attractive (adsorption).

    C1 C2 C1= INLET MASS CONCENTRATIONC2= OUTLET MASS CONCENTRATION

    SEPARATION EFFICIENCY =

  • 8/12/2019 Lectures - Gas Emissions - b&w

    7/36

    SOLID PARTICLE (DUST) REMOVAL

    SEPARATION EFFICIENCY

  • 8/12/2019 Lectures - Gas Emissions - b&w

    8/36

    CYCLONES

    vIN= 15-40 m/s

  • 8/12/2019 Lectures - Gas Emissions - b&w

    9/36

    INVOLUTE CYCLONE

  • 8/12/2019 Lectures - Gas Emissions - b&w

    10/36

    AXIAL CYCLONES

    Battery of vane axial cyclones

  • 8/12/2019 Lectures - Gas Emissions - b&w

    11/36

    CYCLONE

    DP(m)

    0-1 1-2 2-3 3-4 4-5 5-6 6-7 7-8 8-9 9-10 10-15 15-20 20-30 30-40 40-50 50-75

    DP,MEAN

    (m) 0.5 1.5 2.5 3.5 4.5 5.5 6.5 7.5 8.5 9.5 12.5 17.5 25 35 45 62.5

    fD 1 3 4 5 4 3 3 5 12 15 18 7 8 7 3 2

    0 0 0 0 0.05 0.15 0.2 0.35 0.5 0.8 1 1 1 1 1 1

    *D

    T= fD

    fD* = fD(1 )/(1 T)

    For this cyclone, T= 0.66 = 66 %

    cIN= 3 g/m3 Q = 1200 m3/h

    With T= 0.66, cOUT= 1 g/m3 and

    SEP= (3 1) 1200 = 2400 g/h REMOVED PARTICLES

  • 8/12/2019 Lectures - Gas Emissions - b&w

    12/36

    CYCLONE

    Q = vINS = vINDODO/2 = vINDO2/2

    With vIN= 25 m/s, DO= 0.16 m

    DC= 5 DO= 0.8 m L = 8 DO= 1.28 m

    30

    f(D)

    f(D)*

    0

    10

    20

    0 10 20 30 40 50

    fD,

    fD*

    DP,MEAN(m)

  • 8/12/2019 Lectures - Gas Emissions - b&w

    13/36

    FILTRATION

    Woven filters

  • 8/12/2019 Lectures - Gas Emissions - b&w

    14/36

    FILTRATION

    Felted filters

  • 8/12/2019 Lectures - Gas Emissions - b&w

    15/36

    FABRIC FILTER WITHVENTURI CLEANING SYSTEM

  • 8/12/2019 Lectures - Gas Emissions - b&w

    16/36

    vF= 0.01 0.06 m/s

    DB= 0.15-0.7 m

    LB= 1.5-4m

  • 8/12/2019 Lectures - Gas Emissions - b&w

    17/36

    FABRIC FILTER

    DP(m) 0-1 1-2 2-3 3-4 4-5 5-6 6-7 7-8 8-9 9-10 10-15 15-20 20-30 30-40 40-50 50-75

    DP,MEAN(m)

    0.5 1.5 2.5 3.5 4.5 5.5 6.5 7.5 8.5 9.5 12.5 17.5 25 35 45 62.5

    fD 1 3 4 5 4 3 3 5 12 15 18 7 8 7 3 2

    0.85 0.95 1 1 1 1 1 1 1 1 1 1 1 1 1 1

    f*D 50 50 0 0 0 0 0 0 0 0 0 0 0 0 0 0

    T= fD

    fD* = fD(1 )/(1 T)

    For this filter, T= 0.997 = 99.7 %

    cIN= 3 g/m3 Q = 1200 m3/h

    With T= 0.997, cOUT= 0.009 g/m3 and

    SEP= (3 0.009) 1200 = 3589.2 g/h REMOVED PARTICLES

  • 8/12/2019 Lectures - Gas Emissions - b&w

    18/36

    FILTER

    Q = vINS AND with vIN= 0.04 m/s, S = 8.3 m2

    S = NDBL

    With DB= 0.15 m and L = 1.5 m, we obtain N = 11.8 N* = 12 bags

    60

    f(D)

