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Mass Transfer Column

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    1

    STUDY AND DESIGN OF PACKED TOWER FOR

    ABSORBING GASES WITH LOW SOLUBILITIES

    Heat and Mass Transfer Laboratory project by

    Vishal Surana

    Vivek Nagar

    Vivek Nigam

    under the guidance of

    Dr. A. Kannan and Dr. R. Ramnarayan

    Department of Chemical Engineering

    Indian Institute of Technology Madras

    Chennai - 600 036

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    Contents

    Topic Pages

    1 Acknowledgements 1

    2 Introduction 2

    2 Brief outline of issues tackled in this project 4

    3 Theory of gas absorption 5

    4 Determination of HTU and NTU for various packing

    Experimental Procedure

    Precautions to be followed

    Experimental Observations

    Sample Calculations

    Error Analysis

    7

    5 Design of packed tower using different packing

    Introduction

    Theoretical Predictions of model

    Experimental Observations

    16

    6 Design of optimum packed

    Introduction Matlab Code for finding out the optimal packing

    Experimental Observations

    18

    7 Results and discussion 24

    8 Suggestions for improvement 24

    9 References 25

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    Acknowledgements

    First of all, we would like to thank Dr. A. Kannan and Dr. R. Ramnarayan for giving us

    an opportunity to design our own experiment. And at the end of it, we have to accept the

    fact that it was a very challenging experience and but for their constant guidance and

    support the project couldnt have been completed. To have come up with not only an

    experiment but to also have put forth a general strategy to design packed towers has

    indeed been a very thrilling and satisfying experience. We would also like to that Dr.

    Krishnamurthy and Mr. Meghanathan of the Chemical Engineering Workshop

    Laboratory who were very patient and helpful throughout the course of this project.

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    Introduction

    Gas absorption is one of the major mass transfer unit operations used in the separation or

    purification of gas mixtures. The operation is carried out by contacting the gas with a

    liquid solvent, usually in a packed or plate column. The dissolved solute is frequently

    recovered by thermal "desorption" or "stripping", and the regenerated solvent is recycled

    to the absorption column.

    Among major industrial uses are the absorption of SO3 in oleum in the production of

    H2SO4, and of HCl and NO2 in water in hydrochloric and nitric acid manufacturing.

    Another major application is the purification of various process streams to prevent

    pollution, corrosion, catalyst poisoning or condensation in subsequent low temperature

    treatment. Examples of these applications are the large scale removal of CO2 from air or

    natural gas prior to liquefaction, absorption of sulphur compounds from natural gas and

    CO2 removal from ammonia synthesis gas.

    A packed bed is a hollow tube or pipe that is filled with a packing material. The packing

    can be randomly filled small objects like Raschig rings or else it can be a specifically

    designed structured packing.

    The purpose of a packed bed is typically to improve contact between two phases in a

    chemical or similar process. Packed beds can be used in a chemical reactor, distillation

    process, or a scrubber, but packed beds have also been used to store heat in chemical

    plants. In this case, hot gases are allowed to escape through a vessel that is packed with a

    refractory material until the packing is hot. Air or other cool gas is then fed back to the

    plant through the hot bed, thereby pre-heating the gas feed.

    Distillation columns with packing are often called packed columns. Columns used in

    certain types of chromatography consisting of a tube filled with packing material can also

    be called packed columns and their structure has similarities to packed beds.

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    A packed column is usually favorable, when

    1. Only a small pressure drop is allowed in the column (for example in vacuum

    columns).

    2. The components are corrosive.

    3. The diameter of the column is small (below 1 m).

    4. The hold-up must be small (for example due to thermal decomposition).

    5. The liquid foams.

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    Brief outline of issues tackled in this project

    1. Study the mass transfer from gas to liquid phase in a tower filled with random

    packing.

    2. Explore how changing the water flow rate affects absorption. Carbon dioxide gas

    flow rate is fixed.

    3. What are the HTU and NTU for this condition?

    4. Compare the changes in gas absorption arising due to using different kind of

    packing.

    5. Study the performance of a tower having different packing of various heights.

    6. Optimize the tower packing so as to reduce the cost of packing used.

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    7

    Theory of Gas Absorption

    The simpler theoretical equations for gas absorbers serve three main purposes:

    They are used to "design" the column, i.e., to find the height of a column necessary to

    achieve a given separation.

