Destilación de azeotropo

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     Azeotropic Distillation

    Problem & solution principle

    Ethanol cannot be obtained through simple distillation from an ethanol-water mixture because

    of an azeotrope.

    Different methods are available for this purpose. Here we will introduce azeotropic distillation

    using n-pentane as entrainer (see fig. 1).

    In a pre-treatment step, an ethanol-water mixture is concentrated to approx. 90% ethanol

    content (see fig. 1, column 1).

    Afterwards, the mixture is fed to a column together with the n-pentane, which results in a low-

    boiling ternary in the head (see fig. 1, column 2) that disintegrates into two liquid phases after

    condensation.

    The wet phase is then discharged into a flash and the arid phase returned to the column (see

    fig. 1, flash 5).

    Through formation of the ternary azeotrope and expulsion of the water, the ethanol turns into

    a high boiler and can be removed from column 2 in almost pure form as bottom component.

    Entrainer residues are removed from the water in column 4 and discharged afterwards.

    Figure 1 Flow sheet of azeotropic distillation 

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    Figure 2 Residue curves/binodal plot

    In the next step, the bottom component of column 1 is fed into column 2 together with the

    entrainer n-pentane. In this process, a mixture compound forms in proximity to the ternary

    azeotropic point (green arrow tip, arrow 3).

    In the downstream flash, the condensed distillate stream then disintegrates into two liquid

    phases along the conode, due to the miscibility gap (blue arrow tips, arrow 4).

    The organic phase (arrow 4a) is added again to the second column, which results in a

    concentration shift of the ternary mixture across the distillation boundary (see [II] De Filliers,

    French, Koplos; 2002). The distillation boundary progresses along the residue curves, starting at

    the binary azeotropic points towards the ternary azeotrope. This way, after reflux of the recycle

    stream of the organic phase, the material system is located in the distillation section limited bythe points binary azeotrope ethanol-n-pentane, pure ethanol and ternary azeotrope (see [I] 

    Ulrich; 14 et seq.).

    Almost dry ethanol can now be extracted from column 2 as the bottom component (violet

    arrow tip, arrow 5).

    The wet part of the second phase (arrow 4b) in the flash is cleaned in a third distillation column

    (see fig. 1, column 4), so that pure water can be extracted as bottom component and a water-

    ethanol-n-pentane mixture as top component. This is then added to column 2 again.

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    The feed stream is defined before the columns are

    specified (see fig. 3).

    The pressure is set to 1 bar and the temperature to

    30°C. The feed concentration is selected arbitrarily in

    the first distillation section (azeotropic point

    water/ethanol - ternary azeotrope - pure water). The

    mass flow is set to 250

     water and 1000

     ethanol,

    which corresponds to an ethanol concentration of 61

    %.

    The feed composition can be selected with any

    ethanol content below the azeotropic point water-

    ethanol, due to the pre-treatment.

    The layout of the first column is defined after the

    feed definition. The feed stage is set to the 15th stage

    1

     at medium column height. Altogether,30 stages

    2  are simulated. With rigorous column design, numerous additional specification

    options are available, such as pressure losses, pressures or temperatures within the column

    (see fig. 4).

    As the water-ethanol mixture is supposed to be advanced as close as possible to the azeotropic

    point, the mole fraction in the distillate stream (distillate component mole fraction) is set to

    0.9, while the mole fraction in the bottom (bottom component mole fraction) is set to 0.001

    (see fig. 5).

    1 The optimum feed stage has been calculated using a shortcut column as described by Fenske-Underwood-Gilliland. As this is

    based on ideal mixtures and constant volatilities, deviations from the real optimum feed stage may occur. 2 With rigorous design, the number of stages can be selected by performing a sensitivity analysis or determining the theoreticalnumber of stages with the McCabe-Thiele diagram (see [III] Stephan, Schaber, Stephan, Mayinger; 460 et seq.). 

    Figure 3 Feed definition

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    Figure 4 Design parameters of the first column

    Figure 5 Design parameters of the first column

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    Figure 6 Design parameters of the second column 

    The number of stages of column 2 is set to 151  (see fig. 6). The product stream of the first

    column (stream 2) is fed at stage 82, while the recycle streams 4, 5 and 7 enter the column on

    the three next higher stages.

    An ethanol mole fraction of 0.999 is set as vaporizer specification to achieve the product

    specification.

    The condenser is specified with a reflux rate of 1, due to the minimum reflux rate of 0.9152. The

    minimum value has been determined beforehand using a shortcut column.

    Alternatively, graphic definition of the minimum reflux ratio using the McCabe-Thiele diagram is

    also possible.

    1 With rigorous design, the number of stages can be selected by performing a sensitivity analysis or determining the theoretical

    number of stages with the McCabe-Thiele diagram (see [III] Stephan, Schaber, Stephan, Mayinger; 460 et seq.). 2

     The optimum feed stage as well as the minimum reflux rate have been calculated using a shortcut column as described by

    Fenske-Underwood-Gilliland. As this is based on ideal mixtures and constant volatilities, deviations from the real optimum feed

    stage or from the minimum reflux rate may occur.

