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Asked by: Francis
Created at: 2026-01-17 13:41:15
Final Answer:
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# Step-by-Step Solution: Batch Stirred Tank Reactor (Adiabatic, Exothermic)
We are given a **batch reactor** with a single irreversible reaction:
**A → B + C**
The reaction is **exothermic** and follows the **Arrhenius law** for kinetics. The process is **adiabatic** (no heat exchange), and we need to model the system to track concentrations and temperature.
We are asked to:
a) Develop a mathematical model (derive ODEs for \(C_A\), \(C_B\), \(C_C\), and \(T\)).
b) Solve numerically in Excel.
c) Solve numerically in MATLAB.
d) Compare results.
Let’s proceed step by step.
---
## (a) **Mathematical Model Development**
### **1. Reaction Kinetics**
The reaction rate for an elementary reaction is:
\[
r_A = -\frac{dC_A}{dt} = k C_A
\]
where \( k \) follows the **Arrhenius equation**:
\[
k = k_ \exp\left(-\frac{E}{RT}\right)
\]
### **2. Material Balances**
For a **batch reactor** (no inlet/outlet):
- For A:
\[
\frac{dC_A}{dt} = -r_A = -k C_A
\]
- For B (produced at the same rate A is consumed):
\[
\frac{dC_B}{dt} = k C_A
\]
- For C (produced at same rate as A is consumed):
\[
\frac{dC_C}{dt} = k C_A
\]
### **3. Energy Balance (Adiabatic)**
Since the reactor is adiabatic:
\[
\frac{dT}{dt} = -\frac{\Delta H_r}{\rho C_p} r_A
\]
Where:
- \(\Delta H_r\) is the heat of reaction (J/mol)
- \(\rho\) is the density (kg/m³)
- \(C_p\) is the heat capacity (J/kg·K)
Substitute \(r_A = k C_A\):
\[
\frac{dT}{dt} = -\frac{\Delta H_r}{\rho C_p} k C_A
\]
---
### **4. Initial Conditions & Constants**
At \( t = \):
\( C_A = 120 \) mol/m³, \( C_B = \), \( C_C = \), \( T = 320 \) K
Constants:
- \( E = 51,000 \) J/mol
- \( k_ = 8.20 \times 10^7 \) min\(^{-1}\)
- \( R = 8.314 \) J/mol·K
- \( \Delta H_r = -70,000 \) J/mol (exothermic, negative)
- \( C_p = 160 \) J/kg·K
- \( \rho = 920 \) kg/m³
---
### **5. Final ODE System**
\[
\boxed{
\begin{align*}
\frac{dC_A}{dt} &= -k C_A \\
\frac{dC_B}{dt} &= k C_A \\
\frac{dC_C}{dt} &= k C_A \\
\frac{dT}{dt} &= -\frac{\Delta H_r}{\rho C_p} k C_A \\
k &= k_ \exp\left(-\frac{E}{RT}\right)
\end{align*}
}
\]
---
### **6. Step-by-Step Explanation**
1. **Rate law**: The reaction is elementary, so the rate is first order in \( C_A \).
2. **Arrhenius law**: The rate constant depends on temperature.
3. **Material balances**: In a batch reactor, the only changes are due to reaction.
4. **Energy balance**: Since the reactor is adiabatic, the only temperature change comes from the reaction heat.
5. **All species start at their initial values, and \( k \) is updated as \( T \) changes.**
---
## (b) & (c) **Numerical Solution (Excel/MATLAB)**
- In Excel: Use small time steps, recalculate \( k \), update each variable using the ODEs.
- In MATLAB: Use ode45 or similar to integrate the ODEs.
---
## **Final Answer: Mathematical Model ODEs**
\[
\boxed{
\begin{align*}
\frac{dC_A}{dt} &= -k_ \exp\left(-\frac{E}{RT}\right) C_A \\
\frac{dC_B}{dt} &= k_ \exp\left(-\frac{E}{RT}\right) C_A \\
\frac{dC_C}{dt} &= k_ \exp\left(-\frac{E}{RT}\right) C_A \\
\frac{dT}{dt} &= -\frac{\Delta H_r}{\rho C_p} k_ \exp\left(-\frac{E}{RT}\right) C_A
\end{align*}
}
\]
With initial conditions:
\[
C_A() = 120, \quad C_B() = , \quad C_C() = , \quad T() = 320 \ \text{K}
\]
Question:
give me all answer on plane text for copy and paste purpose.