    They are used in adapting an existing column to a new process or to new operating

    conditions. The problem might then be: what flow rates should be used to achieve a given

    separation, knowing the mass transfer and equilibrium characteristics of the system?

    Finally, they can be used to evaluate the mass transfer characteristics themselves from

    measured concentrations and flow rates. The experiment described here falls in this

    category.

    In all the three cases, what is needed is an equation relating all the system variables, i.e.:

    Concentration=f(height of column, flow rates, mass transfer rate, feed concentration)

    Since CO2

    is sparingly soluble in water, operation of the scrubbing column requires large

    water to air flow rate (L/V) ratio. If the L/V ratio is too small, the flow rate of CO2

    in the

    effluent gas stream will be almost the same as in the incoming gas stream and the

    operating line will appear to be almost horizontal. To achieve a large L/V ratio, operate at

    low gas flow rates and CO2

    concentrations. Under these conditions, the concentration of

    CO2

    in the effluent gas stream will be significantly smaller than in the incoming gas

    stream.

    Let

    a is the interfacial area per unit volume (m2/m

    3)

    c* is the solubility of CO2 in water at 250C (mol/l)

    c is the bulk concentration in the differential element (mol/ l)

    dZ is the differential length of the column taken for consideration (in m)

    S is the cross sectional area (m2)

    Co is the concentration of CO2 in the output liquid stream (mol/ l)

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    L is the liquid flow rate (m3/hr)

    Ka is the liquid phase mass transfer coefficient (in m/hr)

    L dC= S a dZ Ka (c - c*)

    co

    a cc

    dc

    aKS

    LZ

    0*

    Z = HTU X NTU

    NTU = co

    ccdc

    0*

    and HTU =aKaS

    L**

    HTU values generally vary with gas and liquid flow rates, going through a minimum and

    rising again as flooding conditions are approached. In order to reduce the tower cost, it is

    advantageous to operate near this minimum, and one of the objectives of the present

    experiment is to study the variation of HTU with L to establish the region of optimum

    operation. In addition, the experiment provides an opportunity to test various mass

    transfer concepts and design procedures taught in mass transfer courses.

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    DETERMINATION OF HTU AND NTU FOR VARIOUS PACKINGS

    Experimental Procedure

    Start up

    1. Switch on the CO2

    heater and heat it for about an hour or so so as to prevent cold

    carbon dioxide from damaging the pipes.

    2. Prepare 0.05N NaOH solution in distilled water. For preparing a 0.05N solution,

    weigh out NaOH (1g for 500 ml) in a beaker and add distilled water (500 ml) in it

    and stir the beaker to get a uniform solution.

    Building the Column

    1. Disconnect all the pipes connecting the tower to the water and the gas supplies.

    2. Unscrew the nuts and bolts using a spanner.

    3. Empty the earlier packing, and then fix the tower back to its original place.

    4. Fill the tower with the desired packing. Use a wire gauze to make the flow of

    fluids more uniform.

    5. Screw back the nuts and bolts using a spanner.

    6. Connect the supply lines, and test the tower for any leakages. If there are no

    leakages then we can go ahead with the next stage of the experiment.

    7. Before starting the experiment, the water flow is turned on full to allow air

    bubbles to escape, and to clean the column.

    Mass transfer process

    1. Open the appropriate valves to start CO2

    gas flow to the system. Control the CO2

    flow rate using the valve.

    2. Similarly adjust the liquid flow meter.

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    3. Meanwhile when the system reaches steady state take a sample of the output

    liquid stream.

    4. Titrate known volume of the sample against 0.05N NaOH solution using

    phenolphthalein as indicator.

    5. Repeat the procedure for different liquid flow rates.

    Shut down

    1. Turn off water flow to the system by closing the water valve

    2. Close the CO2

    gas cylinder. Check that the pressure gauges on the cylinder read

    zero.

    3. Close all valves on the CO2

    inlet line, starting from the gas cylinder and working

    up to the flow meter.

    4. Unplug the CO2

    gas heater.

    Precautions to be followed

    1. All the apparatus should be rinsed with distilled water and dried before every

    titration.

    2. System should be allowed to reach steady state for every reading.

    3. Liquid flow rates tend to fluctuate quite a lot, and so care must be taken to ensure

    that it is reasonably constant.

