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List of CAD Lab. Experiments
Sl. No PROBLEM TITLE MATHEMATICAL MODEL SUBJECT AREA
1 Molar Volume and Compressibility
Factor from Van Der Waals Equation
Single Nonlinear Equation Introduction to Ch. E.
2 Steady State Material Balances on a
Separation Train
Simultaneous Linear Equations Introduction to Ch. E.
3 Vapor Pressure Data Representation by
Polynomials and Equations
Polynomial Fitting, Linear and
Nonlinear Regression
Mathematical Methods
4 Reaction Equilibrium for Multiple Gas
Phase Reactions
Simultaneous Nonlinear Equations Thermodynamics
5 Terminal Velocity of Falling Particles Single Nonlinear Equation Fluid Dynamics
6 Unsteady State Heat Exchange in a
Series of Agitated Tanks
Simultaneous ODE’s with known
initial conditions.
Heat Transfer
7 Diffusion with Chemical Reaction in a
One Dimensional Slab
Simultaneous ODE’s with split
boundary conditions.
Mass Transfer
8 Binary Batch Distillation Simultaneous Differential and
Nonlinear Algebraic
Equations
Separation Processes
9 Reversible, Exothermic, Gas Phase
Reaction in a Catalytic Reactor
Simultaneous ODE’s and Algebraic
Equations
Reaction Engineering
10 Dynamics of a Heated Tank with PI
Temperature Control
Simultaneous Stiff ODE’s Process Dynamics and
Control
Modelling & Simulation Lab. Experiments
Sl. No PROBLEM TITLE
1 Simulation of biomass gasification in fluidized bed reactor using
2 Simulation of CO2 Removal from Coal and Gas Fired Power Plants
3 Optimization of crude distillation system
4 Simulation of commercial dimethyl ether production plant
5 Simulation of ethanol production processes based on enzymatic hydrolysis of woody biomass
6 Steady-state simulation of a novel extractive reactor for enzymatic biodiesel production
Computer Aided Design Lab
Chemical Engg. Deptt.
Group No.:
Name(S): 1.
2.
3.
4.
5.
PROBLEM TITLE: Steady State Material Balances on a Separation Train
MATHEMATICAL MODEL: Simultaneous Linear Equations
Answer:
CAD Lab. CH Exp-2 10/01/2018
Group No.:
Name(S): 1.
2.
3.
4.
5.
PROBLEM TITLE: Pressure Drop in Pipe
MATHEMATICAL MODEL: Single Nonlinear Algebraic Equations
Answer:
CAD Lab. CH Exp-3 17/01/2018
Group No.:
Name(S): 1.
2.
3.
4.
5.
PROBLEM TITLE: Initial Value Problems
MATHEMATICAL MODEL: Solution of Single Ordinary Differential Equation
Answer:
CAD Lab. CH Exp-4 17/01/2018
Group No.:
Name(S): 1.
2.
3.
4.
5.
PROBLEM TITLE: Initial Value Problems
MATHEMATICAL MODEL: Solution of Single Ordinary Differential Equation
CAD Lab. CH Exp-4 17/01/2018
Answer:
CAD Lab. CH Exp-5 24/01/2018
Group No.:
Name(S): 1.
2.
3.
4.
5.
PROBLEM TITLE: Initial Value Problems
MATHEMATICAL MODEL: Solution of Simultaneous Ordinary Differential Equations
CAD Lab. CH Exp-5 24/01/2018
PROBLEM:
Answer:
CAD Lab. CH Exp-6 07/02/2018
Group No.:
Name(S): 1. 2. 3.
4. 5.
PROBLEM TITLE: Terminal Velocity
MATHEMATICAL MODEL: Nonlinear Algebraic Equation
CAD Lab. CH Exp-6 07/02/2018
CAD Lab. CH Exp-6 07/02/2018
PROBLEM:
Answer:
CAD Lab. CH Exp-7 21/03/2018
Group No.:
Name(S): 1. 2. 3.
4. 5.
