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Continuous Stirred Tank Reactor
Chemical engineering skills & practice 1 (University of Bath)
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Abstract
The experiment was carried out by the saponification of ethyl acetate with sodium hydroxide to
determine the effect of residence time and temperature on the conversion of reactant in a stirred
tank reactor. A calibration graph of reactant conversion against residence time was plotted as
shown in Figure 2. From the graph, it was shown that the reactant conversion increases with a
decrease in reactant flow rate due to the increase of residence time as expected. At 30 °πΆ, the
reactant conversion had increased by 6.76% with a decreasing reactant flow rate whereas the
reactant conversion had increased by 4.19% with a decreasing reactant flow rate at 40 °πΆ. The
conversion of reactant was expected to increase with an increasing temperature. However, the
result was not as expected due to experimental errors. The rate constant at 30 °πΆ was found to
be 0.0675 𝑙 π‘šπ‘œπ‘™ −1 𝑠 −1 whereas the rate constant at 40 °πΆ was found to be 0.042 𝑙 π‘šπ‘œπ‘™ −1 𝑠 −1 . The
activation energy was found to be −37447.1 J/mol which was inaccurate as it was calculated
with the inaccurate rate constant.
1.Introduction and Theory
There are many types of reactors generally used for different purposes in the chemical industry.
Continuous-stirred tank reactor (CSTR) are most commonly used in industrial processing,
mainly for homogenous liquid-phase flow reactions, where constant agitation is required (Awdry,
2019). The CSTRs consist of a tank, a stirrer, an inlet and an outlet. It is an open system and
operates on a steady state-basis where all the conditions do not change with time (Mazzotti,
2015). The flow rate into the reactor is equal to the flow rate out of the reactor. The contents in
the CSTR are assumed to be mixed perfectly. Therefore, variables such as temperature and
concentration of the reaction mixture are assumed to be uniformed in all parts of the reaction
vessel.
The general mole balance equation is shown in Equation 1. Since CSTR operates at a steady
state and assumed to have perfect mixing, thus
form the design equation in Equation 2.
𝑉
𝐹𝐽0 − 𝐹𝑗 + ∫ π‘Ÿπ‘— 𝑑𝑉 =
𝑑𝑁𝑗
𝑑𝑑
𝑬𝒒(𝟏)
.𝑉=
𝑑𝑁𝐽
𝑑𝑑
𝐹𝐽0 −𝐹𝑗
−π‘Ÿπ‘—
𝑉
= 0 and ∫0 π‘Ÿπ‘— 𝑑𝑉 = π‘‰π‘Ÿπ‘— . This allows us to
𝑬𝒒(𝟐)
where V represents the reactor volume, 𝐹𝐽0 and 𝐹𝑗 is the input and output flow rate and π‘Ÿπ‘— is the
rate of reaction.
The objective of this experiment was to study how the percentage of conversion of reactant was
affected by the residence time and temperature in the saponification reaction between sodium
hydroxide and ethyl acetate. In this process, hydroxide ions in sodium hydroxide are consumed.
Thus, the reaction progress can be determined by measuring the change in conductivity of
reactant mixture. The percentage conversion of the reactants, X, was calculated with the
conductivity values obtained at different flow rates and temperatures as shown in Equation 3
(University of Bath, 2018).
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𝑋 = (1 −
𝐾 − 𝐾𝑒
) βˆ™ 100
𝐾𝑂 − 𝐾𝑒
𝑬𝒒(πŸ‘)
Where X is the percentage conversion of the reactants (%), K is the actual measured value for
conductivity (mS/cm), Ke is the conductivity at the end of the reaction (mS/cm) and Ko is the
initial conductivity of the 2.3% sodium hydroxide (mS/cm). It was expected that the conversion
would decrease with increasing flow rate due to the decrease of residence time, and conversely,
the conversion would increase with decreasing flow rate due to the increase of residence time.