    4. During titration, the indicator must be added in minimal quantities.

    5. Do not leave pressure in lines after shut down.

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    Experimental Observations

    Gas Rate=2.5m3/hr

    Height Z=0.9m

    C*=0.0329

    Data for rashcig rings

    Water Flow

    Rate(LPH)

    Initial

    Volume(ml)

    Final

    Volume(ml)

    Volume of base

    required(ml)

    Concentration

    of CO2 (M) NTU HTU(m)

    30 0 3.2 3.20.0020 0.0566 15.8958

    50 8 13 50.0031 0.0937 9.6045

    70 13 16.2 3.20.0020 0.0566 15.8958

    Variation of NTU with liquid flow rate

    0.0000

    0.0200

    0.0400

    0.0600

    0.0800

    0.1000

    0 20 40 60 80

    Liquid flow rate(l/hr)

    NTU(m)

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    Data for spherical packing (7 mm dia)

    Water Flow

    Rate(LPH)

    Initial

    Volume(ml)

    Final

    Volume(ml)

    Volume of base

    required(ml)

    Concentration

    of CO2 (M) NTU HTU(m)

    30 16.3 19.3 30.0019 0.0526 17.1162

    50 19.3 24.8 5.50.0034 0.1043 8.6325

    70 24.8 29.3 4.50.0028 0.0833 10.8088

    Variation of NTU with liquid flow rate

    0.0000

    0.0500

    0.1000

    0.1500

    0 20 40 60 80

    Liquid flow rate(l/hr)

    NTU(m)

    Data for spherical packing (4 mm dia)

    Water Flow

    Rate(LPH)

    Initial

    Volume(ml)

    Final

    Volume(ml)

    Volume of base

    required(ml)

    Concentration

    of CO2 (M) NTU HTU(m)30 29.3 33.5 4.2

    0.0026 0.0771 11.680350 33.5 39.8 6.3

    0.0039 0.1214 7.415170 39.8 44.6 4.8

    0.0030 0.0895 10.0540

    Variation of NTU with liquid flow rate

    0.0000

    0.0500

    0.1000

    0.1500

    0 20 40 60 80

    Liquid flow rate(l/hr)

    NTU(m)

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    Data for plastic pall ring

    Water Flow

    Rate(LPH)

    Initial

    Volume(ml)

    Final

    Volume(ml)

    Volume of base

    required(ml)

    Concentration

    of CO2 (M) NTU HTU(m)

    30 1 2.9 1.90.0024 0.0688 13.0759

    50 3.4 4.2 0.80.0010 0.0248 36.3356

    70 4.8 5.8 10.0013 0.0326 27.5761

    Variation of NTU with liquid flow rate

    0.00000.0200

    0.0400

    0.0600

    0.0800

    0 20 40 60 80

    Liquid flow rate(l/hr)

    NTU(m)

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    Sample Calculations

    Solubility of CO2 in water at 250C (c*) = 0.0329 mol/l

    The conc. of CO2 in inlet water flow rate = 0.0002 mol/l

    The following chemical reaction is assumed to take place without any side reactions:

    CO2 + 2 NaOH Na2CO3 + H2O

    Mole/litre of CO2 = oBB Cmlsample

    NV

    )(2

    VB = 1.9 ml

    NB = 0.05 N

    Sample volume = 20 ml

    Concentration of CO2 = 0.0022

    NTU =*

    C

    Co

    dc

    c c =*

    ln*

    oc c

    c c

    = 0.0631

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    SAMPLE ERROR ANALYSIS

    1 1 2 2

    101 1

    1 1 10

    1 1 2

    1 1 2

    ,

    N V N V

    dVdN dW

    N W V

    dN dV dV dCThus

    C N V V

    Where C is Concentration of CO2

    100dC

    C =

    0.0001 10 0.1 1100

    1 1000 3.2 20

    =9.135

    ln

    1

    ln

    CNTUC C

    dNTU dC

    NTU CC C

    C C

    100dNTU

    NTU =

    0.004 9.135 1

    0.03290.0329 0.004ln

    0.0329 0.004

    =9.7535

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    DESIGN OF A PACKED TOWER WITH MIXED PACKINGS

    The above set of experiments gives us an idea of the absorption characteristics of a

    packed tower when the tower is filled with one kind of packing only. In the next stage,

    we study the effect of packing the tower with different kinds of packing and observing

    whether the process of gas absorption follows the same relationship as earlier or whether

    it is different. Differences could arise due to change in flow characteristics, etc.