    0

    20

    40

    0 25 50

    fD,

    f*D

    DP,MEAN(m)

  • 8/12/2019 Lectures - Gas Emissions - b&w

    19/36

    ELECTROSTATIC PRECIPITATOR

  • 8/12/2019 Lectures - Gas Emissions - b&w

    20/36

    The gas velocity must be in the range of laminar flow, to avoidsolid particle detachment.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    21/36

  • 8/12/2019 Lectures - Gas Emissions - b&w

    22/36

    ADSORPTION

  • 8/12/2019 Lectures - Gas Emissions - b&w

    23/36

    ADSORPTION is an exothermic surface phenomenon that occurs

    between a solid (adsorbent) and a compound (adsorbate) distributedin a gas or in a liquid (solution).

    It is a MASS TRANSFER OPERATION.

    Adsorbate can be bonded on the adsorbent through weak forces,

    such as van der Waals and London forces (physical adsorption more common), or through an exchange of electrons(chemiadsorption) with chemical reaction.

    .

    Physical adsorption is reversible, with exothermicity 4-40 kJ/moladsorbate.

    Chemiadsorption is nonreversible, with exothermicity > 200 kJ/moladsorbate.

    Very often, the solid is activated carbon.

    Other common adsorbents are: silica gel, zeolites, syntheticpolymeric adsorbents.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    24/36

    CHARACTERISTICS OF ACTIVATED CARBON

    Their origin can be vegetal (very common, from weak woods) ormineral (their use is limited).

    According to their morphology, they can be:- Powdered activated carbon (PAC): particle size in the range 1-150m

    - Granular activated carbon GAC : article size in the ran e 0.5-4 mm

    - Extruded activated carbon: particle size in the range 0.8-4 mm

    Typically the activation, to say the creation of activated sites, isthermal (to say, using heat), even if chemical one is sometimes

    carried out.

    Thermal activation is carried out at 850-1000 C, with a gase ousactivating agent (very often steam).

  • 8/12/2019 Lectures - Gas Emissions - b&w

    25/36

    CHARACTERISTICS OF ACTIVATED CARBON

    Activating agent, duration and temperature of operation influence theadsorbent characteristics, namely:

    -

    the inner surface area; typical values are 400-1500 m2

    /gADSORBENT- the pore volume; it can be in the range 0.1-0.8 ml/gADSORBENT

    -the porosity (% void); never > 50 % for structural reasons.

    ,

    -micropores: d < 2 nm

    -mesopores: d = 2-50 nm

    -macropores: d > 50 nm.

    For physical adsorption, lower the operation temperature higher thequantity of adsorbed compounds.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    26/36

    FREUNDLICHS ISOTHERM

    x = kAD

    c1/n

    [massADSORBATE/massADSORBENT]

    kAD= adsorption capacity[mg/g ] [l/mg]1/n

    1/n = adsorption intensity [-]

    The isotherm describes the

    ADSORPTION EQUILIBRIUM.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    27/36

    REGENERATION AND REACTIVATION

    OF ACTIVATED CARBON

    When the adsorption capacity is exhausted, to say the most

    activated sites are bonded to molecules, the molecules must beremoved through desorption.

    The operation is called regeneration; it exploits the parameters

    Steam or hot air can be used to desorb Volatile Organic Compounds(VOCs) in air treatment applications.

    For wastewater treatment carbons, regeneration is seldom practicedsince a low adsorption capacity is obtained due to the large

    molecules of adsorbate that are not volatilized.Reactivation is similar to the activated carbon manufacturing, withburnoff of the adsorbate and partially of the carbon surface.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    28/36

    DESIGN OF ACTIVATED CARBON PLANT

    For gas treatment, granular carbon is used (powdered carbon is usedjust for masks), distributed in circular columns.

    Freundlichs isotherm gives the maximum quantity of adsorbate thatcan be adsorbed by a unit mass of activated carbon.

    The gas velocity is in the order 0.05-0.4 m/s, to give a contact time of3-4 s.

    Generally, the equilibrium is not reached, so the activated carbonmass obtained with Freundlichs isotherm represents the minimumquantity to achieve a given result.

    The quantity really used in the plant is10-15% more than the calculated oneon the basis of experimental-derivedisotherm relationship

  • 8/12/2019 Lectures - Gas Emissions - b&w

    29/36

    COMBUSTION

    If pollutants are organics, they canbecome fuel and be destroyedthrough combustion.