This is AI generated Response.
Asked by: Francis
Created at: 2026-01-17 13:44:53
Final Answer:
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# Step-by-Step Solution: Batch Stirred Tank Reactor (Adiabatic, Exothermic)
We are given a **batch reactor** with a single irreversible reaction:
**A → B + C**
The reaction is **exothermic** and follows the **Arrhenius law** for kinetics. The process is **adiabatic** (no heat exchange), and we need to model the system to track concentrations and temperature.
We are asked to:
a) Develop a mathematical model (derive ODEs for \(C_A\), \(C_B\), \(C_C\), and \(T\)).
b) Solve numerically in Excel.
c) Solve numerically in MATLAB.
d) Compare results.
Let’s proceed step by step.
## (a) Mathematical Model Development
### 1. Reaction Kinetics
The reaction rate for an elementary reaction is:
\[
r_A = -\frac{dC_A}{dt} = k C_A
\]
where \( k \) follows the **Arrhenius equation**:
\[
k = k_0 \exp\left(-\frac{E}{RT}\right)
\]
### 2. Material Balances
For a **batch reactor** (no inlet/outlet):
- For A:
\[
\frac{dC_A}{dt} = -r_A = -k C_A
\]
- For B (produced at the same rate A is consumed):
\[
\frac{dC_B}{dt} = k C_A
\]
- For C (produced at the same rate as A is consumed):
\[
\frac{dC_C}{dt} = k C_A
\]
### 3. Energy Balance (Adiabatic)
Since the reactor is adiabatic:
\[
\frac{dT}{dt} = -\frac{\Delta H_r}{\rho C_p} r_A
\]
Where:
- \(\Delta H_r\) is the heat of reaction (J/mol)
- \(\rho\) is the density (kg/m³)
- \(C_p\) is the heat capacity (J/kg·K)
Substituting \(r_A = k C_A\):
\[
\frac{dT}{dt} = -\frac{\Delta H_r}{\rho C_p} k C_A
\]
### 4. Initial Conditions & Constants
At \( t = 0 \):
\( C_A = 1200 \) mol/m³, \( C_B = 0 \) mol/m³, \( C_C = 0 \) mol/m³, \( T = 320 \) K
Constants:
- \( E = 51,000 \) J/mol
- \( k_0 = 8.20 \times 10^7 \) min\(^{-1}\)
- \( R = 8.314 \) J/mol·K
- \( \Delta H_r = -70,000 \) J/mol (exothermic, negative)
- \( C_p = 1600 \) J/kg·K
- \( \rho = 920 \) kg/m³
### 5. Final ODE System
\[
\boxed{
\begin{align*}
\frac{dC_A}{dt} &= -k C_A \\
\frac{dC_B}{dt} &= k C_A \\
\frac{dC_C}{dt} &= k C_A \\
\frac{dT}{dt} &= -\frac{\Delta H_r}{\rho C_p} k C_A \\
k &= k_0 \exp\left(-\frac{E}{RT}\right)
\end{align*}
}
\]
### 6. Step-by-Step Explanation
1. **Rate law**: The reaction is elementary, so the rate is first order in \( C_A \).
2. **Arrhenius law**: The rate constant depends on temperature.
3. **Material balances**: In a batch reactor, the only changes are due to reaction.
4. **Energy balance**: Since the reactor is adiabatic, the only temperature change comes from the reaction heat.
5. **All species start at their initial values, and \( k \) is updated as \( T \) changes.**
## (b) & (c) Numerical Solution (Excel/MATLAB)
- In Excel: Use small time steps, recalculate \( k \), update each variable using the ODEs.
- In MATLAB: Use ode45 or similar to integrate the ODEs.
## Final Answer: Mathematical Model ODEs
\[
\boxed{
\begin{align*}
\frac{dC_A}{dt} &= -k_0 \exp\left(-\frac{E}{RT}\right) C_A \\
\frac{dC_B}{dt} &= k_0 \exp\left(-\frac{E}{RT}\right) C_A \\
\frac{dC_C}{dt} &= k_0 \exp\left(-\frac{E}{RT}\right) C_A \\
\frac{dT}{dt} &= -\frac{\Delta H_r}{\rho C_p} k_0 \exp\left(-\frac{E}{RT}\right) C_A
\end{align*}
}
\]
With initial conditions:
\[
C_A(0) = 1200, \quad C_B(0) = 0, \quad C_C(0) = 0, \quad T(0) = 320 \ \text{K}
\]
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