    Discounting any such effects, the theory behind such an experiment would follow

    analogously.

    1HTU

    k

    * /

    1

    * /

    2

    * /

    1

    * /

    2

    *

    1 1 *

    1

    *

    12 2 *

    2

    *

    1

    *

    ln( )

    ln( )

    ln( )

    ln( )

    ln( )nn n

    n

    C Cz

    HTU C C

    C Ckz

    C C

    Ck z

    C C

    C Ck z

    C C

    C Ck z

    C C

    So if different packing materials were to be stacked upon each other in the tower, then thenet effect of the entire tower will be described as

    * **11

    1 1 2 2 * * *

    1 2

    ..... ln( ) ln( )...... ln( )o nn n

    n

    C C C C C Ck z k z k z

    C C C C C C

    * **

    11

    * * *

    1 2

    ln( . ....... )o n

    n

    C C C C C C

    C C C C C C

    *

    *ln( )o

    n

    C C

    C C

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    Additionally, we have a constraint on the height of packing:

    1 2 3.....

    nz z z z Z

    Summarily,

    1

    *

    *1

    ln ( )

    0

    n

    i

    i

    no

    i i

    i n

    i

    z Z

    C Ck z

    C C

    z Z

    Thus, if we choose zi such that they add up to the height of tower, then the final outlet

    concentration can be obtained from the second relation. The values of HTU for each of

    the packing were obtained in the first part of the project and with the assumptions that wehave made, their values can be used here too. In effect, packing a tower with different

    materials is equivalent to passing it through towers of height zi. In order to verify our

    model, we performed an experiment with different packing materials and the results of

    that experiment are described in the next section.

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    Experimental Observations

    Gas Rate=2.5m3/hr

    Height Z=0.9m

    C*=0.0329 M

    Individual heights of each packing = 0.225m

    Predicted final concentration is given by the relation:

    * **

    111 1 2 2 * * *

    1 2

    ..... ln( ) ln( )...... ln( )o nn n

    n

    C C C C C Ck z k z k z

    C C C C C C

    *

    *ln( )o

    n

    C C

    C C

    Thus, Cn=0.0021

    Actual experimental data:

    Water Flow

    Rate(LPH)

    Initial

    Volume(ml)

    Final

    Volume(ml)

    Volume of base

    required(ml)

    Concentration of

    CO2 (M) NTU HTU(m)

    7016.5 18.6 2.1 0.0026 0.0771 11.6803

    The difference between experiment and actual values of outlet concentrations of carbon

    dioxide turn out be 12%. This may seem too large an error, but one has to take into

    account the fact that an error of 10% is possible due to limit on the accuracy of the

    apparatus itself. It is very much possible that with better apparatus, the theoretical and

    experimental results would match very well. From the experiment, it can be seen that

    packing a tower with various materials is equivalent to, with reasonable accuracy, a group

    of tower filled with a single kind of packing material. This finding can be used to design

    towers with different kinds of packing materials so as to minimize the total cost of

    packing. This is exactly what is done in the section that follows.

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    DESIGN OF AN OPTIMUM PACKED TOWER

    Before we discuss the details of the experiment, it is necessary to understand the

    interpretation of optimum for there are several ways in which a packed tower could be

    optimized. In our case, we shall propose a strategy that can be used to absorb some

    desired amount of gas while minimizing the total cost of the packing used. This is

    because different packing materials have different costs and contacting properties and so

    we can neither go in for the material which provides the best contacting, since the cost o f

    the material may be prohibitive, nor the cheapest, since that may require a very long

    tower, but settle for a compromise between the two. The basic theory comes from the

    theory behind the design of packed tower using different packing materials. Let Ci denote

    the cost per unit height of packing. By unit height we mean unit height of the same tower

    that we worked on. This can be found out by filling the tower and measuring the mass of

    packing taken and the height of the packing. Using this value of Ci, we will have an

    additional equation. So now the problem is described as follows:

    1HTU

    k

    1

    *

    *1

    ln ( )

    0

    n

    i

    i

    no

    i i

    i n

    i

    z Z

    C Ck z

    C C

    z Z

    The total cost of packing materials, C is given by:

    1 1 2 2 3 3.....

    n nC z C z C z C z C

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    We have to find out that combination of heights of packing so that C, the total cost of

    packing is minimized. As it can be seen, we have several equations and inequations, all of

    which are linear. That is to say that the above set of equations form a linear program and

    so we can use tools like Simplex to solve for the optimum cost.

