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Absorption for HAP and VOC Control. 朱信 Hsin Chu Professor Dept. of Environmental Engineering National Cheng Kung University. 1. Introduction .

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Absorption for hap and voc control l.jpg

Absorption for HAP and VOC Control


Hsin Chu


Dept. of Environmental Engineering

National Cheng Kung University

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1. Introduction

  • Absorption is a diffusional mass-transfer operation. Soluble gaseous component is removed from a gas stream by dissolution in a solvent liquid.The driving force for mass transfer: concentration difference

  • Driving force is positive: absorption Driving force is negative: desorption or stripping

  • Solvent: water or a low volatility organic liquid

  • Adequate solubility

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2. Aqueous systems

  • Acidic gases such as HCl, HF, and SiF4 can be absorbed in water efficiently. Alkaline is better.

  • Less soluble acidic gases such as SO2, Cl2, and H2S can be absorbed more readily in a dilute caustic solution.Na2CO3, NaHCO3, or NaOH < 5~10%CaO, Ca(OH)2, CaCO3: plugging, scalingNH4OH: NH3 slip

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  • CO2: consume more caustic solutionpH < 9: the amount of CO2 absorbed can be kept low

  • NH3: can be removed with acidic water solutions such as dilute H2SO4, H3PO4, or HNO3Becomes fertilizer ingredients

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3. Nonaqueous systems

  • AminesMonoethanol-, diethanol-, and triethanolamine; methyldiethanolamine; and dimethylanalineFor CO2, SO2 and H2S absorbingHigh absorbent cost: absorbent regeneration is a must

  • Organic solventHeavy oils, other solvents with low vapor pressure For organic vapors absorbingAbsorber- stripper system

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4. Types and Arrangements of Absorption Equipment

  • Contact between a gas and a liquidBreak the liquid up into small droplets or thin films, which are constantly renewed through turbulence to provide high liquid surface area for mass transfer

  • Most commonly used devicesPacked and plate columnsOpen spray chambersCyclonic spray chambers

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  • Next slide (Fig. 11.1)

    Countercurrent packed column: maximizes driving force, because it brings the least concentrated outlet gas into contact with fresh absorbing liquid

    However, it plugs rapidly when appreciable particulates are present.

  • Second slide (Fig. 11.2)Spray chamber

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  • Next slide (Fig. 11.3)Cyclonic spray chamber

  • Second slide (Fig. 11.4)Plate columnBubble cap tower: greater variations in gas flow rateSieve plates: simple, low cost but narrow gas flow operating ranges

  • Third slide (Fig. 11.5)Baffle tray tower: plug resistant, mass transfer is poor.

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5. Design Techniques for Countercurrent Absorption Columns

  • Co-current towersCross-flow towersCountercurrent towers: the most frequently used

  • Two main factors:The height: determined by the rate of mass transferThe diameter: determined by the quantity of gas passing up the tower

  • The upper limit of flow occurs when the tower begins to flood

  • Higher flow rates result in higher pressure losses

  • Assume the columns operate isothermally because of the dilute solutions: for the following design equations

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5.1 Equilibrium Relationships

  • Vapor-liquid equilibria for miscible systemsEquality of fugacity in both phases at the same temp. and pressure:

    i: component i, f: fugacity, v: vapor, L: liquid

  • Component i in the liquid phase:xi: molar fraction of component i in the liquid, γi: activity coefficient, :standard state fugacity of the pure component only

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  • The Gibbs-Duhem equation for n componentsM: solution property, :the corresponding partial molar property, T: temp.

  • Using excess Gibbs free energy changes, above equation can be written in terms of the enthalpy and volume changes on mixing △H and △V, respectively, and the activity coefficient, γi:

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  • Solutions of nonpolar molecules or solutions at low concentration, △H and △V are smallTherefore, for a binary mixture:

  • For a solution at low pressure where the vapor is an ideal gas:presuming to be equivalent of the pure component fugacity.At constant temp., above equation can be rewritten:

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  • , the partial pressure of component 1 concentration, △H and △V are smallTherefore, Integrate, Therefore, from partial pressure data of one component of a binary solution, the partial pressure of the second component may be calculated.