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    Figure 7 Design parameters of the second column 

    Figure 8 Design parameters of the Multipurpose Flash 

    Once column 2 has been initialized, the flash mode is set to 1 in the "Multipurpose Flash" at

    [Flash Mode] (see fig. 8). A low mole vapour fraction is selected in order to completely

    condense a distillate while preventing convergence problems at the same time. The pressure

    may remain unspecified as the inlet pressure of the flash is applied.

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    In column 4, the number of stages is set to 30 and the feed stage centrally to 15

    (see fig. 9). Both parameters have been calculated using a shortcut column.

    Figure 9 Design parameters of the third column 

    Figure 10 Design parameters of the third column 

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    Due to the low n-pentane fraction of the wet phase, a water-mole concentration of 0.999 is

    selected as vaporizer specification (see fig. 10). At the same time, the distillate is concentrated

    until an ethanol concentration of 85% is achieved so that the fraction of water recycled in the

    second column is not too large.

    Once all "Unit Operations" have been entered, linked and

    specified, the start values of the cut stream (see fig. 1, stream 3)

    have to be initialized.

    The simulation can be started with "run all", and an immediate

    convergence of the "Unit Operations" as well as of the material

    streams should be achieved. In case of convergence problems

    with the recycle stream, it may be necessary to restart the

    simulation.

    Cut Stream (stream 3)

    p = 1 bar

    T = 33°C

      ̇ Water  = 100

     

      ̇ Ethanol  = 1000

     

      ̇ N-Pentane  = 20000

     

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    Assessment of the simulation results

    In order to obtain a simple overview of the material streams during the process, a list of

    characteristics of selected streams can be displayed in real time at [Format][Add Stream Box]

    (see fig. 11).

    Figure 11 Stream box with selected streams 

    The approx. 21.7

     ethanol fraction in the global feed can be removed almost dry at product

    stream 9. The process runs in a bar (absolute) here.

    The product specification has thus been achieved.

    The entrainer n-pentane is completely recycled without loss in the simulation model. In real

    operation, slight entrainer losses must be compensated for through constant addition. In

    CHEMCAD, this compensation is realized with the unit operation "Controller".

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    Optimization of azeotropic distillation

    The energy input and the type of entrainer can be optimized.

    In order to reduce the energy input, economisers can be used and the purity of the top and

    bottom components reduced. CHEMCAD provides the option to perform the sensitivity study to

    realize optimization.

    In addition, selection of a suitable entrainer can influence the energy expenditure and the

    entrainer quantity. When using cyclohexane, for example, less entrainer is required due to the

    higher ethanol fraction in the tertiary azeotrope. However, as the boiling temperatures of the

    tertiary azeotropes as well as the impacts of the different organic substances on the

    environment vary, a suitable compromise must be found in practice. Benzol, for example, is nolonger used due to its high degree of toxicity despite its good entrainer characteristics.

    Usually, the activity coefficients at infinite dilution are determined first when selecting a

    suitable entrainer, and the effects on the relative volatility of the substances to be separated

    are investigated (see [IV] Gmehling, Kolbe, Kleiber, Rarey; 2012; 512 pp.).

    The simulation discussed in this document was generated in CHEMCAD 6.5.3 and can be used

    with all versions as of CHEMCAD 5.

    Are you interested in further tutorials, seminars or other solutions with CHEMCAD?

    Then please contact us:

    Mail: [email protected] 

    Phone: +49 (0)30 20 200 600

    www.chemstations.eu 

    Authors:

    Daniel Seidl

    Meik Wusterhausen

    Armin Fricke

    Sources

    mailto:[email protected]:[email protected]:[email protected]://www.chemstations.eu/en/tutoriallphttp://www.chemstations.eu/en/tutoriallphttp://www.chemstations.eu/en/tutoriallpmailto:[email protected]://www.chemstations.eu/en/tutoriallp

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    I. 

    Ulrich, Jan"Operation and Control of Azeotropic Distillation Column Sequences"

    Diss. ETH No. 14890, Swiss Federal Institute of Technology, Zurich, 2002

    II.  De Villiers, French, Koplos

    "Navigate Phase Equilibria via Residue Curve Maps"

    2002, http://people.clarkson.edu/~wwilcox/Design/rescurve.pdf  

    (Accessed on 10.09.2013)

    III.  Stephan, Schaber, Stephan, Mayinger

    "Thermodynamik"

    Band 2 Mehrstoffsysteme und chemische Reaktionen, 15th edition, Springer

    IV.  Gmehling, Kolbe, Kleiber, Rarey

    "Chemical Thermodynamics for Process Simulation"

    2012, Wiley-VCH

    http://people.clarkson.edu/~wwilcox/Design/rescurve.pdfhttp://people.clarkson.edu/~wwilcox/Design/rescurve.pdfhttp://people.clarkson.edu/~wwilcox/Design/rescurve.pdfhttp://people.clarkson.edu/~wwilcox/Design/rescurve.pdfhttp://www.chemstations.eu/en/tutoriallp