The conversions of the reactants were also expected to increase with the increase in
temperature of water. (GUNT, 2000)
2. Methods
Temperature
controller
Speed pump 1
Pump 2
Switch box
Pump 1
Heater switch
Master switch
Stirrer
switch
Reaction vessel
Beakers
Figure 1: The general view of the CE310 CSTR
The CE310 Continuous Stirred Tank Reactor was the main apparatus. The switch box contains
switches for the pumps, heater, stirrer and a combined conductivity and temperature measuring
unit. It also has two different controllers which are used to adjust the water temperature in the
heating circuit and to adjust the volumetric flow rate of each pump individually. The main power
switch was turned on. The heater and pump 1 were switched on after the temperature of water
tank was set to 30°C. 2 liters of NaOH (0.2M) and ethyl acetate (0.2M) were poured into the
separate labelled beakers that form part of the CSTR. Both beakers were checked regularly to
ensure there was sufficient reagents throughout the experiment. Pump 2 was turned on to start
filling the reagents into the reaction vessel. The pump dial speed was also set to 10 1/min.
When the mixture reached the overflow limit, the stirrer was turned on. The GUNT-CE310
software in the computer was used to record the conductivity and temperature of the reaction
solution. The conductivity measured within the reaction vessel was observed to determine if the
steady state has been reached. When a steady value has been achieved, the stirrer and pump
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2 were turned off. The GUNT-CE310 software was paused to stop unnecessary recording. The
data was then exported. The volume of the reaction mixture was measured by syringing it out
into a measuring cylinder. These steps were repeated with a different flow rates of 20 1/min and
30 1/min. The temperature was increased to 40°C. Each step was repeated again with three
different flow rates as before. After the experiment, the remaining reagents were emptied back
into the bottles while the reaction mixture and the overflow mixture were poured down the sink.
Each reagent beaker was added with 1L of deionized water to wash through the reactor and
tubing at a high flow rate. The main power supply was turned off after switching off all the
pumps and stirring.
3. Results and Calculations
The average steady state conductivity was recorded in Table 1 and Table 2 (Appendix A). The
pump speed, steady state conductivity and volume of reaction mixture were recorded in Table 3.
Table 3: Conversion of reactant calculated with different pump speeds and temperatures
Pump
Volume of
Pump
reaction
Reactant
speed, Speed,
mixture, V Residence Average steady state
conversion,
Temperature x
𝑣̇
X (%)
(°C)
time, 𝜏 (s) conductivity (mS/cm)
(1/min) (ml/min) (ml)
30
10
42.68
290
407.70
12.40
71.89
30
20
81.46
280
206.24
14.26
67.30
30
30
120.24
260
129.74
15.14
65.13
40
10
42.68
280
393.65
13.09
70.18
40
20
81.46
290
213.61
14.25
67.32
40
30
120.24
260
129.74
14.79
65.99
In Equation 4, the conversion of units of pump speed from 1/min to ml/min was shown.
𝑣̇ = 2 βˆ™ (1.939π‘₯ + 1.949)
𝑬𝒒(πŸ’)
Where 𝑣̇ is the pump speed (ml/min) and x is the pump speed (1/min)
The calculation of residence time was shown in Equation 5.
𝜏=
60
𝑣̇
(𝑉 )
𝑬𝒒(πŸ“)
Where 𝜏 is the residence time and V is the volume of the reaction mixture.
The conversion of reactant was determined according to Equation 3 as mentioned in
Introduction.
𝑋 = (1 −
𝐾 − 𝐾𝑒
) βˆ™ 100
𝐾𝑂 − 𝐾𝑒
𝑬𝒒(πŸ‘)
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Where X is the percentage conversion of the reactants, K is the actual measured value for
conductivity, Ke is the conductivity at the end of the reaction and Ko is the initial conductivity of
the 2.3% sodium hydroxide.
Reactant Conversion (%)
From Table 1, Figure 1 was plotted with the calculated conversion of reactant and residence
time.
