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Impact of Dispersion of gases from combustion of Coal tar Dissertation Submitted To The department of Chemical Engineering Of National Institute of Technology, Rourkela In partial fulfillment of the requirements For the degree of Bachelor in Technology By V Divya Sree (Roll no. 111CH0425) Under the supervision of Dr. BASUDEB MUNSHI Department of Chemical Engineering National Institute of Technology Rourkela, Rourkela- 769008, Odisha, India

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Page 1: Impact of Dispersion of gases from combustion of Coal tarethesis.nitrkl.ac.in/7932/1/639.pdf1.1 Coal tar Coal tar is a brown or black liquid of extremely high viscosity. It is among

Impact of Dispersion of gases from combustion of Coal tar

Dissertation Submitted

To

The department of Chemical Engineering

Of

National Institute of Technology, Rourkela

In partial fulfillment of the requirements

For the degree of

Bachelor in Technology

By

V Divya Sree

(Roll no. 111CH0425)

Under the supervision of

Dr. BASUDEB MUNSHI

Department of Chemical Engineering

National Institute of Technology Rourkela,

Rourkela- 769008, Odisha, India

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Chemical Engineering

National Institute of Technology Rourkela

Rourkela-769008, Odisha, India.

Certificate

This is to certify that the work in the thesis entitled Impact of Dispersion of gases from

combustion of Coal Tar, by V Divya Sree bearing roll number 111Ch0425 is a record of

an original thesis work carried out by her under my supervision and guidance in partial

fulfillments of the requirements for the award of degree of Bachelor of Technology in

Chemical Engineering

Dr. Basudeb Munshi,

Assistant Professor,

NIT Rourkela.

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Declaration

I hereby declare that all the work contained in this report is my own work unless

otherwise acknowledged. Also, all of my work has not been previously submitted for any

academic degree. All sources of quoted information have been acknowledged by means

of appropriate references

V Divya Sree

111CH0425

Department of Chemical Engineering

National Institute of Technology Rourkela,

Rourkela- 769008, Odisha, India

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Acknowledgement

I would like to express my deepest gratitude to the people who helped me with the work

presented in this dissertation, be it through supplying alternative and usually simplifying

views during scientific discussions, or through moral support during periods of stress and

doubt, or by providing the possibility of embarking on the extraordinary experience of

participating in this adventure.

Firstly, I am deeply indebted to my supervisor, Dr. Basudeb Munshi. He provided an

open and free environment that allowed me to choose this topic and provided valuable

insight that helped me in completing the project. I would also like to acknowledge his

exemplary guidance, monitoring and constant encouragement throughout the course of

this thesis.

I present many thanks to all my professors who over the years have molded me in the

field of Chemical Engineering. I would like to convey my special regards to Mr. Akhilesh

Sir for helping me with the rapid software without whom this project would be almost

incomplete.

I am very much thankful to those, who have been giving inspiration and kind advice

without which, it would not have been possible for me to complete this project work .I

thank all my friends and well-wishers who have rendered help in this endeavor.

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I

ABSTRACT

This project ‘Impact of Dispersion of gases from combustion of Coal tar’ deals with

gases released during combustion of Coal tar and the area affected by these gases. This

depends on many parameters. This is solved by using the software “ANSYS”. For

modeling, the parameters which affect the flow of gases are need to be known. In general,

wind flow, presence of obstacles and temperature may affect the flow.