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5.2 Ideal Solutions-Henry’s Law concentration, △H and △V are small

  • A general relationship for fugacity of a component in a liquid mixture in terms of the pure component fugacity: (1)

  • An ideal solution: Therefore, , called the Lewis and Randall Fugacity Rule id: ideal solution

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  • F concentration, △H and △V are smallor a pure component

  • Henry’s LawFor a dilute solutionRewrite:ki: Henry’s Law constant

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  • From previous equation: concentration, △H and △V are smallFor solutions at low pressure, and (partial pressure)Therefore, (common form of Henry’s Law)

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  • Rewrite: concentration, △H and △V are smallDefine m=ki/P (a common form for Henry’s Law)Therefore, yi = mxi (2)

  • Henry’s Law is an adequate method of representing vapor-liquid phase equilibria for many dilute solutions encountered in absorption work.However, weak electrolytes: dissociation of the electrolyte may take place upsetting the normal equilibrium relationship.

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5.3 Countercurrent Absorption Tower Design Equations concentration, △H and △V are small

  • Next slide (Fig. 11.7)A packed tower with countercurrent flow

  • Mass balance around the cross-section A-A:yAG + xAL = (yA- dyA)G + (xA+ dxA)LTherefore, G dyA = L dxAHowever, the flow rates do not remain constant through the column:d(GyA) = d(LxA)

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  • Rewrite Eq. (3): cross-section A-A: (4)For dilute solution:Eq. (4) reduces to Eq. (3) which is called the “operating line”.Eq. (4): general equation with a general equilibrium relationship

  • Eq. (2): Henry’s Law Equation , called the “equilibrium line” (will be shown later)

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5.4 Origin of Volume-Based Mass-Transfer Coefficients cross-section A-A:

  • Several theories have been devised Whitman “two-film” concept remains an excellent basis

5.4.1 Steady-State Molecular Diffusion

  • Molecular diffusion serves a basis for mass transfer coefficients Driving force across the interface: concentration gradientComplete thermodynamic equilibrium: no concentration, temperature, or pressure difference in the areas of the diffusion

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  • Assume that only one component is in motion across the interfaceMolecular diffusivity: a relative velocity of the diffusion component with respect to an average velocity of the entire stream is a direction normal to the interface

  • The molecular motion is accounted for by Fick’s Law.Total flux is the sum of the molecular diffusion and the convective bulk flow.

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  • Because y diffusing through a stagnant layer of B, thus . A0+yB0 = 1 yAL+yBL = 1 A loghrithmic mean concentration can be difined: (6)A mass transfer coefficient can be defined: (7)

  • Eq. (6) & Eq. (7) can be substituted into Eq. (5):

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5.5 The Whitman Two-Film Theory diffusing through a stagnant layer of B, thus .

  • Next slide (Fig. 11.8)A schematic diagram

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  • The theory summarized: diffusing through a stagnant layer of B, thus . (1) The gas film and the liquid film, on either side of the interface(2) Transfer in the bulk phases by convection currents Concentration differences are negligible except in the vicinity of the interface (3) On each side of the interface, convection currents die out(4) Both films offer resistance to mass transfer Transfer takes place through these films by a mechanism similar to molecular diffusion(5) The interface is at equilibrium and offers no resistance to mass transfer(6) Uniform composition in the main stream(7) At the interface, yAi and xAi are in equilibrium described by Henry’s Law yAi= mxAi

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  • Packed Column diffusing through a stagnant layer of B, thus . The fluid is in turbulent motionMass transfer through the films is defined by ky and kx (turbulent mass transfer coefficient)

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5.6 Overall Mass-Transfer Coefficients diffusing through a stagnant layer of B, thus .

  • Mass-transfer coefficients defined on the basis of interfacial mole fractions have little practical value since these mole fractions cannot be measured.

  • Two new pseudo-mole fractions are defined as illustrated in the next slide (Fig. 11.9)Overall mass transfer coefficients Ky and Kx are defined based on these new pseudo-mole fractions.yA* = equilibrium mole fraction of the solute in the vapor corresponding to the mole fraction xA in the liquid xA* = equilibrium mole fraction of the solute in the liquid corresponding to the mole fraction yA in the vapor

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  • The mass transfer may now be written: diffusing through a stagnant layer of B, thus .