74.00
72.00
30°C
70.00
40°C
68.00
Linear (30°C)
66.00
Linear (40°C)
64.00
62.00
60.00
0.00
50.00
100.00
150.00
200.00
250.00
300.00
350.00
400.00
450.00
Residence Time (s)
Figure 1: Graph of reactant conversion against residence time
A rearrangement of the Equation 6 to Equation 7 in the form of a straight-line equation (y = mx +
𝑋𝐴
versus 𝜏 where the gradient (m) is kCA0 as shown
c) was done to plot a graph of (1−𝑋 )(𝑀−𝑋
)
𝐴
in Figure 2.
𝑋𝐴
(1−𝑋
𝐴0
𝐴 )(𝑀−𝑋𝐴 )
𝑋𝐴
(1−𝑋𝐴 )(𝑀−𝑋𝐴 )
𝑬𝒒(πŸ”)
𝜏 = π‘˜πΆ
𝐴
= (𝜏)π‘˜πΆπ΄0
𝑬𝒒(πŸ•)
Where XA is the conversion of reactant, M is the initial molar ratio of reactants and CA0 is the
initial concentration of reactant. From Table 2 (Appendix B), the following graph was produced.
10
y = 0.0135x + 3.5575
R² = 0.9993
9
8
𝑋𝐴/(1−𝑋A )(𝑀−𝑋𝐴 )
y = 0.0084x + 4.577
R² = 0.9977
7
6
30°C
5
40°C
4
3
Linear (30°C)
2
Linear (40°C)
1
0
0.00
50.00
100.00
150.00
200.00
250.00
300.00
350.00
400.00
450.00
Residence time (s)
Figure 2: Graph of (1−𝑋
𝑋𝐴
𝐴 )(𝑀−𝑋𝐴 )
against residence time
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Since the gradient for 30°πΆ is 0.0135 and for 40°πΆ is 0.0084, therefore the rate constant can be
calculated as follows with Equation:
π‘˜=
π‘”π‘Ÿπ‘Žπ‘‘π‘–π‘’π‘›π‘‘
𝐢𝐴0
πΉπ‘œπ‘Ÿ 30 °πΆ, π‘˜ =
0.0135
0.2
𝑬𝒒 (πŸ–)
= 0.0675 𝑙 π‘šπ‘œπ‘™ −1 𝑠 −1
πΉπ‘œπ‘Ÿ 40°πΆ, π‘˜ =
0.0084
0.2
= 0.042 𝑙 π‘šπ‘œπ‘™ −1 𝑠 −1
To obtain the activation energy, a graph of ln (k) against 1/T was plotted as shown in Figure 3
with values from Table 3 (Appendix B).
-2.6
0.00318
-2.7
0.0032
0.00322
0.00324
0.00328
0.0033
0.00332
y = 4504.1x - 17.553
R² = 1
-2.8
ln (k)
0.00326
-2.9
-3
-3.1
-3.2
1/T (K-1)
Figure 3: Graph of ln(k) against 1/T
Equation 9 showed the Arrhenius equation where k is the rate constant, Ea is the activation
energy, R is the gas constant (8.314J/K mol), and T is the temperature expressed in Kelvin.
𝐸
π‘˜ = 𝐴𝑒 −π‘…π‘‡π‘Ž
Eq (9)
Equation 10 was obtained by taking the natural logarithm of both sides in Equation 9. It was
rearranged to plot a straight line graph for ln(k) versus 1/T, where the slope is -Ea/R as shown in
Equation 11.
𝐸
π‘™π‘›π‘˜ = 𝑙𝑛𝐴 − π‘Ž
𝑅𝑇
𝑬𝒒 (𝟏𝟎)
𝐸 1
π‘™π‘›π‘˜ = 𝑙𝑛𝐴 − π‘Ž ( )
𝑅 𝑇
From Equation 12, the activation energy was calculated.