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II

CONTENTS

Abstract………………………………………………………..……….………...I

List of figures…………………………………………………………………...IV

1. Introduction………………………….……………………………….….........1

1.1 Coal tar ……………………………..………….………………….………….1

1.2 Chemical composition………………………….…………………….……....1

2. Literature Review………………………………………………….….………2

2.1 ANSYS SOFTWARE……………..…………………….…………….………2

2.2 Parameters effecting the flow…………………………………………...…....2

2.3 Summary of review……………………………………………………….…..3

3. Modeling and simulation …………………………………………………….4

3.1 Problem statement……………………………………………….……............4

3.2 Mesh……………………….. ……………………………………….......…....5

3.3 Modeling equations……………………………………………..……………6

3.4 Solution methodology………………………………………….……………..6

4. Effect of wind velocity on dispersion of gases…………………..………........7

4.1 Dispersion of gases at 1m/s.……………………………………………..........7

4.2 Dispersion of gases at 19m/s……...…………………………………………..9

5. Results & Discussion………………………………………………….............11

5.1 Wind velocity at 1m/s…………………………………………………………11

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III

5.2 Wind velocity at 3m/s…………………………………………………………13

5.3 Wind velocity at 5m/s…………………………………………………………14

5.4 Wind velocity at 7m/s…………………………………………………………16

5.5 Wind velocity at 9m/s..…………………………………………………...........18

5.6 Wind velocity at 11m/s…………………………………………………………20

5.7 Wind velocity at 13m/s…………………………………………………………21

5.8 Wind velocity at 15m/s…………………………………………………………23

5.9 Wind velocity at 17m/s…………………………………………………………25

5.10 Wind velocity at 19m/s……………………………………………………......26

6 Conclusion…… ……………………………………………………………….......30

7 References………………………………………………………………………….31

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IV

List of figures

Figure 3.1: Geometry…………………………………………………………………….4

Figure 3.2: Mesh………………………………………………………………………....5

Figure 4.1.1: Contour of SO2 at Wind velocity 1m/s…………..….……………………..7

Figure 4.1.2: Contour of NOx at wind velocity 1m/s…….……………………………...7

Figure 4.1.3: Contour of CO at wind velocity 1m/s……………………………………..8

Figure 4.1.4: Contour of CO2 at wind velocity 1m/s…………………………………….8

Figure 4.2.1: Contour of SO2 at Wind velocity 1m/s…………..….……………………..9

Figure 4.2.2: Contour of NOx at wind velocity 1m/s…….……………………………...9

Figure 4.2.3: Contour of CO at wind velocity 1m/s……………………………………..10

Figure 4.2.4: Contour of CO2 at wind velocity 1m/s…………………………………….10

Figure 5.1.1: Graph of SO2 at Wind velocity 1m/s……………..….…………………….11

Figure 5.1.2: Graph of NOx at wind velocity 1m/s…..….…………….………………...12

Figure 5.1.3: Graph of CO at wind velocity 1m/s………………………………………..12

Figure 5.1.4: Graph of CO2 at wind velocity 1m/s………………………………………13

Figure 5.2.1: Graph of SO2 at Wind velocity 3m/s……………..….……………………13

Figure 5.2.2: Graph ofCO2at wind velocity 3m/s………..……………………………...14

Figure 5.3.1: Graph of CO at wind velocity 5m/s……….………………………………14

Figure 5.3.2: Graph of CO2 at wind velocity 5m/s………………………………………15

Figure 5.3.3: Graph of NOx at Wind velocity 5m/s…………..….………..……………15

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V

Figure 5.3.4: Graph of SO2 at wind velocity 5m/s.…..….…………….…………………16

Figure 5.4.1: Graph of SO2at wind velocity 7m/s……………………………………….16

Figure 5.4.2: Graph of NOx at wind velocity 7m/s.……………………………………..17

Figure 5.4.3: Graph of CO2 at Wind velocity 7m/s……………..….……………………17

Figure 5.4.4: Graph of CO at wind velocity 7m/s………..……………………..………..18

Figure 5.5.1: Graph of SO2 at wind velocity 9m/s……….………………………………18

Figure 5.5.2: Graph of NOx at wind velocity 9m/s………………………………………19

Figure 5.5.3: Graph of CO at Wind velocity 9m/s…………..….………..………………19

Figure 5.5.4: Graph of CO2 at wind velocity 9m/s.…..….….………….…….…………..20

Figure 5.6.1: Graph of SO2 at wind velocity 11m/………………………………………20

Figure 5.6.2: Graph of NOx at wind velocity 11m/s.……………………………………21

Figure 5.7.1: Graph of SO2 at Wind velocity 13m/s……..………..….………………….21

Figure 5.7.2: Graph of CO at wind velocity 13m/s………..……………………………..22

Figure 5.7.3: Graph of CO2 at wind velocity 13m/s………...……………...……………22

Figure 5.7.4: Graph of NOx at wind velocity 13m/s…………………….………………23

Figure 5.8.1: Graph of CO at Wind velocity 15m/s……..………..….…………………..23

Figure 5.8.2: Graph of CO2 at wind velocity 15m/s………..……………………………24

Figure 5.8.3: Graph of NOx at wind velocity 15m/s………...…………...……………...24

Figure 5.8.4: Graph of SO2 at wind velocity 15m/s…………………….……………….25

Figure 5.9.1: Graph of CO2 at Wind velocity 17m/s…………..….……………………..25

Figure 5.9.2: Graph of CO at wind velocity 17m/s……..……………………..…………26

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VI

Figure 5.10.1: Graph of SO2 at Wind velocity 19m/s……..………..……………………26

Figure 5.10.2: Graph of NOx at wind velocity 19m/s………..……..…………………...27

Figure 5.10.3: Graph of CO at wind velocity 19m/s…..…...…………...………………27

Figure 5.10.4: Graph of CO2 at wind velocity 19m/s………………….………………...28

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1. INTRODUCTION

1.1 Coal tar

Coal tar is a brown or black liquid of extremely high viscosity. It is among the

byproducts when coal is carbonized to make coke. This is mixture of Phenols, polycyclic

