Adiabatic Reactor
Analysis for Methanol Synthesis
An important industrial reaction is the combination of
carbon monoxide with hydrogen to produce methanol. Methanol is quite useful for
a variety of chemical synthesis reactions, including the transesterification
of triglycerides in vegetable oils for biodiesel
production. The gaseous mixture of carbon monoxide and hydrogen can be used to
synthesize a wide array of hydrocarbons, including synthetic fuels, and is
therefore often referred to as “syn-gas”.
Syngas can be obtained from coal, as discussed in
this paper by Octave Levenspiel (Professor,
The overall reaction for methanol synthesis from syngas is written as:
CO + 2 H2 à CH3OH
And can be approximated as an elementary reaction, such that the rate expression (assuming irreversible reaction, as written above) is:
![]()
Where
, ko = 5.7x1010
L2.mol-2.min-1, EA = 100.5 kJ/mol
I. Energy Balance and the Conversion-Temperature Relationship
The Thermodynamics of reaction species are (From Felder & Rousseau)
|
Species |
Cp(J/mol.K) |
Hf
(kJ/mol) at 298K |
|
CO |
29 |
-110.5 |
|
H2 |
28.8 |
0 |
|
CH3OH |
43 |
-201.2 |
We can then calculate the change in thermodynamic properties (Enthalpy and heat capacity) upon reaction, using stoichiometry.
DCprxn = 1*43 – 2*28.8 – 1*29 = -43.6 J/mol.K
DHrxn = -201.2 – 2*0 – 1*(-110.5) = -90.7 kJ/mol.K
For an adiabatic reactor (either a CSTR or PFR w/o significant heat dispersion), the energy balance yields the following temperature vs. conversion dependency (Fogler, eqn 8-30),

II. Mass Balance and Rate Expression
We can write a general stoichiometric table for this reaction system, accounting for the presence of inert diluent, I.
|
Species |
Initial |
Change |
Final |
|
CO |
|
|
|
|
H2 |
|
|
|
|
CH3OH |
|
|
|
|
Inert |
|
0 |
|
|
Total |
|
|
|
If we assume that everything is ideal gas, then concentration = moles/volume, and accounting for changing volume with temperature and conversion, (Pressure is constant, or pressure drop defined by momentum balance, e.g. Ergun equation)

Our concentrations for each species can then be calculated from stoichiometric table, in terms of conversion, pressure and temperature



We can substitute these terms into the rate expression, as follows:

III. Inlet Conditions
We further assume that there is no pressure drop associated
with gas flow through the continuous reactor, i.e. P =
IV.A. Calculation 1: Solve for 5% conversion (X = 0.05)
Using Equation (8-30) from Fogler,
350.97 Kelvin
For our rate expression, substituting T = 350.97 and X = 0.05,
= 2.8x10-11 mol.min-1.L-1
For obtaining a Levenspiel plot
(for sizing either a CSTR or PFR), we want to calculate
,
Liters.
IV.B. Calculation 2: Solve for 10% conversion (X = 0.10)
404.7 Kelvin
For our rate expression, substituting T = 404.7 and X = 0.1,
= 3.4x10-9 mol.min-1.L-1.
For obtaining a Levenspiel plot
(for sizing either a CSTR or PFR), we want to calculate
,
Liters.
IV.C. Calculation 3: Solve for 50% Conversion (X = 0.50)
Using Equation (8-30) from Fogler,
870.8 Kelvin
For our rate expression, substituting T = 870.8 and X = 0.50,
=9.1x10-3 mol.min-1.L-1
For obtaining a Levenspiel plot
(for sizing either a CSTR or PFR), we want to calculate
,
Liters.
IV.D. Generate Data for Levenspiel Plot
|
X |
T |
k |
-rCO |
Fao/-rCO |
|
0.05 |
351.0 |
6.28 x 10-5 |
2.82x10-11 |
1.18x1010 |
|
0.10 |
404.7 |
6.08 x 10-3 |
3.43x10-9 |
9.73x107 |
|
0.15 |
459.4 |
2.13 x 10-1 |
1.18x10-7 |
2.83x106 |
|
0.20 |
515.0 |
3.65 x 100 |
1.83x10-6 |
1.82x105 |
|
0.25 |
571.7 |
3.74 x 101 |
1.63x10-5 |
2.05x104 |
|
0.30 |
629.3 |
2.59 x 102 |
9.60x10-5 |
3.47x103 |
|
0.35 |
688.0 |
1.34 x 103 |
4.14x10-4 |
8.04x102 |
|
0.40 |
747.8 |
5.44 x 103 |
1.30x10-3 |
2.38x102 |
|
0.45 |
808.7 |
1.84 x 104 |
3.88x10-3 |
8.60x101 |
|
0.5 |
870.5 |
5.33 x 104 |
9.12x10-3 |
3.65x101 |
|
0.55 |
934.0 |
1.36 x 105 |
1.87x10-2 |
1.79x101 |
|
0.60 |
998.4 |
3.14 x 105 |
3.38x10-2 |
9.85x100 |
|
0.65 |
1064.0 |
6.64 x 105 |
5.49x10-2 |
6.08x100 |
|
0.70 |
1130.9 |
1.30 x 106 |
7.99x10-2 |
4.17x100 |
|
0.75 |
1199.1 |
2.39 x 106 |
1.04x10-1 |
3.20x100 |
|
0.80 |
1268.7 |
4.15 x 106 |
1.20x10-1 |
2.78x100 |
|
0.85 |
1339.7 |
6.87 x 106 |
1.17x10-1 |
2.85x100 |
|
0.90 |
1412.1 |
1.09 x 107 |
8.76x10-2 |
3.81x100 |
|
0.95 |
1486.0 |
1.67 x 107 |
3.61x10-2 |
9.23x100 |
|
0.96 |
1501.0 |
1.81 x 107 |
2.55x10-2 |
1.31x101 |
|
0.97 |
1516.0 |
1.96 x 107 |
1.58x10-2 |
2.11x101 |
|
0.98 |
1531.0 |
2.12 x 107 |
7.75x10-3 |
4.30x101 |
|
0.99 |
1546.2 |
2.29 x 107 |
2.13x10-3 |
1.56x102 |
We can then plot this data to see how to best perform this reaction.

We can see from the plot that a CSTR will get us to a conversion of ~ 85% - after that we would prefer a PFR to keep reactor volume to a minimum.
Caveat
Sometimes people write for a gas-phase reaction the rate expression in terms of partial pressures
![]()
Our true form of the rate expression, which is in terms of concentrations, is
![]()
Comparing the two, we see that

Which when linearized does not fit an Arrhenius relationship.