Flow of vapors through relief
Concepts Utilized: Assuming flow condition is choked
Course Useage: relief sizing design
Problem back ground: Normally gases are stored under high pressure. If the gas vents through a
hole or relief device, choked flow condition exist. In such a cases, the mass flow rate of gas is
computed as follows
(Qm)choked=Co AP
√γgc M
RgT ( 2
γ+1)
(γ +1/γ−1)
(1)
(Qm)choked =the discharge mass flow,
Co =discharge coefficient
A =area of discharge
P = Absolute upstream pressure
γ =heat capacity ratio for the gas
gc =Gravitational constant
M = Molecular wt of the gas
Rg = Ideal gas constant
T =Absolute temperature of the gas
To perform relief sizing calculation for the two-phase vents, the mass flux
GT through relief is
computed assuming the choked flow
GT=
Qm
A
=
ΔHv
νfg √ gc
CPTs (2)
Equation-2 is called Equilibrium rate model for low-quality choked flow
Qm =mass flow through the relief
ΔHv =heat of vaporization of the fluid
A =area of the hole
νfg =change in specific volume of the flashing liquid
CP =heat capacity of the fluid
Ts =Absolute saturation temperature of the fluid at set pressure
Leung further modified the equation-2 for homogeneous venting of a reactor
GT=
Qm
A
=0.9Ψ
ΔHv
νfg √ gc
CP Ts (3)
Equation-3 is called homogeneous equilibrium rate model. For a pipe of length 0, Ψ =1
As one know
ΔHv
νfg
=Ts
dP
dT (4)
Equation-3 can be rearrange using equation-4 in finite difference derivative after being approximated
by exact derivative
CAD Lab. CH Exp-7 21/03/2018
GT≃0.9Ψ
ΔP
ΔT √gcTs
CP (5)
ΔP is the over pressure and ΔT is the temperature rise corresponding to over pressure.
The required vent area is computed by solving a particular form of dynamic energy balance equation
A=
mo q
GT (√VΔHv
mo νfg
+√CV ΔT)
2
(6)
Alternative form of equation-6 can be used to find relief area
A=
mo q
GT (√V
mo
Ts
dP
dT
+√CV ΔT
)
2
(7)
mo =Total mass contained within the reactor vessel before relief
q =Exothermic heat release per unit mass
V =Volume of the vessel and
CV = the liquid heat capacity at constant volume.
Exothermic heat release per unit mass can be computed through experimentation by obtained by
Vent Sizing Packaging data, using the following equation
q=
1
2
CV [(dT
dt )s
+(dT
dt )m] (8)
Subscripts s denotes corresponding to the heating rate at set pressure and the m corresponding to
the temperature rise at the maximum turn around pressure.
Problem Statement
Leung9
reported on the data of Huff10
involving a 3500-gal reactor with styrene monomer
undergoing adiabatic polymerization after being heated inadvertently to 70°C. The maximum
allowable working pressure (MAWP) of the vessel is 5 bar. Given the following data,
determine the relief vent diameter required. Assume a set pressure of 4.5 bar and a maximum
pressure of 5.4 bar absolute:
Data:
Volume: 3500 gal=13.16 m3
Reaction Mass=9500 kg
Set temperature=209.4o
C=482.5K
VSP Data
Maximum temperature Tm=219.5o
C=492.7 K
(dT
dt )s =29.6 o
C/min=0.493 K/s
(dT
dt )m =39.7 o
C/min=0.662 K/s
Physical property data
4.5 –bar set 5.4-bar Peak
νf (m3
/kg)
0.001388 0.001414
νg (m3
/kg)
0.08553 0.07278
CP (kJ/kg K)
2.470 2.514
CAD Lab. CH Exp-7 21/03/2018
ΔHv (kJ/kg )
310.6 302.3
CAD Lab. CH Exp-8 28/03/2018
Group No.:
Name(S): 1. 2. 3.
4. 5.
ELECTRICAL CHARGE ACCUMULATION IN A FEED LINE
RESULTING FROM FLUID FLOW.
Numerical method: Solution of a linear algebraic equation.
