Chapter 5: Isothermal Reactor Design: Conversion
Topics
- Algorithm for Isothermal Reactor Design
- Applications/Examples of CRE Algorithm
- Reversible Reactions
- ODE (Polymath) Solutions to CRE Problems
- General Guidelines for California Problems
- PBR with Pressure Drop
- Engineering Analysis
Algorithm for Isothermal Reactor Design | top |
For the $5^{th}$ edition $\frac{P}{P_o}$ equals $p$ i.e. $p = \frac{P}{P_o}$. In the $4^{th}$ and earlier editions
$y = \frac{P}{P_o}$
Example: The elementary liquid phase reaction
is carried out isothermally in a CSTR. Pure A enters at a volumetric flow rate of 25 dm3/s and at a concentration of 0.2 mol/dm3.
What CSTR volume is necessary to achieve a 90% conversion when k = 10 dm3/(mol*s)?
Mole Balance |
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Rate Law |
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Stoichiometry |
liquid phase (v = vo) |
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Combine |
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Evaluate |
at X = 0.9, |
V = 1125 dm3 |
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Space Time |
Here are some links to example problems. You could also use these problems as self tests.
Videos
The following humorous videos were made by Professor Lane's 2008 Chemical Reaction Engineering class at the University of Alabama, Tuscaloosa.
Applications/Examples of the CRE Algorithm | top |
Gas Phase Elementary Reaction | Additional Information | ||
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only A fed |
P0 = 8.2 atm |
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T0 = 500 K |
CA0 = 0.2 mol/dm3 |
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k = 0.5 dm3/mol-s |
vo = 2.5 dm3/s |
Solve for X = 0.9
Applying the algorithm to the above reaction occurring in a Batch,
CSTR, and PFR.
Batch | CSTR | PFR | |
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Mole Balance: | |||
Rate Law: | |||
Stoichiometry: |
Gas: V = V0 |
Gas: T =T0, P =P0 |
Gas: T = T0, P = P0 |
Per Mole of A:
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Per Mole of A:
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Combine: | |||
Integrate | |||
Evaluate | |
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For X = 0.9: |
V = 680.6 dm3 |
V = 90.7 dm3 |
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Reversible Reactions | top |
To determine the conversion or reactor volume for reversible reactions, one must first calculate the maximum conversion that can be achieved at the isothermal reaction temperature, which is the equilibrium conversion. (See Example 3-8 in the text for additional coverage of equilibrium conversion in isothermal reactor design.)
Equilibrium Conversion, Xe
From Appendix C:
Example: Determine Xe for a PFR with no pressure drop, P = P0
Given that the system is gas phase and isothermal, determine the reactor volume when X = 0.8 Xe.
Reaction | Additional Information | |
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CA0 = 0.2 mol/dm3 |
k = 2 dm3/mol-min |
First calculate Xe:
X = 0.8Xe = 0.711
One could then use Polymath to determine the volume of the PFR. The corresponding Polymath program is shown below.
ODE (Polymath) Solutions to CRE Problems | top |
Equations
Plot of X vs. V
Results in Tabular Form
A volume of 94 dm3 (rounding up from slightly more than 93 dm3) appears to be our answer.
General Guidelines for California Problems | top |
Every state has an examination engineers must pass to become a registered professional engineer. In the past there have typically been six problems in a three hour segment of the California Professional Engineers Exam. Consequently one should be able to work each problem in 30 minutes or less. Many of these problems involve an intermediate calculation to determine the final answer.
Some Hints:
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PBR with Pressure Drop | top |
Note: Pressure drop does NOT affect liquid phase reactions
Sample Question:
Analyze the following second order gas phase reaction that occurs isothermally in a PBR:
Mole Balance
Must use the differential form of the mole balance to separate variables
Rate Law
Second order in A and irreversible:
Stoichiometry
Need to find (P/P0) as a function of W (or V if you have a PFR).
