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CHE1023
Chemical Process Calculations
Week 9 (1st session): Material Balance
Single Phase Systems
2
Single Phase Systems
Real situations:
physical properties of process materials is not readily available -
must find it:
1) literature (handbook, library or web sources)
2) estimation techniques (correlation or theory)
3) measurement (most expensive but sometimes required)
use to derive relations among system variables to solve for
unknowns
3
Single Phase Systems
Liquid and Solid Densities
• usually independent of temperature in most process
• similarly with pressure - called INCOMPRESSIBLE fluids
So how do we obtain data in absence of literature values?
4
Single Phase Systems
Liquid and Solid Densities
Estimate from component mass fractions and pure densities in 2
ways:
1. Volume additivity: thus
or
∑
= i
V
V ∑
=
i
i
w
ρ
ρ
1
∑
∑
=
=
i
i
i
i
V
x
M
x
V
M
ˆ
ˆ
ρ
5
Single Phase Systems
Liquid and Solid Densities
Estimate from component mass fractions and pure densities in 2
ways:
2. Pure components’ density average:
ρ = Σ xi ρi
6
Single Phase Systems
Gas provides more difficult ways of estimation
Ideal Gas concept is usually the best way:
• relation between specific volume and temperature and
pressure must be established
• or P,V,T relationship
7
Single Phase Systems
Ideal Gas (Perfect Gas)
Use “Equation of State” relates P,V and T.
For ideal gas the equation of state is:
PV = nRT or PV = nRT
where R is the gas constant
P = RT
= V/n ; specific molar volume
V
ˆ
V
ˆ
8
Single Phase Systems
Non-Ideal Gas
Need to put in a correction factor:
Compressibility factor:
z = 1 for ideal gases
RT
V
P
z
ˆ
=
9
Single Phase Systems
Standard conditions:
1) scientific 0oC, 1 atm
1 mol (at std. conditions) ⇒ 22,400 cm3 or 22.4 m3
1 lbmol ⇒ 359 ft3
2) natural gas industry 60oF, 14.7 psia
1 lbmol ⇒ 379 ft3
10
Single Phase Systems
Calculations: usually involve converting from one set of
conditions to another
or
1
2
1
1
2
2
ˆ
ˆ
T
T
V
P
V
P
=
1
1
2
2
1
1
2
2
T
n
T
n
V
P
V
P
=
11
Single Phase Systems
Ideal gas mixtures
Partial pressure of component A:
Note: This is used as the definition of "partial pressure", even
for non-ideal gases. It is equal to the pressure that would be
exerted if A alone occupied the container only for ideal gases.
A
A Py
p =
12
Single Phase Systems
Ideal gas mixtures
Total pressure = sum of partial pressures:
)
1
(
P
y
P
Py
P i
i =
=
= ∑
∑
13
Single Phase Systems
Ideal gas mixtures
Similarly:
Total volume = sum of partial volumes.
PV = nRT can also be written PvA= nART
where vA is partial volume of component A in a
mixture an nA is its mole fraction.
14
Single Phase Systems
Ideal gas mixtures
PvA= nART ; divide this by PV = nRT, we obtain,
vA / V = nA/n = yA
or vA = yAV
15
Single Phase Systems
Ideal gas mixtures
PvA= nART ; divide this by PV = nRT, we obtain,
vA / V = nA/n = yA
or vA = yAV (cf. pA= yAP)
16
Single Phase Systems
Ideal gas mixtures
PvA= nART ; divide this by PV = nRT, we obtain,
vA / V = nA/n = yA
or vA = yAV (cf. pA= yAP)
volume fraction = mole fraction
for ideal gases only.

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Week 9_1st session_Single Phase Systems.pdf

  • 1. CHE1023 Chemical Process Calculations Week 9 (1st session): Material Balance Single Phase Systems
  • 2. 2 Single Phase Systems Real situations: physical properties of process materials is not readily available - must find it: 1) literature (handbook, library or web sources) 2) estimation techniques (correlation or theory) 3) measurement (most expensive but sometimes required) use to derive relations among system variables to solve for unknowns
  • 3. 3 Single Phase Systems Liquid and Solid Densities • usually independent of temperature in most process • similarly with pressure - called INCOMPRESSIBLE fluids So how do we obtain data in absence of literature values?
  • 4. 4 Single Phase Systems Liquid and Solid Densities Estimate from component mass fractions and pure densities in 2 ways: 1. Volume additivity: thus or ∑ = i V V ∑ = i i w ρ ρ 1 ∑ ∑ = = i i i i V x M x V M ˆ ˆ ρ
  • 5. 5 Single Phase Systems Liquid and Solid Densities Estimate from component mass fractions and pure densities in 2 ways: 2. Pure components’ density average: ρ = Σ xi ρi
  • 6. 6 Single Phase Systems Gas provides more difficult ways of estimation Ideal Gas concept is usually the best way: • relation between specific volume and temperature and pressure must be established • or P,V,T relationship
  • 7. 7 Single Phase Systems Ideal Gas (Perfect Gas) Use “Equation of State” relates P,V and T. For ideal gas the equation of state is: PV = nRT or PV = nRT where R is the gas constant P = RT = V/n ; specific molar volume V ˆ V ˆ
  • 8. 8 Single Phase Systems Non-Ideal Gas Need to put in a correction factor: Compressibility factor: z = 1 for ideal gases RT V P z ˆ =
  • 9. 9 Single Phase Systems Standard conditions: 1) scientific 0oC, 1 atm 1 mol (at std. conditions) ⇒ 22,400 cm3 or 22.4 m3 1 lbmol ⇒ 359 ft3 2) natural gas industry 60oF, 14.7 psia 1 lbmol ⇒ 379 ft3
  • 10. 10 Single Phase Systems Calculations: usually involve converting from one set of conditions to another or 1 2 1 1 2 2 ˆ ˆ T T V P V P = 1 1 2 2 1 1 2 2 T n T n V P V P =
  • 11. 11 Single Phase Systems Ideal gas mixtures Partial pressure of component A: Note: This is used as the definition of "partial pressure", even for non-ideal gases. It is equal to the pressure that would be exerted if A alone occupied the container only for ideal gases. A A Py p =
  • 12. 12 Single Phase Systems Ideal gas mixtures Total pressure = sum of partial pressures: ) 1 ( P y P Py P i i = = = ∑ ∑
  • 13. 13 Single Phase Systems Ideal gas mixtures Similarly: Total volume = sum of partial volumes. PV = nRT can also be written PvA= nART where vA is partial volume of component A in a mixture an nA is its mole fraction.
  • 14. 14 Single Phase Systems Ideal gas mixtures PvA= nART ; divide this by PV = nRT, we obtain, vA / V = nA/n = yA or vA = yAV
  • 15. 15 Single Phase Systems Ideal gas mixtures PvA= nART ; divide this by PV = nRT, we obtain, vA / V = nA/n = yA or vA = yAV (cf. pA= yAP)
  • 16. 16 Single Phase Systems Ideal gas mixtures PvA= nART ; divide this by PV = nRT, we obtain, vA / V = nA/n = yA or vA = yAV (cf. pA= yAP) volume fraction = mole fraction for ideal gases only.