Seader & Henley, Separation Process Principlesche.uri.edu/course/che349/distallation.pdf · Seader...

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f01_11 Seader & Henley, Separation Process Principles 1

Transcript of Seader & Henley, Separation Process Principlesche.uri.edu/course/che349/distallation.pdf · Seader...

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    Seader & Henley, Separation Process Principles 1

  • Separation Processes • Absorption – Solutes removed from a gas into a liquid

    •  Solutes removed from liquid into gas is called stripping or desorption

    •  Distillation – Thermal vapor-liquid separation processes (Ch 11); vapor phase generated from liquid

    •  Liquid-liquid extraction – Solute extracted from liquid A into an immiscible liquid B (a solvent)

    •  Leaching (extraction) – Solute extracted from a solid into a solvent phase (liquid, dense gas, or supercritical fluid)

    •  Membrane processing – Molecules separated using a dense (non-porous film) or porous physical barrier

    •  Filtration – Suspended solids separated from a liquid or gas phase using a porous membrane

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  • Methanol more volatile than water

    Pm > Pw

    Pm > 1 atm

    Vapor-liquid equilibria... (e.g. ideal, methanol-water system)

    BP diagram at const P (ideal)

    dew-point

    bubble-point

    x = y (1 component)

    x-y diagram at const P

    P (= pm + pw) diagram at const T

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    Ethanol more volatile γePe > γhPh

    Ethanol less volatile γePe < γhPh

    x = y at 58oC

    Low T

    High T

    Vapor-liquid equilibria... (e.g. non-ideal, n-hexane-ethanol system)

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  • The greater the separation between the equilibrium and 45o line, the easier the separation

    Getting into separations

    x = y

    x-y diagram at const P

    α AB =yA / xAyB / xB

    =yA / xA

    (1− yA ) /(1− xA )

    α AB =PAPB

    yA =α AB xA

    1+ (α AB −1)xAif α AB =1, yA = xA

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  • The greater the separation between the equilibrium and 45o line, the easier the separation

    Simple flash distillation (single stage; heated to T, phase split)

    x = y

    x-y diagram at const P

    F = V + LFxF = Vy + Lx∴ FxF = Vy + (F −V )x

    heater separator F, xF

    V, y

    L, x 6

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    Where liquid is stripped of A by raising vapor from reboiler Stripping section

    Binary distillation of components A & B (A is more volatile, e.g. methanol (A)-water (B) system)

    Where “cold” reflux liquid condenses some or the vapor Enriching section

    Vapor enriched

    in A

    Liquid depleted of

    A

    Near yA = 1 @ TB,A (light boiler)

    Near xB = 1 @ TB,B (high boiler)

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  • F = D+W (molar flow)FxF = DxD +WxWDF

    =xF − xWxD − xW

    , WF

    =xD − xFxD − xW

    Vm+1 = Lm −WVm+1ym+1 = Lmxm -WxW

    ym+1 =LmVm+1

    xm −WVm+1

    xW

    Vn+1 = Ln + DVn+1yn+1 = Lnxn + DxD

    yn+1 =LnVn+1

    xn −DVn+1

    xD

    W xW

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  • Approximation - Constant molal overflow

    •  Liquid and vapor flowrates are nearly constant in rectifying (top) and stripping (bottom + feed plate) sections –  Ln=Ln+1=Ln+2… Vn=Vn+1=Vn+2… –  L and V, rectifying; L and V, stripping

    •  ΔHv (condensing high boiler) ≈ ΔHv (vaporizing low boiler)

    •  Operating equations or lines are linear

    yn+1 =LnVn+1

    xn −DVn+1

    xD

    ym+1 =LmVm+1

    xm −WVm+1

    xW

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  • Variables

    •  # Plates, plate design, height of column, etc. (later)

    •  Cooling in condenser –  Liquid returned to top of column

    (reflux) •  Heating in reboiler

    –  Vapor returned to bottom of column •  Location and conditions of feed

    –  Cold? Hot? L or V or L-V?

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  • R = LnD

    =Vn+1 −D

    D (overhead product, L at B.P.)

    yn+1 =R

    R +1xn −

    1R +1

    xD

    Top plate (1) Total condenser

    Partial condenser

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  • •  Reboiler with saturated steam

    •  Condenser with cooling water

    Heating and cooling requirements

    ms =Vm+1λλ s

    λ = latent heat steamλs = latent heat vapor mixtureVm +1 = vapor flowrate from reboiler (stripping section)

    mw =Vn+1 λ

    (T2 −T1)c p,w

    cp,w = heat capacity cooling water(T2 −T1) = Temp change in cooling waterVn+1 = vapor flowrate into condensor

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  • q > 1 (sub-cooled L)

    q = 1 (@ BP)

    0 < q < 1 (L-V)

    q = 0 (@ D.P.)

    q < 0 (superheated V)

    Feed conditions

    q = moles L in stripping section from feedmoles feed

    q = HV (D.P.)−HFHV (D.P.)−HL (B.P.)

    q =(HV −HL ) + cp,L (TB −TF )

    HV −HL

    Lm = Ln + qF (stripping)Vn =Vm + (1− q)F (rectifying)

    y = q1− q

    x − 11− q

    xF13

  • McCabe-Thiele Method - # of ideal plates McCabe & Thiele, Industrial Engineering & Chemistry Research, 17 (1925) 605.

    V=L, R→∞ (total reflux)

    y=x (P=Pi at each tray)

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  • yn+1 =R

    R +1xn −

    1R +1

    xD

    xD ≡ design condition R ≡ design variable

    Rectifying section

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  • Stripping section

    ym+1 =LmVm+1

    xm −WVm+1

    xW

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  • Feed conditions (feed line)

    @ D.P.

    @ B.P.

    yn+1 =R

    R +1xn −

    1R +1

    xD

    ym+1 =LmVm+1

    xm −WVm+1

    xW

    y = q1− q

    x − 11− q

    xF

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  • Putting it all together…

    yn+1 =LnVn+1

    xn −DVn+1

    xD

    ym+1 =LmVm+1

    xm −WVm+1

    xW

    y = q1− q

    x − 11− q

    xF

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  • Stepping off stages (start at xD)

    What we want in overhead product

    What we want in bottoms product

    (start here)

    operating equilibrium

    x = xF

    4 stages + reboiler

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    x = xW

  • Minimum # of plates

    αav = (αAαB )1/ 2

    Fenske equation :

    Nm =ln xD

    (1− xD )(1− xW )xW

    lnαav*includes rebioler

    OR

    xB xD

    V=L (op lines = 45o)

    R→∞ (total reflux)

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  • Minimum reflux (occurs @ pinch point, P)

    yn+1 =R

    R +1xn −

    1R +1

    xD€

    RmRm +1

    =xD − y

    '

    xD − x'

    y ',x ' @ pinch point

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