    Combustion is an oxidation process,

    at high temperature, with a ratherhigh energy generation.

    Process is highly EXOTHERMIC:

    q ~ 13-15 kJ/g O2.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    30/36

    Pollutant combustion is equal to fuel combustion, but the aim is

    destroying the pollutant since it is harmful (in ordinary combustionthe aim is energy recovery).

    So, the controlling parameters are the same (3 Ts rule):

    -temperature: it must be at least 850 C, to have good kinetics

    -time: for homogeneous systems (gas systems) it must be over 1 s

    -turbulence: fluid velocity inside the combustor influencesturbulence level, with a minimum value of 6 m/s.

    Combustion can be carried out in thermal or in catalytic combustors.

    The aim and the result are the same, but the operative conditions aredifferent.

    Generally, auxiliary fuel is used during operation to maintain theoperative temperature (the quantity of pollutant does not develop asufficient quantity of heat).

  • 8/12/2019 Lectures - Gas Emissions - b&w

    31/36

    THERMAL COMBUSTORS

    They have not limits for inner temperature, and they can be used totreat gas flows containing pollutants in high concentration.

    Pollutant concentration influences the combustion temperature;when it is rather high, less auxiliary fuel is used.

    In these combustors, auxiliary fuel can be fed directly to thecombustor where it mixes with the contaminated flow.

    Thermal combustors are robust equipment, to say they can work in awide variability range for operative conditions.

    Flue gases have always high temperatures, so energy recovery ismandatory as much as possible, for example to heat up the inlet flow

    through heat exchangers.This common thermal combustors are named recuperative.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    32/36

    Thermal combustors are named regenerative when energy is

    recovered inside the combustor itself, through packing of ceramicmaterial having the function of a heat wheel able to receive heateasily from such gas and store the heat, then give it back readily tothe gas itself.

    In this way, auxiliary fuel consumption is very low.The combustor is constituted with 2 beds packed with inert ceramicmaterial, joined through an horizontal combustor chambers.

    During operation, the contaminatedgas flows through the first bed ofceramic material and is heated untilreaching a temperature close toself-combustion of the VOC

    molecules contained in the stream.VOC thermal oxidation generatesheat in the top part of the bed and inthe combustion chamber.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    33/36

    After leaving the combustion chamber, the carrier fluid mixed with

    the combustion products, meets and flows through the second bed,cooler than the first, thus giving up most of its enthalpy to theceramic packing. Then, the flue gas is discharged through the stack.

    After reaching the set-point temperature in the top part of the second

    bed, the system is switched to the cyclic operating conditions:-the gas flow is inverted so that it enters the already hot second bed,and after combustion, before discharging, it gives its enthalpy to thefirst bed

    -when again the set-point temperature is reached, the gas input is

    again changed and sent to the first bed.

    Cyclically, each bed works as preheater and heat recovery device.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    34/36

    CATALYTIC COMBUSTORS

    They make use of a catalyst to reduce the activation energy of theoxidation reaction and, consequently, the process temperature.

    The maximum temperature range is 150-650 C:-if lower than 150 C, the kinetics is too slow

    -if higher than 650 C, the catalyst can sinter.

    ,

    window.

    The auxiliary fuel is burnt in a separate heater, then the deriving fluegases are mixed with the polluted gas and sent to the combustor.

    In these combustors, process is flameless, differently from thermal

    ones.

  • 8/12/2019 Lectures - Gas Emissions - b&w

    35/36

    CATALYTIC COMBUSTORS

    To avoid catalyst clogging due to solid particles, filtration of pollutedgas is mandatory.

    In addition, some compounds can be poisons for the catalysts, tosay they bond irreversibly to the catalyst activated sites. Whencatalyst poisoning occurs, catalyst must be replaced and reactivated.

    Ver often catal sts are metals or metal oxides the can be:

    -supported: they are deposited on support (very often alumina,

    Al2O3), in form of pellets (cylinders or spheres, with D = 2-4 mm) ormonolithes (honeycomb)

    -pure: in form of powder (250-750m).

  • 8/12/2019 Lectures - Gas Emissions - b&w

    36/36