Thermodynamic - Unit Operations - Lecture Slides, Slides of Engineering Chemistry

Multicomponent Distillation, Mass transport theories , Principles of adsorption , Principles of humidification , Principles of drying are main topics covered in this Unit Operations course. This lecture covers following points: Rigourous Methods, Distillation Process, Thermodynamic System, Equilibrium Stage, Material Balance Equations, Equilibrium Relations, Degrees of Freedom Analysis, Design Strategy, Stage Efficiency Analysis, Thermodynamics Data

Typology: Slides

2012/2013

Uploaded on 08/30/2013

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Thermodynamic relations:
Simplified models
Raoult’s law (Ideal solution/ideal gas):
s
iii Pxp pi is the partial pressure of component i
Dalton’s law (Ideal gas):
Pyp ii
Composition and K-value for ideal gas/ideal solution system:
PPxyK s
iiii //
Relative volatility for ideal gas/ideal solution system:
s
j
s
iji PPKK //
Antoine equation:
i
i
i
s
iCT
B
ATP
)(ln
T, P
V
L
PxPy i
s
ii /
P is total pressure in the system
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Thermodynamic relations:Simplified models^ Raoult’s law (Ideal solution/ideal gas):

s ii i^

Px

p^ 

p^ is the partial pressure of component i^

i

Dalton’s law (Ideal gas):

Py

p^

i

i Composition and K-value for ideal gas/ideal solution system:

P P x y K^

s i i i i^

/ /^

 

Relative volatility for ideal gas/ideal solution system:

s j s i j i^

P

P

K

K^

/^

Antoine equation:

i^ i i s i

C B T A TP

  ) ( ln

T, P

V L

P

xP

y^

s ii i^

P^ is total pressure in the system

Thermodynamic relations:Simplified models^ Henry’s law:

i i i^

xT H p^

)( ^

H(T) is the Henry’s constant

Dalton’s law (Ideal gas):

Py

p^

i

i Composition and K-value:

P T H x y K^

i i i i^

/) ( /^

 

Relative volatility in the Henry’s law regime:

/^

T

H

T

H

K

K^

j i j i^

T, P

V L

P xT H y^

i i i^

/ )( 

P^ is total pressure in the system

1. Absorption: Design considerations Limiting conditions: Gas-liquid ratio; straight operating and equilibrium lines Condition

: L, V constant -> L/V constant, y

=mxe^

e

This is possible for very dilute (<3% mole fraction) mixturesso change in total number of moles of each flow isinsignificant and the region of interest is in the Henry’s law regimeA) Limiting (L/V)

value:min^

y

x

(mole fraction of A in L)

(mole fraction of A in V) xa

xb

yb ya

equilibrium line

x*^ b

B) Number of ideal stages: can be calculatedanalytically

a b

a b a b

a b

a a b b

x m y

y y x x

y y L V

Lx V Vy Lx V y

^        

 

/

    • min

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1. Kremser equation: the number of idealstages

^

A

y

y

y

y

N^

a
a
b
b

ln

ln^

*^
n
n
e
e^

mx

y

mx

y^

^

Straight equilibrium line

const mVL A^

 ^

/^

Adsorption factor, straight operating line

The Kremser equation (1930)

y

x

(mole fraction of A in L)

x^ a^

xb

equilibrium line

yb y^ b yb y^ b

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2. Thermodynamic calculations using K-values^ Bubble pointProcedure:

a) Select Tb) K
(T)i
c) d) if^
T is too high

 e) Adjusting Tg) Final composition can be corrected using i

xii K

(^1) 

i

xii K

^ ^ i

i ii i i^

x xK K y

2. Thermodynamic calculations using K-valuesDew

point

  • Model system: binary mixture A, B- Consider the process in the figure: we start witha mixture of composition 1 and temperature T

1

and start decreasing the temperature- As we decrease the temperature we are going toreach a point where the first drop of liquid forms- The liquid in the droplet obeys:- On the other hand:- Thus as we decrease the temperature we put newK-values the above equation until this condition is met

^

B
A^

y

y

^

B
A^

x

x

/^

^

T

K

y

T

K

y^

B
B
A
A

T^

V

L

2. Isothermal multicomponent flash separation

D Dhyi^ D^

, ,

F F F F i^

T P h zF

, , , ,

,T^11 P

Objective: find D, B, andtheir compositions

B Bhxi^ B^

, ,

) 1 ( 1

 

F i^ i i^

z K x

) 1 ( 1

 

F ii i i^

zK K y

  ^

  

 ^

i^

i i F i i i i i

K K z y x^

0 ) 1 ( 1

) (^1) ( 

2. Multicomponent flash separation (Adiabatic)

B hxi B^

, ,

D hyi D^

, ,

F F F F i^

T P h zF

, , , ,

,T^11 P

  • Liquid feed is heated under pressure and then adiabatically flashed throughthe pressure reducing valve

F T F

T

P

P^1 ^1

F i
i
i^

Fz Dy Bx^

 

F D B^

 

F
D
B^

Fh Dh Bh

 ^

0

) (^1) (^

   ^

F
D
B^

h h h

 

2. Fenske Equation: binary case

1

ln

)] (^1) ( /) (^1) ( ln[ min^

 

AB

D B B D^

x x x x

N

Fenske equation

2. Limiting cases: minimum reflux

D

n

n^

x

R

x

R R

y^

1

y

x

zf

zf

xB^

xD

y1 yB

xN

At this point: x
=x* and yn
=y*n+^

x*

y*

* min

min

min min

x

y

y

x

R

x

R

x

R R

y

D

D

^ 

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2. Fenske equation for multicomponentdistillations: any stages/any componentsAssumption: relative volatilities of components remain constantthroughout the column

ji

jN jn n i in Nn

x x x x

N

,

, ,

, ,

min^

ln ln^

min

min^ 

  

   

i – light componentj – heavy component

)(^ )(

,^

T

K

T

K

T

i j

ji

2. Fenske equation for multicomponentdistillations

)(^ )(

,^

T

K

T

K

T

LK HK

HKLK

Choices for relative volatility: 

D B

T

1) Relative volatility at saturated feed condition

,^

F F HKLK

THK

LK

^

2) Geometric mean relative volatility

(^

,

,

,^

B B D D HKLK

T

T^

HKLK

HKLK

^

^3

,^

(^

,

,

,^

B B D D F F

HKLK

T

T

T^

HKLK

HKLK

HKLK

^

why geometric mean?

2. Gilliland correlation: Number of idealplates at the operating reflux

   

  

    

1

min 1

D

Dm D R

R Rf

NN N

2. Complete short cut design:Fenske-Underwood-Gilliland methodGiven a multicomponent distillation problem:

a) Identify light and heavy key componentsb) Guess splits of the non-key components and compositionsof the distillate and bottoms productsc) Calculated) Use Fenske equation to find Nmine) Calculate distribution of non key componentsf) Use Underwood method to find R

Dm

g) Use Gilliland correlation to find actual number of ideal stagesgiven operating refluxh) Use Kirkbride equation to locate the feed stage

HKLK , 