Concepts Utilized: Streaming current
Course Useage: Controlling of electrostatic hazards
Problem back ground:
A streaming current
Is is the flow of electricity
produced by transferring electrons from one surface
to another by a flowing fluid or solid. When a liquid
or solid flows through a pipe (metal or glass), an
electrostatic charge develops on the streaming
material. This current is analogous to a current in an
electrical circuit. The relation between a liquid
streaming current and the pipe diameter, pipe length,
fluid velocity, and fluid properties is given by
Is=
[10∗10−6
amp
(m/s)2
m2 ](ud)2
[1−exp(−
L
uτ )] (1)
Is is the streaming current (amps),
u is the velocity (m/s),
d is the pipe diameter (m),
L is the pipe length (m), and
τ is the liquid relaxation time (seconds).
The relaxation time is the time required for a charge to dissipate by leakage. It is determined
using
τ =
εr εo
γc (2)
Where
τ is the relaxation time (seconds),
εr is the relative dielectric constant (unitless),
εo is the permittivity constant, that is,
γc is the specific conductivity (mho/cm)
Electrostatic Voltage Drops in the tank feed line can be calculated as V=Is.R and resistance can be computed as
R=
L
γc A , where L and A are the length and area of the conductor respectively. Energy of charged capacitors
and charge accumulated can be calculated using following
J=
QV
2
=
CV
2
2 (3)
Q=Is t (4)
CAD Lab. CH Exp-8 28/03/2018
Problem statement:
Determine the voltage developed between a charging nozzle and a grounded tank, as shown in Figure. Also,
compute the energy stored in the nozzle and the energy accumulated in the liquid. Explain the potential hazards
in this process for a flow rate of
a. 1 gpm
b. 150 gpm
The data are:
Hose length: 20 ft
Hose diameter: 2 in
Liquid conductivity: mho/cm
Dielectric constant: 25.7
Density: 0.88 g/cm3
Capacitance between the two 1-in flanges=20x10-12
coulomb/volt
CAD Lab. CH Exp-9 28/03/2018
Group No.:
Name(S): 1. 2. 3.
4. 5.
Numerical method: Solution of a non-linear algebraic equation.
Concepts Utilized: Minimum Fluidization Velocity
Course Usage: Fluidization Engineering
Problem back ground:
CAD Lab. CH Exp-9 28/03/2018

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List of Computer aided design Lab. Experiments.pdf

  • 1. List of CAD Lab. Experiments Sl. No PROBLEM TITLE MATHEMATICAL MODEL SUBJECT AREA 1 Molar Volume and Compressibility Factor from Van Der Waals Equation Single Nonlinear Equation Introduction to Ch. E. 2 Steady State Material Balances on a Separation Train Simultaneous Linear Equations Introduction to Ch. E. 3 Vapor Pressure Data Representation by Polynomials and Equations Polynomial Fitting, Linear and Nonlinear Regression Mathematical Methods 4 Reaction Equilibrium for Multiple Gas Phase Reactions Simultaneous Nonlinear Equations Thermodynamics 5 Terminal Velocity of Falling Particles Single Nonlinear Equation Fluid Dynamics 6 Unsteady State Heat Exchange in a Series of Agitated Tanks Simultaneous ODE’s with known initial conditions. Heat Transfer 7 Diffusion with Chemical Reaction in a One Dimensional Slab Simultaneous ODE’s with split boundary conditions. Mass Transfer 8 Binary Batch Distillation Simultaneous Differential and Nonlinear Algebraic Equations Separation Processes 9 Reversible, Exothermic, Gas Phase Reaction in a Catalytic Reactor Simultaneous ODE’s and Algebraic Equations Reaction Engineering 10 Dynamics of a Heated Tank with PI Temperature Control Simultaneous Stiff ODE’s Process Dynamics and Control Modelling & Simulation Lab. Experiments Sl. No PROBLEM TITLE 1 Simulation of biomass gasification in fluidized bed reactor using 2 Simulation of CO2 Removal from Coal and Gas Fired Power Plants 3 Optimization of crude distillation system 4 Simulation of commercial dimethyl ether production plant 5 Simulation of ethanol production processes based on enzymatic hydrolysis of woody biomass 6 Steady-state simulation of a novel extractive reactor for enzymatic biodiesel production