  • The construction in Fig. 11.9 (last page) illustrates how to determine xA* for any yA, and yA* for any xA.

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  • The overall coefficients (K diffusing through a stagnant layer of B, thus . y & Kx) can be related to the individual phase coefficients (ky & kx) making use of Henry’s Law.Therefore:

  • Also:

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  • Combining: diffusing through a stagnant layer of B, thus .

  • Rearranging:

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5.7 Volume-Based Mass-Transfer Coefficients diffusing through a stagnant layer of B, thus .

  • Packing has a characteristic area per unit volume of packing:

  • Flow rate of vapor and liquid phases, viscosity, density, surface tension, and size and shape of the packing determine the value of “a”.These same factors affect the value of the mass transfer coefficients Ky and Kx.

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  • Therefore, two new quantities K diffusing through a stagnant layer of B, thus . y a and Kx a (volumetric mass transfer coefficients) are common to be used.

  • If A is the absorption tower cross-sectional area, and Z the packing height, then Az is the tower packing volume.Defining Ai as the total interfacial area: Ai = aAzor in differential form: dAi = aAdz

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  • Rewrite in dN diffusing through a stagnant layer of B, thus . A, with units (moles/unit time) = (moles/unit time‧area) (area):or dNA = Kya(yA-yA*)Adz = Kxa(xA-xA*)Adz

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5.8 Determining Height of Packing in the Tower: the HTU Method

  • For the gas phase, the differential rate of mass transfer of component A is equal to the differential rate of change of the mass of A in the incoming gas stream.dNA = d (GyA)

  • Rewrite the flow rate on a solute-free basis:GB = (1-yA)G, where GB is a constantthen,

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  • Therefore, Method (8)

  • A similar equation based on the liquid phase can be written which would be useful in stripping calculations.

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5.9 Dilute Solution Case gas phase, N

  • For dilute solutions, Henry’s Law is usually a good choice for an equilibrium relationship.yA* = mxA (9)(1-yA) ≈ (1-yA)LM ≈ 1.0

  • Therefore, (10)

  • The operating line, yAG - yA1G1 = xAL - xA1L1, may be rewritten as: (11)

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  • Note that gas phase, NThe absorption factor, Ab, can be defined as: (12)

  • Use Eqs. (9), (11), and (12): (13)

  • Substitute Eq. (13) in Eq. (10) and integrate:

  • When a pure solvent such as water is used, xA1 = 0.0:

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6. Countercurrent Flow Packed Absorption Tower Design gas phase, N

6.1 General Considerations

  • When a packed tower is designed for treating a given quantity of gas per hour, the height of packing is determined from mass transfer consideration, and the diameter or cross-sectional area is determined by the gas velocity in the empty tower cross-section.

  • Next slide (Table 11.1)Economic factors in packed tower design

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6.2 Operations as Packed Towers gas phase, N

  • In a packed tower operating in counterflow at constant liquid rate, the pressure drop varies with the gas mass velocity.

  • With liquid holdup in the packing, there is smaller void space in the column, and a higher pressure drop exists than with dry packing.

  • Next slide (Fig. 11.10)Pressure drop vs. superficial gas mass velocity L: liquid flow rate

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  • From Fig. 11.10 (last slide) gas phase, NThe point at which the rate of change of pressure drop increases more rapidly than a constant value has been called the “upper loading point”.The liquid holdup is now increasing with the increasing gas rate.

  • The gas velocity corresponding to this upper limit is known as the “flooding velocity”.At gas rates greater than the flooding velocity, the column will act as a gas bubbler.

  • The greater the liquid rate, the lower the gas velocity at which flooding occurs.Larger, more open packings flood at high velocities than smaller, more dense packings.

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  • Two types of liquid holdup: gas phase, N(1) Static holdup is the volume of liquid per volume of packing that remains after gas and liquid flows are stopped and the bed has drained. Static holdup depends on packing surface characteristics.(2) Operating holdup is the volume of liquid per volume of packing that drains out of the bed after gas and liquid flows have been stopped.

  • Gas flow rate has little effect on holdup below upper loading point. Packed towers may be operated above 90% of the flooding velocity.