πΈπ‘Ž = π‘”π‘Ÿπ‘Žπ‘‘π‘–π‘’π‘›π‘‘ βˆ™ 𝑅
𝑬𝒒(𝟏𝟐)
𝑬𝒒 (𝟏𝟏)
πΈπ‘Ž = −4501.1 × 8.314 = −37447.1 J/mol
4.Discussion
Based on Figure 1, the reactant conversion increased with an increasing residence time as
expected. For example, at 40 °πΆ, the conversion was 65.99% at the residence time of 129.74s
and the conversion was 70.18% at the residence time of 393.65s. This clearly showed an
increase of 4.19%. Residence time refers to the time spent by the fluid elements within the
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reactor. Thus, an increased residence time means more contact time for the chemicals in the
reactor due to a decreasing pump speed.
The reactant conversions should increase with an increased temperature due to the raised of
average kinetic energy of reactant molecules. Therefore, a greater proportion of molecules will
have sufficient energy for an effective collision, giving a higher conversion of reactant. (Ullah et
al., 2015) However, from Figure 1, the graph showed that the conversion of reactant at 30 °πΆ
was higher than the conversion of reactant at 40 °πΆ. The highest reactant conversion in 30 °πΆ
was 71.89% but the highest conversion in 40 °πΆ was only 70.18%. This error can be explained
by the incorrect temperature of water. The actual temperature of water was different from the
value set by the temperature controller. According to data saved from the computer software,
the temperature recorded in three different flow rates were only 34.1 °πΆ , 34.6 °πΆ , 34.7 °πΆ
instead of 40 °πΆ. This was because it takes more time for the CSTR to heat up to that specific
temperature. More time should have been given to achieve the temperature of 40 °πΆ before the
conductivity was measured. A lower conductivity would have been obtained in higher
temperature, giving a higher conversion of reactant. With the pump speed of 20 1/min, the
difference between the reactant conversion at 30 °πΆ and 40 °πΆ was only by 0.02%. This small
percentage was insignificant to justify the theory. Therefore, a larger temperature range should
have been used to plot a more reliable graph.
The rate constant at 30 °πΆ was 0.0675 𝑙 π‘šπ‘œπ‘™ −1 𝑠 −1 while the rate constant at 40 °πΆ was
0.042 𝑙 π‘šπ‘œπ‘™ −1 𝑠 −1. This result was unacceptable as a higher temperature should have given a
higher rate constant. This could be due to the same error as mentioned earlier.
By using Arrhenius’s equation, the activation energy obtained was -37447.1 J/mol.
In this experiment, results could have been improved by reducing parallax error while taking the
measurement such as the volume of the reaction mixture. The position of eye must be
perpendicular to the reading scale of measuring cylinder. The experiment should have been
carried out with more different flow rates to obtain a more accurate result.
5. Conclusion
The Continuous Stirred Tank Reactor was used to determine the effect of residence time and
temperature on the conversion of reactant based on the saponification of ethyl acetate with
sodium hydroxide. The progress of the reaction was determined by the change in the hydroxide
concentration. From Figure 1, it was clear that the conversion of reactant increases as
residence time increases. From 10 1/min to 30 1/min, the reactant conversion increased by
6.76% at 30 °πΆ while the reactant conversion increased by 4.19% at 40 °πΆ. An increase in
temperature will increase the percentage of reactant conversion as well. However, the results
had shown otherwise. This was caused by the inaccurate temperature as mentioned earlier.
The results could be improved by measuring the conductivity only when the temperature
reaches 40 °πΆ.To increase the accuracy of this experiment, it is recommended that a larger
difference in temperature should be used. To plot a more reliable graph, the experiment should
have been carried out with more different flow rates. Overall, the experiment was successful.
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References
1) Awdry, S. (2019). University of Bath Single Sign-on. [online] Moodle.bath.ac.uk. Available at:
https://moodle.bath.ac.uk/pluginfile.php/1119404/mod_resource/content/5/BOOKLET%20OF%2
0CHEMICAL%20REACTION%20ENGINEERING_Forstudents.pdf [Accessed 8 Feb. 2019].
