2. Objective
The objective of our project is to determine a mixing model
for the continuous stir tank (Reactor 1). In order to do so, the
behavior of the waterβs temperature inside R1 is analyzed in
two cases which are ideal and non-ideal CST.
3. Rationale
To obtain a better understanding of basic characteristics of
industrial process equipment by independently
comprehending mixing process in continuous stir tank
reactors (CSTR).
8. EHS & LP
Our project entails minimal environmental and safety risks.
β’ However, things to be conscious of include:
β’ Slipping hazards could occur from water leaking out on the floor
β’ All liquid water must be carefully carried away from electrical equipment to
prevent electrical shock
β’ Potential energy waste by excess usage of the CST without running
experiments
9. ExperimentalTesting for Ideality/Non-ideality
130ΒΊF100ΒΊF
100% 85%85% 100%
5 5 57 7 75
Reactor 1 Initial Temperatures:
% of Pump 1 Flow Rate:
Mixer 1 Speed: 7
Note: Data was measured every 6 seconds for a total of 6 minutes. (60 data points per trial )
Reactor 1 total volume was measured with a graduated cylinder
8Total ExperimentalTrials
10. Ideal and Non-Ideal Factors
Ideal
β’ No ambient losses
β’ Perfect Mixing
β’ Uniform and constant cooling
Non-Ideal
β’ Ambient Heat Losses
β’ Non-perfect mixing
β’ Baffles
β’ Conduction from water
to metal reactor/reactor
to water
12. Theory: Ideal Model
Newtonβs Law of Cooling:
ππ
ππ‘
= βπ(π β πππ)
Where:
β’ t is time
β’ T is the temperature of the water within Reactor 1 (R1) at time t
β’ Tin is the temperature of inlet cold water fromTank 1 (TK1)
β’ k is the heat transfer coefficient
13. Theory: Ideal Model
Ideal Model:
π π‘ = π π π
β
πΉ
π π
βπ‘
where
β’ ΞΈ (t) is the temperature deviation from the nominal at time t
β’ ΞΈo is the temperature difference between the inlet cold water fromTK1 and the
initial hot water inside R1.
β’ F is the volume flow rate of the inlet cold water to R1
β’ VT is the total volume of water in R1
14. Theory: Non-ideal Model
Energy balance in temperature:
Active zone:
ππ
πππ
ππ‘
= πΉ πππ β ππ + π(ππ β ππ)
Dead zone:
ππ
πππ
ππ‘
= π(ππ β ππ)
Dead Zone
Active Zone
Baffle
21. T-test
π‘ =
πβ0
π / π
= 2.89
Two-tailed
95% confidence level
Degree of freedom 60
t critical = 2.00
N = the number of residuals
π = the average residual
s = standard deviation of the residuals
Terms Critical value
23. Conclusions
β’ Model fails to passT-test and r-lag-1 tests but illustrates CST temperature behavior
β’ Flow rate Temperature Drop
β’ Mixing Speed Temperature Drop
β’ Due to baffles in all experimental trials, ambiguity exists between Ideal and non-
ideal models.
ππ π+1
= ππ π
+
Ξπ‘
ππ
πΉ πππ β ππ π
+ π(ππ π
β ππ π
)
24. Suggestions
Accounting for conduction between the water and Reactor 1 as well as ambient heat
losses could potentially make it acceptable for us not to statistically reject our
model.
25. Conduction Between Reactor 1 andWater
β’ Initially hot water in Reactor 1 exchanges heat with Reactor 1.
β’ As cold water flows in, the water in the reactor becomes colder than R1 walls
β’ Reactor 1 then conducts heat to the water.
27. Effects of Ambient losses
100 ΒΊF Heat Loss 130 ΒΊF Heat Loss
Average experimental losses (ΒΊF): 14.15 ΒΊF 27.75 ΒΊF
Ambient Heat loss (ΒΊF): 0.6 ΒΊF 2.75 ΒΊF
Percent of Ambient Losses: 4.25 % 10 %
Conclusion: Negligible Not Negligible
28. References
β’ Murrell, Kaston (2015). Standard Operating Procedure: CST Unit & Batch Reactor
Experiments. Oklahoma State University
β’ Myers, Kevin J., Mark F. Reeder, and Julian B. Fasano. "Optimize Mixing by Using the
Proper Baffles." People.clarckson.edu, Feb. 2002. Web. Feb. 2016.
<http://people.clarkson.edu/~wwilcox/Design/mixopt.pdf>.
β’ Rhinehart, R. R. (2016). Sketch CST with Dead Zone. Oklahoma State University.
β’ Skogestad, Sigurd.Chemical and Energy Process Engineering, 1st order. Boca Raton:
CRC Press,Taylor and Francis Group, 2009. pp. 274-280. Print.