    We solved the above linear program using Matlab 7 and found out the optimum tower

    heights. Then the tower was setup based on the output of this program and the absorption

    experiment was carried out using in order to verify the model put forth by us.

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    MATLAB CODE FOR FINDING OUT THE OPTIMAL PACKING

    Z=0.9; %Total height of tower

    cstar=0.0329 %Solubility

    cf=0.0024 %Desired final concentration

    ntu=log(cstar/(cstar-cf))

    %Inverse of htu for a particular experiment

    ihturaschig=0.1296

    ihtuysphere=0.1875

    ihtuwsphere=0.2013

    ihtuclock=0.0387

    %kg per metre of individual packing

    draschig=1.55

    dysphere=1.98

    dwsphere=2.39

    dclock=0.67

    %There is no inequations

    A=[]

    b=[]

    %Constraints due to effect of packing and total height of packing

    Aeq = [ihturaschig ihtuysphere ihtuwsphere ihtuclock

    1 1 1 1]

    Beq = [ ntu

    Z]

    lb=zeros(4,1); %Lower bound on the individual heights of packing

    ub=[Z; Z; Z; Z] %Upper bound on the individual heights of packing

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    %cost per kg of individual packing

    for craschig=1:100

    for cysphere=1:100

    for cwsphere=1:100

    for cclock=1:100

    %Objective function

    f =[craschig*draschig cysphere*dysphere cwsphere*dwsphere cclock*dclock]

    %The linear program

    [x, fval, exitflag, output, lambda]=linprog(f, A, b, Aeq, beq, lb, ub)

    end

    end

    end

    end

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    Experimental Observations

    The final concentration was set to 0.0024 and the program was executed. It turns out that

    the cost is minimized when 7mm dia spheres of height 0.76m and plastic pall ring of

    height 0.14m.

    Gas Rate=2.5m3/hr

    Height Z=0.9m

    C*=0.0329 M

    Water Flow

    Rate(LPH)

    Initial

    Volume(ml)

    Final

    Volume(ml)

    Volume of base

    required(ml)

    Concentration

    of CO2 (M) NTU HTU(m)

    70 37.5 39.6 2.1 0.0026 0.0771 11.6803

    The difference between experiment and actual values of outlet concentrations of

    carbon dioxide turn out be 12%. This may seem too large an error, but one has to take

    into account the fact that an error of 10% is possible due to limit on the accuracy of the

    apparatus itself. It is very much possible that with better apparatus, the theoretical and

    experimental results would match very well. From the experiment, it can be seen that

    packing a tower with various materials is equivalent to, with reasonable accuracy, a group

    of tower filled with a single kind of packing material. This finding can be used to design

    towers with different kinds of packing materials so as to minimize the total cost of

    packing. This is exactly what is done in the section that follows.

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    Results and Discussions

    1. The gas absorption process in a packed tower was studied for various packing

    materials at constant gas flow rate but varying liquid flow rates were studied.

    2. The NTU vs. liquid flow rate curve goes through a minimum and then rises for all

    but one packing for which the trend is the opposite.

    3. The tower was filled with packing of different kinds and the process of gas

    absorption studied. It turn out that filling a tower with different packing is

    equivalent to carrying the gas absorption in different towers but consisting of

    single packing only.

    4. Based on the results obtained, we proposed a method to fill the tower so as to

    minimize the total cost of materials used. This is a simple linear program for

    which numerous techniques exist and can readily be solved using tools such as

    Matlab.

    5. One must remember that these results were observed for carbon dioxide gas,

    which is sparingly soluble in water. Had a more soluble gas been taken, then we

    may not have obtained results that match with predictions so well.

    Suggestions for Improvement

    1. Keep all the flow rates constant. Explore how water temperature affects

    absorption.

    2. Using gases other than carbon dioxide, perhaps even a mixture of gases.

    3. The effect of increasing Z on HTU, NTU, and outlet solute concentrations

    4. Relationship between the height of the packed column and the rate of absorption

    5. The characteristics of flooding point can be studied using this setup.

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    References

    1. Treybal R.E. (1981). Mass Transfer Operations (3rd

    Edition). McGraw-Hill, New

    York.


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