Pressure Drop in Packed Bed Reactors
Ergun Equation |
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Variable Gas Density |
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let |
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where |
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let |
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then |
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English: | |
Español: | |
Svenska: |
We will use this form for multiple reactions: |
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$$\frac{dp}{dW} = -\frac{\alpha}{2p}\frac{T}{T_o}\frac{F_T}{F_{To}}$$ |
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$$ p=\frac{P}{P_o}$$ |
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We will use this form for single reactions: |
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$\frac{dp}{dW} = -\frac{\alpha}{2p}\frac{T}{T_o}(1+\epsilon X)$ |
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Isothermal Operation |
$\frac{dp}{dW} = -\frac{\alpha}{2p} (1+\epsilon X) $ |
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recall that |
$\frac{dX}{dW} = \frac{k{C_{Ao}}^2(1-X)^2}{F_{Ao}(1+\epsilon X)^2} p^2$ |
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notice that |
$\frac{dX}{dW} = f(X,P) and \frac{dP}{dW} = f(X,P) or \frac{dp}{dW} = f(p,X)$ |
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The two expressions are coupled ordinary differential equations. We can
solve them simultaneously using an ODE solver such as Polymath. For the special case of
isothermal operation and epsilon = 0, we can obtain an analytical solution. |
Analytical Solution, [e], PFR with
$\frac{dp}{dW} = -\frac{\alpha}{2p} (1+\epsilon X)$ | ||
CAUTION: Never use this form if |
$C_A = C_{A0}(1-X)p = C_{A0}(1-X)(1-\alpha W)^\frac{1}{2}$ | |
Combine |
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Solve |
Could now solve for X given W, or for W given X.
For gas phase reactions, as the pressure drop increases, the concentration decreases,
resulting in a decreased rate of reaction, hence a lower conversion when compared to a
reactor without a pressure drop.
Here are some links to example problems dealing with packed bed reactors. You could
also use these problems as self tests.
Analysis using Simulation Tools
Consider the following gas phase reaction carried out isothermally in a packed bed reactor containing 100 kg of catalyst. Pure A is fed at a rate of 2.5 mol/s and with $ {C_{A0} = 0.2 \frac{mol}{dm^3}} $, and $ {\alpha = 0.0162kg^{-1}} $.
2AB
Mole Balance
$ {\frac{dX}{dW} = -r_A^{'} / F_{A0}} $
Rate Law
Elementary: $ {r_A^{'} = -kC_A^2} $
Stoichiometry
Gas with ${T = T_0}$
${A \rightarrow \frac{1}{2}B \\ C_A = \frac{F_A}{v} = \frac{C_{A0}(1-X)p}{1+\epsilon X} \\ \frac{dp}{dW} = -\alpha \frac{1+\epsilon X}{2p} \\ \epsilon = -1/2 \\ F_{A0} = 2.5 \\ C_{A0} = 0.2 \\ k = 5 \\ \alpha = 0.0162 \\ W_{final} = 100 \\ X(W = 0) = 0, p(W = 0) = 1 }$
The above equations can be easily combined with the help of simulation tools such as Polymath, Wolfram or Python.
Below is the result from Polymath
Here are links to Polymath, Wolfram, and Python code for the above example
Polymath Code Wolfram Code Python Code
Optimum Paritcle Diameter
Laminar Flow, Fix P0, ρ0,
ρ0 = P0(MW)/RT0
ρ0P0∼P02
Increasing the particle diameter descreases the pressure drop and increases the rate and conversion.
However, there is a competing effect. The specific reaction rate decreases as the particle size increases, therefore so deos the conversion.
k ∼ 1/Dp
DP1 > DP2 |
The larger the particle, the more time it takes the reactant to get in and out of the catalyst particle. For a given catalyst weight, there is a greater external surgace area for smaller particles than larger particles. Therefore, there are more entry ways into the catalyst particle.
Later on in the course, we will learn that effectiveness factor decreases as the particle size increases
Engineering Analysis - Critical Thinking and Creative Thinking | top |
We want to learn how the various parameters (particle diameter, porosity, etc.) affect the pressure drop and hence conversion. We need to know how to respond to "What if" questions, such as:
"If we double the particle size, decrease the porosity by a factor of 3, and double the pipe size, what will happen to D P and X?"
(See Critical Thinking in Preface Table P1 and P2 on pages xvi and xvii. e.g., Questions the probe consenquences)
To answer these questions we need to see how a varies with these parameters.
Turbulent Flow
Compare Case 1 and Case 2:
For example, Case 1 might be our current situation and Case 2 might be the parameters we want to change to.
For constant mass flow through the system= constant
Laminar Flow
Polymath Book Problem
The following is an example problem from the book. It is located on page 192 in Chapter 5. This is a problem done in polymath and the .pol file has been included for reference. The report and accompanying graphs generated in Polymath are also shown.
Here are more links to example problems dealing with packed bed reactors. Again, you could
also use these problems as self tests.
* All chapter references are for the 1st Edition of the text Essentials of Chemical Reaction Engineering .