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  • Some operational characteristics for countercurrent packed tower:(1) Pressure drop between 0.25 in. and 0.60 in. H2O per foot of packing(2) Air velocity between 5.0 and 8.0 ft/s with modern high capacity plastic packing(3) Inlet concentrations of contaminant in the gas stream not to exceed 5,000 ppmv(4) Liquid irrigation rates typically between 2 and 8 gpm/ft2 of column cross-sectional area(5) L/G: 15-90 L/m3 (5-10 L/m3 for FGD, 1-2 L/m3 for particulates) (based on (2) & (4))

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6.3 Choosing a Tower Packing tower:

  • Two major types of packing:(1) Random dumped pieces(2) Structured modular forms

  • It should have enough mechanical strength to carry the load and allow easy handling and installation.

  • It should be able to resist thermal shock and must be chemically resistant to the fluids being processed.

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6.3.1 Dumped Packings tower:

  • Two of the most popular shapes are rings and saddles.Sizes range from ¼ in. to 3.5 in. with 1 in. being a very common size.

  • Packings are ceramic, metal, or plastic, dependent upon the service.

  • Ceramic materials will withstand corrosion and are therefore used where the resultant solutions are aqueous and corrosive.

  • Metals are used where nocorrosive organic liquids are present.

  • Plastic packing may be used in the case of corrosive aqueous solutions and for organic liquids which are not solvents for the plastic of which the packing is made.

  • Next slide (Fig. 9-34)Common packing materials

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  • Metal packing is more expensive, but provides lower pressure drop and higher efficiency.

  • When using plastic materials, care must be taken that the temperature is not too high and that oxidizing agents are not present.

  • Ring-type packings are commonly made of metal or plastic except for Raschig rings, which are generally ceramic.

  • Ring-type packings lend themselves to distillation because of their good turndown properties and availability in metals of all types that can be press formed.

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  • Usually ring-type packings are used in handling organic solutions when there are no corrosive problems.However, rings do not promote redistribution of liquids, and Raschig rings may even cause maldistribution.

  • Saddles are commonly made from ceramic or plastic and give good corrosion resistance.Saddles are best for redistribution of liquid.

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6.4 Choosing a Liquid-Gas Flow Ratio solutions when there are no corrosive problems.

  • The operating line, yAG - yA1G1 = xAL - xA1L1, may be solved for the exit liquid concentration xA0:

  • Therefore, if L or G/L can be found, the entire material balance will be solved.

  • Next slide (Fig. 11.11)A plot of yA vs. xA

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  • Last slide Fig. 11.11 (left panel) solutions when there are no corrosive problems.With a concave equilibrium line, three possible operating lines are shown. L/G is the slope of the operating line.

  • The line furthest to the right with the smallest slope represents the limit to which the slope of the operating line can be drawn.Thus, this slope represents a minimum L/G ratio in which xA0 and yA0 are actually in equilibrium, and the line could not be drawn with a smaller slope because it would go through equilibrium.

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  • Fig. 11.11(right panel) practically, this point represents a theoretical minimum L/G which never can be attained in practice.With “S”-shaped equilibrium curve, the minimum value of L/G is reached at some point within the column where the operating and equilibrium lines are tangential and thermodynamic equilibrium would be “exceeded” if the L/G ratio were any smaller.

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6.5 Determining Tower Diameter-Random Dumped Packing practically, this point represents a theoretical minimum L/G which never can be attained in practice.

  • Next slide (Fig. 11.12)Use a modified Sherwood flooding correlation to determine tower diameter

  • Second slide (Table 11.2)The definition of terms used in Fig. 11.12

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  • The packing factor, F, is a characteristic of a particular packing size and shape.Oringinally it was defined as a/ε3 where a is the interfacial area per packed volume and ε is the void fraction.

  • However, this definition for F did not adequately predict the packing hydraulic performance.Therefore, Table 11.3 (next slide) presents packing factors which have been calculated from experimentally determined pressure drop.

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  • How to use Fig. 11.12 packing size and shape.From the abscissa, the packing factor, and the required pressure drop per foot of packing, the ordinate of the curve can be read and the value of G* in lb/ft2‧s calculated.

