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Separation Process-II
(ChE-306)
1
Ponchon-Savarit Method
β€’ For non-ideal systems
β€’ Molar latent heat is no more constant
β€’ Heat of mixing will be non-zero
β€’ Enthalpy balance
β€’ Using an Enthalpy-Composition diagram
β€’ Phase
A quantity of mixture in any physical
state.
β€’ Phase C between the boiling point
and dew point curve will be:
π‘šπ΄
π‘šπ΅
=
𝐢𝐡
𝐢𝐴
β€’ Combination of phases
β€’ Separation of phases
β€’ Addition of heat
β€’ Adding the phases A and B with mass
m, composition x and H as enthalpy per
unit mass to give phase C will result:
π‘šπ΄ + π‘šπ΅ = π‘šπΆ
π‘šπ΄π‘₯𝐴 + π‘šπ΅π‘₯𝐡 = π‘šπΆπ‘₯𝐢
π‘šπ΄π»π΄ + π‘šπ΅π»π΅ = π‘šπΆπ»πΆ
β€’ If heat Q is added to A then increase in
enthalpy from A to C will be:
𝐻𝐴 +
𝑄
π‘šπ΄π΅
= 𝐻𝐢
Enthalpy balance for a continuous Distillation
Column
β€’ Feed, F (xF)
β€’ Distillate (xD)
β€’ Bottom Product (xW)
β€’ HV and HL represent enthalpy per unit mass
of vapor and liquid
β€’ QC = heat removed in condenser
β€’ QB = heat added in reboiler
Material and Heat Balance
β€’ Overall Material balance across section I
𝑉
𝑛 = 𝐿𝑛+1 + 𝐷
β€’ Material balance with respect to MVC
𝑉
𝑛𝑦𝑛 = 𝐿𝑛+1π‘₯𝑛+1 + 𝐷π‘₯𝑑
β€’ Substitute the value of Vn and simplify
𝐿𝑛+1 + 𝐷 𝑦𝑛 = 𝐿𝑛+1π‘₯𝑛+1 + 𝐷π‘₯𝑑
𝐿𝑛+1
𝐷
=
π‘₯𝑑 βˆ’ 𝑦𝑛
𝑦𝑛 βˆ’ π‘₯𝑛+1
β€’ Heat Balance
𝑉
𝑛𝐻𝑛
𝑉 = 𝐿𝑛+1𝐻𝑛+1
𝐿
+ 𝐷𝐻𝑑
𝐿
+ 𝑄𝑐
β€’ Putting 𝐻𝑑
β€²
= 𝐻𝑑
𝐿
+
𝑄𝐢
𝐷
the above equation will simplify to:
𝑉
𝑛𝐻𝑛
𝑉 = 𝐿𝑛+1𝐻𝑛+1
𝐿
+ 𝐷𝐻𝑑
β€²
β€’ Substitute the value of Vn from first equation and simplify
𝐿𝑛+1
𝐷
=
𝐻𝑑
β€²
βˆ’ 𝐻𝑛
𝑉
𝐻𝑛
𝑉
βˆ’ 𝐻𝑛+1
𝐿
𝐿𝑛+1
𝐷
=
π‘₯𝑑 βˆ’ 𝑦𝑛
𝑦𝑛 βˆ’ π‘₯𝑛+1
𝐿𝑛+1
𝐷
=
𝐻𝑑
β€²
βˆ’ 𝐻𝑛
𝑉
𝐻𝑛
𝑉
βˆ’ 𝐻𝑛+1
𝐿
As left hand sides are same so equating right hand sides
𝐻𝑑
β€²
βˆ’ 𝐻𝑛
𝑉
𝐻𝑛
𝑉
βˆ’ 𝐻𝑛+1
𝐿 =
π‘₯𝑑 βˆ’ 𝑦𝑛
𝑦𝑛 βˆ’ π‘₯𝑛+1
Simplification gives:
𝑦𝑛 =
𝐻𝑑
β€²
βˆ’ 𝐻𝑛
𝑉
𝐻𝑛
𝑉
βˆ’ 𝐻𝑛+1
𝐿 π‘₯𝑛+1 +
𝐻𝑛
𝑉 βˆ’ 𝐻𝑛+1
𝐿
𝐻𝑑
β€²
βˆ’ 𝐻𝑛+1
𝐿 π‘₯𝑑
β€’ Equation of top operating line
β€’ Relation between the compositions of vapor and liquid streams
between any two plates
β€’ The line passes through a common pole N of coordinates (xd , Hd’)
β€’ Overall Material balance across section II
πΏπ‘š = 𝑉
π‘š + π‘Š
β€’ Material balance with respect to MVC
βˆ’π‘‰
π‘šπ‘¦π‘š + πΏπ‘šπ‘₯π‘š+1 = π‘Šπ‘₯𝑀
β€’ Substitute the value of Vm and simplify
πΏπ‘š+1
π‘Š
=
βˆ’π‘₯π‘Š + π‘¦π‘š
π‘¦π‘š βˆ’ π‘₯π‘š+1
9
β€’ Heat Balance
βˆ’π‘‰
π‘šπ»π‘š
𝑉 + πΏπ‘š+1π»π‘š+1
𝐿
= π‘Šπ»π‘Š
𝐿
βˆ’ 𝑄𝐡
β€’ Putting π»π‘Š
β€²