aromatic hydrocarbons and heterocyclic compounds. The composition of coal tar is

influenced by the origin and composition of coal and also by the nature of distilling

process. As a result, it is referred by many names coal tar, crude coal tar, coal tar pitch,

coal tar creosote.

Combustion of coal tar is burning coal tar in presence of oxygen .The gases released

are Sulphur dioxide, carbon monoxide, carbon dioxide, NOx. Some particulates are also

released like ash.

1.2 Chemical composition (%)

Carbon 92-93

Hydrogen 4.3-4.7

Sulphur 0.3-0.8

Nitrogen 1.7-1.8

Oxygen 0.8-1

Ash content 0.2-0.3

Density 1.2-1.3gm/cm3

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2. LITERATURE REVIEW

This chapter summarizes all the back ground reading done to gain enough

knowledge of software Ansys, parameters affecting the flow of cloud.

2.1 ANSYS

Ansys is an Engineering simulation software. Out of the different programs present,

ANSYSCFD is mostly used. ANSYS CFD is used in systems by simulating fluid Flows

in a virtual environment. This is mostly used in aircraft hydrodynamics, hydro cyclones

etc.

The present project work utilizes ANSYS 15.0 where Workbench is used for the

geometry purpose while the further simulation is done using Fluent 6.2.16. The mass

fraction of different gases and pressure profiles are observed at different velocities of the

wind and at different velocities of the gases coming out. The mass fraction for different

gases at different distances along the horizontally and as well as vertically are obtained

and are checked with ambient conditions.

2.2 PARAMETERS AFFECTING THE FLOW

The gases released generally form a cloud and move. At low concentrations all

the gases are transported and dispersed through the atmosphere in the same way. The

internal cloud buoyancy is the measure of whether the in cloud density is greater than or

less than the ambient or environmental density. If the cloud density is greater than

ambient density, it is called dense. If it is less dense, then it is called buoyant, and it may

rise several hundred meters away

The turbulent dispersion(i.e. rate of speed in lateral ,vertical ,downward

direction)of the cloud about its center of mass depends on atmospheric turbulence in the

atmosphere which itself depends on surface roughness conditions, the wind speed, and

stability(i.e. day or night).because of this the geographic area covered by the cloud will

increase ,thus affecting larger population .Buoyant turbulence is generated by heating of

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3

the ground surface by the sun and its suppressed by cooling of the ground surface at

night.

Urban heat-Because of heat generated by human activities, including industrial

processes, urban or industrial areas is often several degrees warmer than its surroundings.

This causes the cloud to be neutral or unstable.

Aerosols and particles with sizes greater than about 10micrometer will have

appreciable settling velocities. For e.g., cloud of 200 micrometer aerosols released near

the ground will settle to the ground in a few minutes. Particles less than 10 micrometer

have velocities so small that they remain suspended.

2.4 SUMMARY OF REVIEW

This chapter has gone over all the concepts vital to this project in detail. It has covered all

the background knowledge in the field of dispersion of gases that is necessary for the

simulation.

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3. MODELLING AND SIMULATION

3.1 THE PROBLEM STATEMENT

The present project work consists of 3D rectangular area having horizontal distance

of1000m, vertical distance of 3500m and width of 500m. Inside the rectangular area coal

tar is combusted at a temperature of 500k, in an area of 5*5 m at a distance of 50 m from

the flow of wind. Wind is flowing in positive X-direction and considering the different

velocities of wind as 1m/s, 3m/s, 5m/s, 7m/s,9m/s,11m/s,13m/s,15m/s,17m/s,19m/s.

velocities of gases are taken as 1 m/s. Mass fractions of the pollutants (SO2, NO2, CO,

PPM10) coming out are known. Mass diffusivities of different pollutants with respect to

air are also known. For a constant value of gases velocity by varying the wind velocity,

different types of dispersion is observed. The geometry of the problem is created using

Workbench, followed by meshing. The rest of work which includes providing initial and

boundary conditions etc. is done in Fluent. Thus the concentration of pollutants at

different heights and horizontal distance is calculated using ANSYS. Tabulation and

plotting is done to get an idea about the relation among the pollutants concentration and

distance.