  • With G converted to lb/s the column cross-sectional area As is then:

  • The column diameter can be found from:

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6.6 Determining Tower Diameter-Structured Packing packing size and shape.

  • Sturctured packings are being favored because they have a higher capacity than dumped packing and scaleup is more predicable.

  • Next slide (Fig. 11.13)A capacity correlation for nonfoaming systemsFlow parameter, Efficient capacity CSC (ft/s) =WhereσL = liquid surface tension in dyne/cm, 5 ≤σL≤ 73 dyne/cmμL = liquid viscosity in cp, 0.07 ≤μL ≤ 1.1 cpDesign is carried out routinely up to 90% of efficient capacity.

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  • Because the pressure drop curves for random and structured packings are similar, pressure drop for structured packing can be estimated from the generalized correlation of Fig. 11.12.

  • However, in this case the packing factor is affected by the operating pressure.Useful packing factors from Strigle are reported in Table 11.4 (next slide) for five different sizes of Intalox Structured packing.

  • Table 11.4:The smaller packing factor should be used for pressure below 10.0 psia or at liquid rates below 4 gpm/ft2.

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6.7 Controlling Film Concept packings are similar, pressure drop for structured packing can be estimated from the generalized correlation of Fig. 11.12.

  • The Whitman Two-Film TheoryThe film that offers the predominant mass transfer resistance is called the controlling film.

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  • The overall mass-transfer coefficient can be solved: packings are similar, pressure drop for structured packing can be estimated from the generalized correlation of Fig. 11.12.

  • Gases with a limit solubility in the liquid phase have a high value of m. Therefore, above eq. reduces Ky≈ kx/m → liquid film controlling

  • Gases with a high solubility in the liquid phase have a low value of m.Therefore, above eq. reduces Ky≈ ky → gas film controlling

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6.8 A Correlation for the Effect of L/G Ratio on the Packing Height

  • The correlation is based on a previous Eq.: (14)

  • Henry’s Law is a straight equilibrium line, and the correlation presented in this section assumes Henry’s Law for the equilibrium relationship.

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  • At the minimum L/G ratio y HeightA0 = mxA0Eq. can be solved for L/G:

  • For any yA there is an xA determined by the operating line:There is also a in equilibrium with the xA such that /m.

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  • Define B as a multiple of (L/G) Heightmin to set the actual (L/G): (L/G) = B(L/G)minWith Then,

  • Substitue Eq. (16) into Eq. (15) (previous slide):For the dilute case, substituting this into:

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  • Integrating N HeightOG:This is the same as Eq. (14).

  • Recall Ab is defined as a function of B:Ab = B(1-yA1/yA0)If the value of (yA1/yA0)is fixed at 0.90, 0.95, and 0.99, NOG can be plotted vs. B with (yA1/yA0) as a parameter (next slide, Fig. 11.14).

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  • Fig. 11.14 (previous slide) HeightFor any given B and percent removal, knowing and a, HOG can be calculated, and the height of the column can be calculated from Z = HOGNOG.

  • Since Eq. (14) is derived for the dilute solution, examination of Fig. 11.14 shows that the number of transfer unit, NOG, cannot be greatly reduced by increasing B, the multiple of the minimum L/G ratio, above 1.70.

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6.9 Henry’s Law Constants and Mass-Transfer Information Height

  • Henry’s Law constants can be found in the chemical Engineers Handbook. It is also possible to calculate Henry’s constant for solubility data, seen in the example in Table 11.5 (next slide).

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  • The measurement of mass-transfer coefficients has occupied many experimenters of the past 70 years.It is surprising that there is not much data available in the open literature.

  • The problems of these measurements:(1) Difficulty in determining the interfacial area(2) Difficulty in determining individual coefficients from measurements of overall coefficients(3) Entrance effects

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  • The packing area becomes effective only if it is wetted. many experimenters of the past 70 years.Thus, Kya must include a hidden factor which reflects the proportion of the packing area that is effective.

  • This effective area is proportional to the follwing factors:(1) Liquid rate(2) Type of packing(3) Method of packing the tower(4) Nature of the liquid distribution(5) Height and diameter of the tower

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  • Next two slides ( many experimenters of the past 70 years.Table 11.6)Mass-Transfer Coefficient data

  • Mass-Transfer Coefficient for structured packing are generally greater than dumped packing, indicating improved mass transfer.