  • 2. Computer Aided Design Lab Chemical Engg. Deptt. Group No.: Name(S): 1. 2. 3. 4. 5. PROBLEM TITLE: Steady State Material Balances on a Separation Train MATHEMATICAL MODEL: Simultaneous Linear Equations Answer:
  • 3. CAD Lab. CH Exp-2 10/01/2018 Group No.: Name(S): 1. 2. 3. 4. 5. PROBLEM TITLE: Pressure Drop in Pipe MATHEMATICAL MODEL: Single Nonlinear Algebraic Equations Answer:
  • 4. CAD Lab. CH Exp-3 17/01/2018 Group No.: Name(S): 1. 2. 3. 4. 5. PROBLEM TITLE: Initial Value Problems MATHEMATICAL MODEL: Solution of Single Ordinary Differential Equation Answer:
  • 5. CAD Lab. CH Exp-4 17/01/2018 Group No.: Name(S): 1. 2. 3. 4. 5. PROBLEM TITLE: Initial Value Problems MATHEMATICAL MODEL: Solution of Single Ordinary Differential Equation
  • 6. CAD Lab. CH Exp-4 17/01/2018 Answer:
  • 7. CAD Lab. CH Exp-5 24/01/2018 Group No.: Name(S): 1. 2. 3. 4. 5. PROBLEM TITLE: Initial Value Problems MATHEMATICAL MODEL: Solution of Simultaneous Ordinary Differential Equations
  • 8. CAD Lab. CH Exp-5 24/01/2018 PROBLEM: Answer:
  • 9. CAD Lab. CH Exp-6 07/02/2018 Group No.: Name(S): 1. 2. 3. 4. 5. PROBLEM TITLE: Terminal Velocity MATHEMATICAL MODEL: Nonlinear Algebraic Equation
  • 10. CAD Lab. CH Exp-6 07/02/2018
  • 11. CAD Lab. CH Exp-6 07/02/2018 PROBLEM: Answer:
  • 12. CAD Lab. CH Exp-7 21/03/2018 Group No.: Name(S): 1. 2. 3. 4. 5. Flow of vapors through relief Concepts Utilized: Assuming flow condition is choked Course Useage: relief sizing design Problem back ground: Normally gases are stored under high pressure. If the gas vents through a hole or relief device, choked flow condition exist. In such a cases, the mass flow rate of gas is computed as follows (Qm)choked=Co AP √γgc M RgT ( 2 γ+1) (γ +1/γ−1) (1) (Qm)choked =the discharge mass flow, Co =discharge coefficient A =area of discharge P = Absolute upstream pressure γ =heat capacity ratio for the gas gc =Gravitational constant M = Molecular wt of the gas Rg = Ideal gas constant T =Absolute temperature of the gas To perform relief sizing calculation for the two-phase vents, the mass flux GT through relief is computed assuming the choked flow GT= Qm A = ΔHv νfg √ gc CPTs (2) Equation-2 is called Equilibrium rate model for low-quality choked flow Qm =mass flow through the relief ΔHv =heat of vaporization of the fluid A =area of the hole νfg =change in specific volume of the flashing liquid CP =heat capacity of the fluid Ts =Absolute saturation temperature of the fluid at set pressure Leung further modified the equation-2 for homogeneous venting of a reactor GT= Qm A =0.9Ψ ΔHv νfg √ gc CP Ts (3) Equation-3 is called homogeneous equilibrium rate model. For a pipe of length 0, Ψ =1 As one know ΔHv νfg =Ts dP dT (4) Equation-3 can be rearrange using equation-4 in finite difference derivative after being approximated by exact derivative