Figure 3.1 Geometry of the physical domain with length 1000m, breadth 500 and width

500m

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Emissions of Pollutants (Mass fractions)

SO2- 0.003

NOx- 0.017

CO- 0.058

CO2- 0.92

3.2 MESH

Meshing is basic requirement for the simulation process. To analyse the fluid flow

problems, the flow domains are divided into the smaller subdomains. For the meshing,

fine tetrahedron mesh is done in 3d geometry. After that named selection was done which

was named as inlet, inlet1, symmetry, wall for the entire geometry.

Figure 3.2 Meshed Geometry of the physical domain

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3.3 MODELLING EQUATIONS

3.3.1 Continuity equation

Equation for mass conservation equation or also known as continuity equation is written

as:-

3.3.1

3.3.2 Transport equation for species transport

For the species transport in ANSYS FLUENT it solves the transport equation inside the

domain which is given as :-

3.3.2

3.4 SOLUTION METHODOLOGY

For the simulation process Phase coupled SIMPLE was chosen for the pressure-velocity

coupling. Second order Upwind scheme was chosen for the discretization of partial

differential equation. In the final step of simulation iterations were given which were as

follows:-

Step size – 0.05

Number of steps – 10000

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4. Effect of Wind Velocity on the Dispersion of Gases

4.1 Wind velocity of 1m/s

4.1.1 Dispersion of SO2

Figure 4.1.1 Dispersion ofSulphur dioxide

Contour clearly shows the dispersion of Sulphur dioxide gas .The dispersion is very less.

4.1.2 Dispersion ofNOx

Figure 4.1.2 Dispersion of Nitrogen oxide

Contour clearly shows the dispersion of nitrogen oxide gas .The downstream length

covered by the gas is less.

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4.1.3 Dispersion of CO

Figure 4.1.3 Dispersion of Carbon monoxide

Contour clearly shows the dispersion of carbon monoxide gas.Dispersion is very less and

the mass fraction is maximum near the combusted area and it decreased in downstream

length.

4.1.4 Dispersion of CO2

Figure 4.1.4 Dispersion of Carbon dioxide

The extent of dispersion is less and the mass fraction is maximum near the area where

coal is combusted and it is reduced in the downstream length.

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4.2 Wind velocity of 19m/s

4.2.1 Dispersion of SO2

The contour clearly shows the dispersion and it is very clear that the downstream length

to which the gas had been dispersed is more than that compared to the length covered by

gas at 1m/s.

Figure 4.2.1 Dispersion of Sulphur dioxide

4.2.2 Dispersion of NOx

Figure 4.2.2 Dispersion of Nitrogen oxide

The dispersion is high in this case as compared to that of wind velocity at 1m/s.

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4.2.3 Dispersion of CO

Figure 4.2.3 Dispersion of Carbon monoxide

The contour clearly shows the dispersion and it is very clear that the downstream length

to which the gas had been dispersed is more than that compared to the length covered by

gas at 1m/s.

4.2.4 Dispersion of CO2

Figure 4.2.4 Dispersion of Carbon Dioxide

The dispersion is high in this case as compared to that of wind velocity at 1m/s.Mass

fraction is decreasing in the downstream.

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5. RESULTS & DISCUSSION

Level 1 is taken as ground level .Level 2 is at a distance of 4m from ground level. Level 3

is taken at a distance of 8m from ground level. Level 4 is taken at a distance of 12m from

ground level. Level 5 is taken at a distance of 16m from ground level. Level 6 is taken at

a distance of 25m from ground level.

5.1 Wind velocity at 1m/s

Figure 5.1.1 Sulphur dioxide dispersion

SO2gas is following a particular trend when the inlet velocity is 1m/s at all the levels.

The downstream length affected by the gas is 130m and the maximum mass fraction is

present on ground at a distance of 100m.

0

0.00001

0.00002

0.00003

0.00004

0.00005

0.00006

0.00007

0.00008

0.00009

-10 10 30 50 70 90 110 130 150

mas

s fr

acti

on

Distance(m)

level 1

level 2

level 3

level 4

level 5

level 6

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Figure 5.1.2 NOx dispersion

NOx gas is following a particular trend at all levels and the downstream length affected

by the gas is 130m and the maximum mass fraction is 0.00045 on ground is at a distance

of 100m.The concentration of the gas has been decreasing from level 1 to level 6 and

maximum concentration is at level 1.