= π»π‘Š
𝐿
βˆ’
𝑄𝐡
π‘Š
the above equation will simplify to:
βˆ’π‘‰
π‘šπ»π‘š
𝑉
+ πΏπ‘š+1π»π‘š+1
𝐿
= π‘Šπ»π‘Š
β€²
Substitute the value of Vm from first equation and simplify
πΏπ‘š+1
π‘Š
=
π»π‘Š
β€²
+ π»π‘š
𝑉
π»π‘š
𝑉
βˆ’ π»π‘š+1
𝐿
πΏπ‘š+1
π‘Š
=
βˆ’π‘₯π‘Š+π‘¦π‘š
π‘¦π‘šβˆ’π‘₯π‘š+1
πΏπ‘š+1
π‘Š
=
π»π‘Š
β€²
+π»π‘š
𝑉
π»π‘š
𝑉 βˆ’π»π‘š+1
𝐿
βˆ’π‘₯π‘Š + π‘¦π‘š
π‘¦π‘š βˆ’ π‘₯π‘š+1
=
π»π‘Š
β€²
+ π»π‘š
𝑉
π»π‘š
𝑉
βˆ’ π»π‘š+1
𝐿
β€’ Equation of operating line below the feed plate
β€’ Line passes through pole M of coordinates (xW ,
HW’)
β€’ Overall sum of phases
𝐹 = 𝑀 + 𝑁
𝐹π‘₯𝐹 = 𝑀π‘₯π‘Š + 𝑁π‘₯𝑑
β€’ Phases F, M and N lie on a straight line.
Determination of number of plates on H-x
diagram
β€’ Locate xd, xf and xw
β€’ Locate pole N
β€’ Join N to F
β€’ Extend backwards till xw, this will give pole M
β€’ Starting from pole N, draw the lines to get the vapor and liquid
compositions on each plate
β€’ Switch to pole M, when feed composition xf is crossed
β€’ Draw the tie lines to count steps
β€’ Stop when composition reached to xw
β€’ Feed plate will be the one where the pole has been switched from N to M
L1
L2
L3
V1
V2
V3
Self Study
β€’ Example 11.10

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Distillation Column-Pohnchon savrit method.pptx

  • 2. Ponchon-Savarit Method β€’ For non-ideal systems β€’ Molar latent heat is no more constant β€’ Heat of mixing will be non-zero β€’ Enthalpy balance β€’ Using an Enthalpy-Composition diagram
  • 3. β€’ Phase A quantity of mixture in any physical state. β€’ Phase C between the boiling point and dew point curve will be: π‘šπ΄ π‘šπ΅ = 𝐢𝐡 𝐢𝐴
  • 4. β€’ Combination of phases β€’ Separation of phases β€’ Addition of heat β€’ Adding the phases A and B with mass m, composition x and H as enthalpy per unit mass to give phase C will result: π‘šπ΄ + π‘šπ΅ = π‘šπΆ π‘šπ΄π‘₯𝐴 + π‘šπ΅π‘₯𝐡 = π‘šπΆπ‘₯𝐢 π‘šπ΄π»π΄ + π‘šπ΅π»π΅ = π‘šπΆπ»πΆ β€’ If heat Q is added to A then increase in enthalpy from A to C will be: 𝐻𝐴 + 𝑄 π‘šπ΄π΅ = 𝐻𝐢
  • 5. Enthalpy balance for a continuous Distillation Column β€’ Feed, F (xF) β€’ Distillate (xD) β€’ Bottom Product (xW) β€’ HV and HL represent enthalpy per unit mass of vapor and liquid β€’ QC = heat removed in condenser β€’ QB = heat added in reboiler
  • 6. Material and Heat Balance β€’ Overall Material balance across section I 𝑉 𝑛 = 𝐿𝑛+1 + 𝐷 β€’ Material balance with respect to MVC 𝑉 𝑛𝑦𝑛 = 𝐿𝑛+1π‘₯𝑛+1 + 𝐷π‘₯𝑑 β€’ Substitute the value of Vn and simplify 𝐿𝑛+1 + 𝐷 𝑦𝑛 = 𝐿𝑛+1π‘₯𝑛+1 + 𝐷π‘₯𝑑 𝐿𝑛+1 𝐷 = π‘₯𝑑 βˆ’ 𝑦𝑛 𝑦𝑛 βˆ’ π‘₯𝑛+1