  • 13. CAD Lab. CH Exp-7 21/03/2018 GT≃0.9Ψ ΔP ΔT √gcTs CP (5) ΔP is the over pressure and ΔT is the temperature rise corresponding to over pressure. The required vent area is computed by solving a particular form of dynamic energy balance equation A= mo q GT (√VΔHv mo νfg +√CV ΔT) 2 (6) Alternative form of equation-6 can be used to find relief area A= mo q GT (√V mo Ts dP dT +√CV ΔT ) 2 (7) mo =Total mass contained within the reactor vessel before relief q =Exothermic heat release per unit mass V =Volume of the vessel and CV = the liquid heat capacity at constant volume. Exothermic heat release per unit mass can be computed through experimentation by obtained by Vent Sizing Packaging data, using the following equation q= 1 2 CV [(dT dt )s +(dT dt )m] (8) Subscripts s denotes corresponding to the heating rate at set pressure and the m corresponding to the temperature rise at the maximum turn around pressure. Problem Statement Leung9 reported on the data of Huff10 involving a 3500-gal reactor with styrene monomer undergoing adiabatic polymerization after being heated inadvertently to 70°C. The maximum allowable working pressure (MAWP) of the vessel is 5 bar. Given the following data, determine the relief vent diameter required. Assume a set pressure of 4.5 bar and a maximum pressure of 5.4 bar absolute: Data: Volume: 3500 gal=13.16 m3 Reaction Mass=9500 kg Set temperature=209.4o C=482.5K VSP Data Maximum temperature Tm=219.5o C=492.7 K (dT dt )s =29.6 o C/min=0.493 K/s (dT dt )m =39.7 o C/min=0.662 K/s Physical property data 4.5 –bar set 5.4-bar Peak νf (m3 /kg) 0.001388 0.001414 νg (m3 /kg) 0.08553 0.07278 CP (kJ/kg K) 2.470 2.514
  • 14. CAD Lab. CH Exp-7 21/03/2018 ΔHv (kJ/kg ) 310.6 302.3
  • 15. CAD Lab. CH Exp-8 28/03/2018 Group No.: Name(S): 1. 2. 3. 4. 5. ELECTRICAL CHARGE ACCUMULATION IN A FEED LINE RESULTING FROM FLUID FLOW. Numerical method: Solution of a linear algebraic equation. Concepts Utilized: Streaming current Course Useage: Controlling of electrostatic hazards Problem back ground: A streaming current Is is the flow of electricity produced by transferring electrons from one surface to another by a flowing fluid or solid. When a liquid or solid flows through a pipe (metal or glass), an electrostatic charge develops on the streaming material. This current is analogous to a current in an electrical circuit. The relation between a liquid streaming current and the pipe diameter, pipe length, fluid velocity, and fluid properties is given by Is= [10∗10−6 amp (m/s)2 m2 ](ud)2 [1−exp(− L uτ )] (1) Is is the streaming current (amps), u is the velocity (m/s), d is the pipe diameter (m), L is the pipe length (m), and τ is the liquid relaxation time (seconds). The relaxation time is the time required for a charge to dissipate by leakage. It is determined using τ = εr εo γc (2) Where τ is the relaxation time (seconds), εr is the relative dielectric constant (unitless), εo is the permittivity constant, that is, γc is the specific conductivity (mho/cm) Electrostatic Voltage Drops in the tank feed line can be calculated as V=Is.R and resistance can be computed as R= L γc A , where L and A are the length and area of the conductor respectively. Energy of charged capacitors and charge accumulated can be calculated using following J= QV 2 = CV 2 2 (3) Q=Is t (4)
  • 16. CAD Lab. CH Exp-8 28/03/2018 Problem statement: Determine the voltage developed between a charging nozzle and a grounded tank, as shown in Figure. Also, compute the energy stored in the nozzle and the energy accumulated in the liquid. Explain the potential hazards in this process for a flow rate of a. 1 gpm b. 150 gpm The data are: Hose length: 20 ft Hose diameter: 2 in Liquid conductivity: mho/cm Dielectric constant: 25.7 Density: 0.88 g/cm3 Capacitance between the two 1-in flanges=20x10-12 coulomb/volt
  • 17. CAD Lab. CH Exp-9 28/03/2018 Group No.: Name(S): 1. 2. 3. 4. 5. Numerical method: Solution of a non-linear algebraic equation. Concepts Utilized: Minimum Fluidization Velocity Course Usage: Fluidization Engineering Problem back ground:
  • 18. CAD Lab. CH Exp-9 28/03/2018