Figure 5.1.3 Carbon monoxide dispersion

CO gas is following a particular trend at all levels and the downstream length affected by

the gas is 130m and the maximum mass fraction is 0.0016 on ground is at a distance of

95m.At 25m height the concentration of gas has become zero.

0.00E+00

1.00E-04

2.00E-04

3.00E-04

4.00E-04

5.00E-04

-10 10 30 50 70 90 110 130 150

mas

s fr

acti

on

Distance(m)

level 1

level 2

level 3

level 4

level 5

level 6

0.00E+00

2.00E-04

4.00E-04

6.00E-04

8.00E-04

1.00E-03

1.20E-03

1.40E-03

1.60E-03

1.80E-03

-10 10 30 50 70 90 110 130 150

mas

s fr

acti

on

Distance(m)

level 1

level 2

level 3

level 4

level 5

level 6

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Figure 5.1.4 Carbon dioxide dispersion

CO2 gas is following a particular trend at all levels and the downstream length affected

by the gas is 140m and the maximum mass fraction is 0.025 on ground is at a distance of

97m.The concentration of the gas has been decreasing from level 1 to level 6 and

maximum concentration is at level 1.

5.2 Wind velocity at 3m/s

Figure 5.2.1 Sulphur dioxide dispersion

SO2 gas had moved 270m downstream distance and the maximum mass fraction is

0.000017 on ground and the concentration has been decreasing as the height has been

increasing.

0.00E+00

5.00E-03

1.00E-02

1.50E-02

2.00E-02

2.50E-02

3.00E-02

-10 10 30 50 70 90 110 130 150

mas

s fr

acti

on

Distance(m)

level 1

level 2

level 3

level 4

level 5

level 6

0

0.000005

0.00001

0.000015

0.00002

0 50 100 150 200 250 300mas

s fr

acti

on

lenth(m)

level 1

level 2

level 3

level 4

level 5

level 6

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Figure 5.2.2 Carbon dioxide dispersion

CO2 gas had moved 260m downstream distance and the maximum mass fraction is

0.00032 on ground and the concentration has been decreasing as the height has been

increasing. The distance covered by the gas has increased as we increased the velocity.

5.3 Wind velocity at 5m/s

Figure 5.3.1 Carbon monoxide dispersion

CO gas had moved 350m downstream distance and the maximum mass fraction is 0.0003

on ground and the concentration has been decreasing as the height has been increasing

and also in the downstream distance.

0

0.00005

0.0001

0.00015

0.0002

0.00025

0.0003

0.00035

0 50 100 150 200 250 300

mas

s fr

acti

on

downstream legth(m)

levell 1

level 2

level 3

level 4

level 5

level 6

0

0.00005

0.0001

0.00015

0.0002

0.00025

0.0003

0.00035

0 50 100 150 200 250 300 350

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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Figure 5.3.2 Carbon dioxide dispersion

CO2 gas had moved 360m downstream distance and the maximum mass fraction is

0.0049 on ground and the concentration has been decreasing as the height has been

increasing. The distance covered by the gas has increased as we increased the velocity.

Figure 5.3.3 Nitrogen oxide dispersion

NOx gas had moved 370m downstream distance and the maximum mass fraction is

0.00009 on ground and the concentration has been decreasing as the height has been

increasing and the concentration at level 6 is minimum which is nearly 0.00001.

0.00E+005.00E-041.00E-031.50E-032.00E-032.50E-033.00E-033.50E-034.00E-034.50E-035.00E-03

-50 50 150 250 350

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

0

0.00001

0.00002

0.00003

0.00004

0.00005

0.00006

0.00007

0.00008

0.00009

0.0001

-30 20 70 120 170 220 270 320 370

mas

s fr

acti

on

length(m)

level 1

level 2

level 5

level 3

level 4

level 6

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Figure 5.3.4 Sulphur dioxide dispersion

SO2 gas had moved 370m downstream distance and the maximum mass fraction is

0.000015 on ground and the concentration at level 6 is minimum which is nearly

0.000002.

5.4 Wind velocity at 7m/s

Figure 5.4.1 Sulphur dioxide dispersion

SO2 gas covered a distance of 550m and the maximum mass fraction is 0.000027 on the

ground and the concentration is decreasing downstream.

