Modeling CSTRs in Series constant holdup, isothermal
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Transcript of Modeling CSTRs in Series constant holdup, isothermal
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CHE412 Process Dynamics and ControlBSc (Engg) Chemical Engineering (7th Semester)
Week 3 (contd.)Mathematical Modeling (Contd.)
Luyben (1996) Chapter 3 Stephanopoulos (1984) Chapter 5
Dr Waheed Afzal Associate Professor of Chemical Engineering
Institute of Chemical Engineering and TechnologyUniversity of the Punjab, Lahore
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Modeling CSTRs in Seriesconstant holdup, isothermal
F0
F1
CA1
F2
CA2 F3
CA3
V1
K1
T1
V2
K2
T2
V3
K3
T3
Basis and AssumptionsA → B (first order reaction)Compositions are molar and flow rates are volumetricConstant V, ρ, T Overall Mass Balance i.e. at constant V, F3 =F2 =F1 =F0 ≡ FSo overall mass balance is not required!
Luyben (1996)
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Modeling CSTRs in Seriesconstant holdup, isothermal
Component A mass balance on each tank (A is chosen arbitrarily)
kn depends upon temperature kn = k0 e-E/RTn where n = 1, 2, 3Apply degree of freedom analysis! Parameters/ Constants (to be known): V1, V2, V3, k1, k2, k3
Specified variables (or forcing functions): F and CA0 (known but not constant) . Unknown variables are 3 (CA1, CA2, CA3) for 3 ODEs Simplify the above ODEs for constant V, T and putting τ = V/F
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Modeling CSTRs in Seriesconstant holdup, isothermal
If throughput F, temperature T and holdup V are same in all tanks, then for τ = V/F (note its dimension is time)
In this way, only forcing function (variable to be specified) is CA0.
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Modeling CSTRs in Series Variable Holdups, nth order
Mass Balances (Reactor 1)
n
Mass Balances (Reactor 2)
n Mass Balances (Reactor 1)
)n
Changes from previous case: V of reactors (and F) varies with time, reaction is nth order Parameters to be known: k1, k2, k3, nDisturbances to be specified:CA0, F0 Unknown variables: CA1, CA2, CA3, V1, V2, V3, F1, F2, F3
CV MVInclude
Controller eqnsV1 (or h1) F1 F1 = f(V1)
V2 (or h2) F2 F2 = f(V2)
V3 (or h3) F3 F3 = f(V3)
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H1
H2
H3
Qin or out
Modeling a Mixing Process
Overall Mass Balance Component Mass Balance 3
Basis and AssumptionsF (volumetric), CA (molar); Well StirredFeed (1, 2) consists of components A and B Enthalpy of mixing is significant Process includes heating/ coolingρ is constant
Stephanopoulos (1984)
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H1
H2
H3
Modeling a Mixing ProcessConservation of energy
(recall first law of thermodynamics)
(for constant ρ/ liquid systems is zero)
Energy Balance
enthalpy balance (h is energy/mass)
We were familiar with energy ; how to characterize h (specific enthalpy) into familiar quantities (T, CA, parameters, …)
H is enthalpy, h is specific enthalpy; CP is heat capacity, cP is specific heat capacity ….
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Modeling a Mixing Process
Since enthalpy depends upon temperature so lets replace h with h(T)
enthalpy associated with ΔT was easy to obtain, how to obtain h(T0)
and are molar enthalpy of component A and B and is heat of solution for stream i at T0.
𝑑 (𝜌𝑉 𝒉𝟑)𝑑𝑡 =𝜌(𝐹 ¿¿1𝒉𝟏+𝐹2𝒉𝟐)−𝜌 𝐹 3𝒉𝟑±𝑄 ¿
Put values of h in overall energy balance
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Modeling a Mixing ProcessRe-arranging (and using component mass balance equations)
If we assume cP1 = cP2 = cP3 = cP
cp If heats of solutions are strong functions of concentrations
then and are significant Mixing process is generally kept isothermal (how?)
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Tips For Assessment (Exam)Introduction + Modeling (week 1-3)
1. Consult your class notes, board proofs, discussions
2. Stephanopoulos (1984) chapters 1-5, examples and end-chapter problems
3. Luyben (1996) chapter 3 page 40 to 74. Practice examples and end-chapter problems for chapter 3.
In exam, you may be asked short descriptive questions to check your understanding of process control and to prepare a mathematical model for a chemical process or processes and to make the system exactly specified (i.e. Nf = 0)
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Week 3Weekly Take-Home Assignment
1. Follow all the example modeling exercises in Luyben (1996) chapter 3 page 40 to 74. Practice these example processes.
2. Solve at least 10 end-chapter problems from Luyben (1996) chapter 3 (Compulsory)
Submit before Friday (Feb 7) Curriculum and handouts are posted at:http://faculty.waheed-afzal1.pu.edu.pk/