2) Mazzotti, M. (2015). Introduction to Chemical Engineering: Chemical Reaction Engineering.
[online] Ethz.ch. Available at: https://www.ethz.ch/content/dam/ethz/specialinterest/mavt/process-engineering/separation-processes-laboratorydam/documents/education/bce%20notes/script_7.pdf [Accessed 8 Feb. 2019].
3) G.U.N.T. (2000) Experiment Instructions: CE 310 Chemical Reactors Trainer.
4) University of Bath, 2018 CE10185 Chemical Engineering Skills and Practice 1, Student Lab
Book 2018-19, pp32-38
5) Mazzotti, M. (2015). Introduction to Chemical Engineering: Chemical Reaction Engineering.
[online] Ethz.ch. Available at: https://www.ethz.ch/content/dam/ethz/specialinterest/mavt/process-engineering/separation-processes-laboratorydam/documents/education/bce%20notes/script_7.pdf [Accessed 8 Feb. 2019].
6) Ullah, I., Ahmad, M.I., Younas, M., 2015. Optimization of Saponification Reaction in a
Continuous Stirred Tank Reactor (CSTR) using Design of Experiments, Pak. J. Engg. & Appl.
Sci. 16, pp. 84-92
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Appendix
Appendix A: Average steady state conductivity measured in different temperatures
Table 1: Average steady state conductivity at 30°C
Steady state
conductivity with
Temperature Data
pump speed of 10
(°C)
number 1/min (mS/cm)
Steady state
conductivity with
pump speed of 20
1/min (mS/cm)
Steady state
conductivity with
pump speed of 30
1/min (mS/cm)
30
1
12.4
14.26
15.14
30
2
12.4
14.26
15.14
30
3
12.4
14.26
15.14
30
4
12.4
14.26
15.14
30
5
12.4
14.26
15.14
30
5
12.4
14.26
15.14
30
6
12.4
14.26
15.14
30
7
12.4
14.26
15.14
30
8
12.4
14.26
15.14
30
9
12.4
14.26
15.14
30
10
Average steady state
conductivity
12.4
14.26
15.09
12.4
14.26
15.14
Table 2: Average steady state conductivity at 40°C
Temperature Data
(°C)
number
40
1
40
2
40
3
40
4
40
5
40
5
40
6
40
7
40
8
40
9
40
10
Average steady state
conductivity
Steady state
conductivity with pump
speed of 10 1/min
(mS/cm)
13.09
13.09
13.09
13.09
13.09
13.09
13.09
13.09
13.09
13.09
13.09
Steady state
conductivity with pump
speed of 20 1/min
(mS/cm)
14.26
14.26
14.26
14.26
14.26
14.26
14.26
14.26
14.26
14.21
14.21
Steady state
conductivity with pump
speed of 30 1/min
(mS/cm)
14.79
14.79
14.79
14.79
14.79
14.79
14.79
14.79
14.79
14.79
14.79
13.09
14.25
14.79
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Appendix B: Reactant conversion and rate constant calculated at different temperatures
Table 2: Reactant conversion at different temperatures
Temperature, T
(°C)
30
30
30
40
40
40
Residence Time, 𝜏
Reactant Conversion, XA
(s)
(-)
407.70
0.719
206.24
0.673
129.74
0.651
393.65
0.702
213.61
0.673
129.74
0.660
𝑋𝐴
(1−𝑋𝐴 )(𝑀−𝑋𝐴 )
(l mol-
1
)
9.095356
6.293719
5.356245
7.895382
6.305532
5.706219
Table 3: Rate constant at different temperatures
Rate
constant, k (l
Temperature, T
mol-1 s-1)
Temperature, T (°C)
(°C)
1/T (K-1)
ln (k)
30
303.15
0.003299
0.0675
-2.69563
40
313.15
0.003193
0.042
-3.17009
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