0

0.000002

0.000004

0.000006

0.000008

0.00001

0.000012

0.000014

0.000016

0.000018

0 50 100 150 200 250 300 350

mas

s fr

acti

on

length(m)

level 1

level 2

leevl 3

level 4

level 5

level 6

0

0.000005

0.00001

0.000015

0.00002

0.000025

0.00003

0 100 200 300 400 500 600

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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17

Figure 5.4.2 Nitrogen oxide dispersion

NOx gas had moved 550m downstream distance and the maximum mass fraction is

0.00015 on ground and the distance covered by the gas is more compared to the

dispersion at wind velocity less than 7m/s.

Figure 5.4.3 Carbon dioxide dispersion

CO2gas had moved 550m downstream distance and the maximum mass fraction is 0.009

on ground at a distance of 100m and the concentration had been decreasing as it is

moving downstream.

0

0.00005

0.0001

0.00015

0.0002

0 100 200 300 400 500 600

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

0.00E+00

1.00E-03

2.00E-03

3.00E-03

4.00E-03

5.00E-03

6.00E-03

7.00E-03

8.00E-03

9.00E-03

1.00E-02

0 100 200 300 400 500 600

mas

s fr

cati

on

downstream length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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18

Figure 5.4.4 Carbon monoxide dispersion

CO gas had moved 550m downstream distance and the maximum mass fraction is

0.00055 on ground and the distance covered by the gas is more compared to the

dispersion at wind velocity less than 7m/s. and the trend followed by the gas in all levels

is almost the same.

5.5 Wind velocity at 9m/s

Figure 5.5.1 Sulphur dioxide dispersion

SO2 gas is following a particular trend at all levels and the downstream length affected by

the gas is almost 700m and the maximum mass fraction is 0.000045 on ground is at a

distance of 100m.At 25m height the concentration of gas is not so less compared to

ground level.

-1E-04

1.2E-18

0.0001

0.0002

0.0003

0.0004

0.0005

0.0006

0 100 200 300 400 500 600

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

0

0.000005

0.00001

0.000015

0.00002

0.000025

0.00003

0.000035

0.00004

0.000045

0.00005

0 100 200 300 400 500 600 700 800

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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19

Figure 5.5.2 Nitrogen oxide dispersion

NOx gas is following a particular trend at all levels and the downstream length affected

by the gas is 630m and the maximum mass fraction is 0.00025 on ground is at a distance

of 95m.The concentration of the gas is decreasing as the height is increasing.

Figure 5.5.3 Carbon monoxide dispersion

CO gas is following a particular trend at all levels and the downstream length affected by

the gas is nearly 690m and the maximum mass fraction is 0.0009 on ground is at a

distance of 95m.

0

0.00005

0.0001

0.00015

0.0002

0.00025

0.0003

0 200 400 600 800

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5+Sheet2!$E$4

level 6

0

0.0001

0.0002

0.0003

0.0004

0.0005

0.0006

0.0007

0.0008

0.0009

0.001

0 100 200 300 400 500 600 700 800

mas

s fr

acti

on

length(m)

level 6

level 1

level 2

level 3

level 4

level 5

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20

Figure 5.5.4 Carbon dioxide dispersion

CO gas is following a particular trend at all levels and the downstream length affected by

the gas is 6900m and the maximum mass fraction is 0.014 on ground is at a distance of

100m.The dispersion to higher levels is increasing compared to previous cases where

wind velocity is less than 9m/s.

5.6 Wind velocity at 11m/s

Figure 5.6.1 Sulphur dioxide dispersion

SO2 gas is following a particular trend at all levels and the downstream length affected by

gas is 7000m and the maximum mass fraction is 0.00002 on ground is at a distance of

98m.At 25m height also dispersion is quiet good with mass fraction 0.000005.

0

0.002

0.004

0.006

0.008

0.01

0.012

0.014

0.016

0 100 200 300 400 500 600 700 800

mas

s fr

acti

on

length(m)

level 6

level 1

level 2

level 3

level 4

level 5

0

0.000005

0.00001

0.000015

0.00002

0.000025

0 100 200 300 400 500 600 700 800

mas

s fr

acti

on

e

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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21

Figure 5.6.2 Nitrogen oxide dispersion

Downstream length affected by the gas is 7000m and the maximum mass fraction is

0.00012 on grounds is at a distance of 98m.As the concentration of gas is very low and as

the velocity is more the gas at level 2 and level 3 had become zero at a distance of 300m.