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6.10 Using Henry’s Law for Multicomponent Solutions many experimenters of the past 70 years.

  • For a binary solvent composed of j and k pure components, Carroll suggests:Where Hi, mix: the Henry’s constant for solute i in a mixture of j and k Hij, Hik: the Henry’s constants for the pure solvents xj, xk: the mole factions of the solvents ajk: an interaction paramter that must be obtained from experimental data

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  • In the absence of any other information it may be assumed that ajk in the previous Eq. is independent of i or set equal to zero.

  • For mixed solutes at low pressure, it may be assumed that each gas is independent of the other.Therefore, for two solutes i and j:xiHik = yiPxjHjk = yjP

  • Thus the solubility of the individual components is determined by its own partial pressure as if the other component were not present.

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7. Sample Design Calculation that a

To remove a dilute concentration VOC from an air emission with a dilute absorbing solution

  • The problemAn air stream from a electronic circuitry manufacturer contains 50 ppm of a VOC which must be treated.Q = 10,000 acfmP = 1 atm T = 20℃

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  • Emission standard = 90% removal (5 ppm) that aAbsorbing liquid = waterHenry’s Law constant, m = 2.0Mass-transfer coefficient = 4.0 lb moles/h‧ft3L/G = 1.5 (L/G)minPacking = 1” ceramic Intalox saddlesΔP = 0.5” H2O/ft of packingPacking factor, F = 92MW (≈air) = 29.0

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  • Solution: that am = 2.0yi = 2.0xiThe operating line based on :yA = (L/G)(xA-xA1) + yA1Minimum L/G ratio can be calculated by:yA0 = 0.000050 (50 ppm) yA1 = 0.000005 (5 ppm) xA1 = 0.0

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  • The minimum slope operating line is that ayA = 1.80 xA + 0.000005Operating (L/G) = 1.5 (L/G)min = 1.5 × 1.80 = 2.70

  • L/G = can be solved for the operatingxA0 with xA1 = 0.0The operating line then becomesyA = 2.70xA + 0.000005

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  • Calculate the height of the tower, Z: that aZ = HOGNOG = 9.31 × 4.64 = 43.21 ftor from Fig. 11.14 (previous) with B = 1.5 and yA1/yA0 = 90%:Read NOG = 4.6 Z = 9.31 × 4.6 = 42.84 ft

  • Calculate the pressure drop through the column:ΔP = 0.5” H2O/ft of packing × 43.21 ft = 21.61” H2O

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7.1 Flooding that a

  • From Fig. 11.12 (previous), the abscissa is the same, 0.058, and the flooding ordinate is then 2.40.CsF0.5υ0.05 = 2.40

  • Calculate the superficial velocity:

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  • Calculate the gas flow rate: that aQ = V‧As = 7.1929 ft/s × 41.21 ft2 × 60 s/min = 18,045 acfm

  • Actual operation is at 10,000 acfm, therefore, operation is at:

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7.2 Structured Packing that a

  • To treat additional sources or to meet higher electronic circuit production demand, consider the possibility of increasing the air flow to 20,000 acfm by switching to structured packing.

  • Choose Intalox structured packing 2T. The X factor has already been calculated to be 0.058.

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  • Calculate the ordinate of Fig. 11.12: remain the same.CsF0.5υ0.05 = 0.2773 × 200.5 ×1.00.05 = 1.2406

  • The abscissa remains the same, 0.058, from Fig. 11.12, the pressure drop is estimated to be 0.45” H2O/ft of packing.

  • The tower capacity is now determined from Fig. 11.13. The X value of 0.058 is the abscissa of Fig. 11.13.The ordinate value is estimated to be C0 = 0.44 ft/s

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  • The surface tension, remain the same.σ, of water at 70ºF is 70 dynes/ft2.The viscosity, μ, is 0.81 cp.

  • The actual capacity factor Cs = 0.2773 ft/s is below 90% of the maximum tower efficient capacity, 0.90 Csc = 0.414 ft/s.Therefore, the tower, if changed to structured packing, could take even a greater air flow.