  • 7. β€’ Heat Balance 𝑉 𝑛𝐻𝑛 𝑉 = 𝐿𝑛+1𝐻𝑛+1 𝐿 + 𝐷𝐻𝑑 𝐿 + 𝑄𝑐 β€’ Putting 𝐻𝑑 β€² = 𝐻𝑑 𝐿 + 𝑄𝐢 𝐷 the above equation will simplify to: 𝑉 𝑛𝐻𝑛 𝑉 = 𝐿𝑛+1𝐻𝑛+1 𝐿 + 𝐷𝐻𝑑 β€² β€’ Substitute the value of Vn from first equation and simplify 𝐿𝑛+1 𝐷 = 𝐻𝑑 β€² βˆ’ 𝐻𝑛 𝑉 𝐻𝑛 𝑉 βˆ’ 𝐻𝑛+1 𝐿
  • 8. 𝐿𝑛+1 𝐷 = π‘₯𝑑 βˆ’ 𝑦𝑛 𝑦𝑛 βˆ’ π‘₯𝑛+1 𝐿𝑛+1 𝐷 = 𝐻𝑑 β€² βˆ’ 𝐻𝑛 𝑉 𝐻𝑛 𝑉 βˆ’ 𝐻𝑛+1 𝐿 As left hand sides are same so equating right hand sides 𝐻𝑑 β€² βˆ’ 𝐻𝑛 𝑉 𝐻𝑛 𝑉 βˆ’ 𝐻𝑛+1 𝐿 = π‘₯𝑑 βˆ’ 𝑦𝑛 𝑦𝑛 βˆ’ π‘₯𝑛+1 Simplification gives: 𝑦𝑛 = 𝐻𝑑 β€² βˆ’ 𝐻𝑛 𝑉 𝐻𝑛 𝑉 βˆ’ 𝐻𝑛+1 𝐿 π‘₯𝑛+1 + 𝐻𝑛 𝑉 βˆ’ 𝐻𝑛+1 𝐿 𝐻𝑑 β€² βˆ’ 𝐻𝑛+1 𝐿 π‘₯𝑑 β€’ Equation of top operating line β€’ Relation between the compositions of vapor and liquid streams between any two plates β€’ The line passes through a common pole N of coordinates (xd , Hd’)
  • 9. β€’ Overall Material balance across section II πΏπ‘š = 𝑉 π‘š + π‘Š β€’ Material balance with respect to MVC βˆ’π‘‰ π‘šπ‘¦π‘š + πΏπ‘šπ‘₯π‘š+1 = π‘Šπ‘₯𝑀 β€’ Substitute the value of Vm and simplify πΏπ‘š+1 π‘Š = βˆ’π‘₯π‘Š + π‘¦π‘š π‘¦π‘š βˆ’ π‘₯π‘š+1 9
  • 10. β€’ Heat Balance βˆ’π‘‰ π‘šπ»π‘š 𝑉 + πΏπ‘š+1π»π‘š+1 𝐿 = π‘Šπ»π‘Š 𝐿 βˆ’ 𝑄𝐡 β€’ Putting π»π‘Š β€² = π»π‘Š 𝐿 βˆ’ 𝑄𝐡 π‘Š the above equation will simplify to: βˆ’π‘‰ π‘šπ»π‘š 𝑉 + πΏπ‘š+1π»π‘š+1 𝐿 = π‘Šπ»π‘Š β€² Substitute the value of Vm from first equation and simplify πΏπ‘š+1 π‘Š = π»π‘Š β€² + π»π‘š 𝑉 π»π‘š 𝑉 βˆ’ π»π‘š+1 𝐿
  • 11. πΏπ‘š+1 π‘Š = βˆ’π‘₯π‘Š+π‘¦π‘š π‘¦π‘šβˆ’π‘₯π‘š+1 πΏπ‘š+1 π‘Š = π»π‘Š β€² +π»π‘š 𝑉 π»π‘š 𝑉 βˆ’π»π‘š+1 𝐿 βˆ’π‘₯π‘Š + π‘¦π‘š π‘¦π‘š βˆ’ π‘₯π‘š+1 = π»π‘Š β€² + π»π‘š 𝑉 π»π‘š 𝑉 βˆ’ π»π‘š+1 𝐿 β€’ Equation of operating line below the feed plate β€’ Line passes through pole M of coordinates (xW , HW’) β€’ Overall sum of phases 𝐹 = 𝑀 + 𝑁 𝐹π‘₯𝐹 = 𝑀π‘₯π‘Š + 𝑁π‘₯𝑑 β€’ Phases F, M and N lie on a straight line.
  • 12. Determination of number of plates on H-x diagram β€’ Locate xd, xf and xw β€’ Locate pole N β€’ Join N to F β€’ Extend backwards till xw, this will give pole M β€’ Starting from pole N, draw the lines to get the vapor and liquid compositions on each plate β€’ Switch to pole M, when feed composition xf is crossed β€’ Draw the tie lines to count steps β€’ Stop when composition reached to xw β€’ Feed plate will be the one where the pole has been switched from N to M
  • 14.

Editor's Notes

  1. https://www.youtube.com/watch?v=Rq9b3ovTnLA