5.7 Wind velocity at 13 m/s

Figure 5.7.1 Carbon monoxide dispersion

The downstream length affected by the gas is nearly 900m and the maximum mass

fraction is 0.00023 on ground.

0

0.00002

0.00004

0.00006

0.00008

0.0001

0.00012

0 100 200 300 400 500 600 700 800

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

0

0.00005

0.0001

0.00015

0.0002

0.00025

-100 100 300 500 700 900

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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22

Figure 5.7.2 Carbon dioxide dispersion

The downstream length affected by the gas is nearly 900m and the maximum mass

fraction is 0.0035 on ground and levels which have less concentration initially have

settled to ground at a distance of 300m.

Figure 5.7.3 Nitrogen oxide dispersion

The downstream length affected by the gas is nearly 900m and the maximum mass

fraction is 0.000065 on ground and the concentration has been decreasing as the height is

increasing.

0.00E+00

5.00E-04

1.00E-03

1.50E-03

2.00E-03

2.50E-03

3.00E-03

3.50E-03

4.00E-03

-100 100 300 500 700 900

mas

s fr

acti

on

length

level 1

level 2

level 3

level 4

level 5

level 6

0

0.00001

0.00002

0.00003

0.00004

0.00005

0.00006

0.00007

0.00008

-100 100 300 500 700 900

mas

s fr

acti

on

length(M)

level 1

level 2

level 3

level 4

level 5

level 6

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23

Figure 5.7.4 Sulphur dioxide dispersion

The gas is following almost the same trend except at level 4 and the length covered by

gas is almost 900m.

5.8 Wind velocity at 15m/s

Figure 5.8.1 Sulphur dioxide dispersion

The downstream length affected by the gas is 900m and the maximum mass fraction is

0.0016 on ground. At 25m height the concentration of gas is nearly 0.000002.

0

0.000002

0.000004

0.000006

0.000008

0.00001

0.000012

0.000014

-100 100 300 500 700 900

mas

s fr

acti

on

length(m)

level 1

level 5

level 2

level 3

level 4

level 6

0

0.000002

0.000004

0.000006

0.000008

0.00001

0.000012

0.000014

0.000016

0.000018

0 50 100 150 200 250 300 350 400

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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24

Figure 5.8.2 Carbon dioxide dispersion

The downstream length affected by the gas is greater than 900m, and the maximum mass

fraction is 0.0003.The concentration of the gas is decreasing as the height increases.

Figure 5.8.3 Carbon dioxide dispersion

The downstream length affected by the gas is greater than 900m and the maximum mass

fraction is 0.0005 on ground .At 25m height the concentration of gas has become zero at

a distance nearly 400m.

0

0.00005

0.0001

0.00015

0.0002

0.00025

0.0003

0.00035

0 200 400 600 800 1000

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

0.00E+00

1.00E-03

2.00E-03

3.00E-03

4.00E-03

5.00E-03

6.00E-03

0 200 400 600 800 1000

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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25

Figure 5.8.4 Nitrogen oxide dispersion

The gas affects downstream length greater than 900m and the concentration is decreasing

down the downstream length.

5.9 Wind velocity at 17m/s

Figure 5.9.1 Carbon monoxide dispersion

The downstream length covered by the gas is 1000m, as the initial concentration is less

the concentration at the last level is less and it is settling on ground at a distance of 400m.

0

0.00001

0.00002

0.00003

0.00004

0.00005

0.00006

0.00007

0.00008

0.00009

0.0001

0 200 400 600 800 1000

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

0

0.00005

0.0001

0.00015

0.0002

0.00025

0.0003

0 200 400 600 800 1000

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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26

Figure 5.9.2 Sulphur dioxide dispersion

The downstream length covered by the gas is 1000m and as the height is increasing the

concentration has been decreasing.

5.10 Wind velocity at 19m/s

Figure 5.10.1 Sulphur dioxide dispersion

The gas is moving a downstream length greater than 1000m and at this velocity it is not

getting settled on ground and the maximum concentration is on ground and the value is

nearly 0.000011.

0

0.000002

0.000004

0.000006

0.000008

0.00001

0.000012

0.000014

0 200 400 600 800 1000

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

0

0.000002

0.000004

0.000006

0.000008

0.00001

0.000012

0 200 400 600 800 1000

mas

s fr

acti

on

length

level 1

level 2

level 3

level 4

level 5

level 6

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27

Figure 5.10.2 Nitrogen oxide dispersion

The gas is moving a downstream length greater than 1000m and at this velocity it is not

getting settled on ground and the maximum concentration is on ground and the value is

nearly 0.00006.

Figure 5.10.3 Carbon monoxide dispersion

The gas is moving a downstream length greater than 1000m and at this velocity gas is

dispersed throughout instead of settling on ground.

0

0.00001

0.00002

0.00003

0.00004

0.00005

0.00006

0.00007

0 200 400 600 800 1000

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

-5E-05

6E-19

5E-05

0.0001

0.00015

0.0002

0.00025

0 200 400 600 800 1000

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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28

Figure 5.10.4 Carbon dioxide dispersion

The gas is moving a downstream length greater than 1000m and as Carbon dioxide

concentration is more, gas present at different levels is going beyond 1000m which is not

the case for NOx ,CO.

0.00E+00

5.00E-04

1.00E-03

1.50E-03

2.00E-03

2.50E-03

3.00E-03

3.50E-03

4.00E-03

0 200 400 600 800 1000

mas

s fr

acti

on

length(m)

level 1

level 2

level 3

level 4

level 5

level 6

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29

At 1m/s wind velocity, gases had settled on ground at a distance of 150 m. At all levels,

gases followed a particular trend. As the wind velocity is increased to 3m/s, 5m/s, gases

had settled at a distance of 250 m, 350 m following similar trend at different levels. Level

6 which is at the maximum height compared to others has a very low concentration of

gases compared to all other levels. At wind velocity 6m/s, 7m/s gases had settled at a

distance of 550m, 650m.As the height from the ground level is increasing, the

concentration of gases is decreasing. At wind velocity 9m/s, 11m/s gases are covering

downstream distance of nearly 800m. As the wind velocity is increased above 13m/s,

gases crossed a downstream distance of 900m.Gases which are near to ground is settling

vastly compare to gases which are at a height more than 10m .At the max wind velocity

of 19m/s gases had crossed 1000m.As carbon dioxide concentration is more than Sulphur

dioxide, nitrogen oxide, carbon monoxide, this gas at 1000m/s wind velocity had crossed

1000m downstream length at different levels whereas for other gases they have been

dispersed and didn’t settle .As the wind velocity is increased gas concentration near to the

ground has been decreasing and as the height is increasing the concentration has been

increasing. As the wind velocity is increased from 1m/s to 9m/s particular gas at different

levels have been following the same trend whereas as the wind velocity is increased from

13m/s to 19m/s there is no such particular trend and the gas at different levels started

settling randomly. The maximum mass fraction for all the gases at wind velocities less

than 9m/s is at the ground level and at a distance of 90-100m roughly. As the Wind

velocity has been increasing the concentration of the gases at the level 6 has been

increasing.

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30

CONCLUSION:

As the velocity is increased from 1m/s to 19m/s it is clear that the gases released from

combustion of coal tar are covering more distance in down wind direction. The maximum

concentrations of gases on ground level are mostly observed at a distance less than 100m.

The concentration of the gases at a particular wind velocity has been decreasing as the

height increases. As the velocity is increased from 1m/s to 9 m/s, concentration profiles

are following a particular path whereas, as the velocity is increased beyond 11 m/s,

ground level gases and gases at level 1 concentration are becoming zero as they are

travelling half the downstream distance travelled by other gases at the same velocity. As

the velocity is increased the concentration of gas settling on ground has decreased.

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31

6. REFERENCES

[1]. http://en.wikipedia.org/wiki/Coal_tar

[2]. http://en.wikipedia.org/wiki/Atmospheric_dispersion_modeling

[3].Stevan R Henna and Rex E Britter (2002), ‘Wind flow and dispersion at industrial and

urban sites’ page 78

[4].Brunekreef B. and Holgate, S.T. (2002), ‘Air pollution and health’, page 213

[5].Guidelines for Chemical Process Quantitative Risk Analysis, By Center for

Chemical Process Safety (CCPS), page 65

[6]. Dennis P. Nolan, ‘Handbook of Fire and Explosion Protection Engineering

Principles’, page 51

[7]. Turner D B (1994), ‘Workbook of Atmospheric Dispersion Estimates: An

Introduction to Dispersion Modeling’ (2nd Edition) CRC Press.

[8].Lutgens F K and Tarbuck E J (1995) ‘The Atmosphere: An Introduction to

Meteorology (6th Edition)’, page 97

[9]. http://www.csun.edu/~vchsc00b/468/EOH468WK4.pdf

[10]. Guidelines for Consequence Analysis of Chemical Releases

By Center for Chemical Process Safety (CCPS), page 77