This document provides information about computer modeling of electrostatic precipitators (ESPs). It begins with an introduction to ESPs, describing how they work to separate particles from gas streams. It then discusses different ESP types (dry and wet), installation, charging mechanisms, particle mobility, resistivity factors, and software used to model and control air pollution using ESPs. The document also includes C programming code examples for modeling parallel plate and cylindrical ESP designs.
Calculation of an Ammonia Plant Energy Consumption: Gerard B. Hawkins
Calculation of an Ammonia Plant Energy Consumption:
Case Study: #06023300
Plant Note Book Series: PNBS-0602
CONTENTS
0 SCOPE
1 CALCULATION OF NATURAL GAS PROCESS FEED CONSUMPTION
2 CALCULATION OF NATURAL GAS PROCESS FUEL CONSUMPTION
3 CALCULATION OF NATURAL GAS CONSUMPTION FOR PILOT BURNERS OF FLARES
4 CALCULATION OF DEMIN. WATER FROM DEMIN. UNIT
5 CALCULATION OF DEMIN. WATER TO PACKAGE BOILERS
6 CALCULATION OF MP STEAM EXPORT
7 CALCULATION OF LP STEAM IMPORT
8 DETERMINATION OF ELECTRIC POWER CONSUMPTION
9 DETERMINATION OF THE TOTAL ENERGY CONSUMPTION OF THE AMMONIA PLANT ISBL
10 ADJUSTMENT OF ELECTRIC POWER CONSUMPTION FOR TEST RUN CONDITIONS
11 CALCULATION OF AMMONIA SHARE IN MP STEAM CONSUMPTION IN UTILITIES
12 CALCULATION OF AMMONIA SHARE IN ELECTRIC POWER CONSUMPTION IN UTILITIES
13 DETERMINATION OF THE TOTAL ENERGY CONSUMPTION OF THE AMMONIA PLANT OSBL
14 DETERMINATION OF THE TOTAL ENERGY CONSUMPTION OF THE AMMONIA PLANT
Calculation of an Ammonia Plant Energy Consumption: Gerard B. Hawkins
Calculation of an Ammonia Plant Energy Consumption:
Case Study: #06023300
Plant Note Book Series: PNBS-0602
CONTENTS
0 SCOPE
1 CALCULATION OF NATURAL GAS PROCESS FEED CONSUMPTION
2 CALCULATION OF NATURAL GAS PROCESS FUEL CONSUMPTION
3 CALCULATION OF NATURAL GAS CONSUMPTION FOR PILOT BURNERS OF FLARES
4 CALCULATION OF DEMIN. WATER FROM DEMIN. UNIT
5 CALCULATION OF DEMIN. WATER TO PACKAGE BOILERS
6 CALCULATION OF MP STEAM EXPORT
7 CALCULATION OF LP STEAM IMPORT
8 DETERMINATION OF ELECTRIC POWER CONSUMPTION
9 DETERMINATION OF THE TOTAL ENERGY CONSUMPTION OF THE AMMONIA PLANT ISBL
10 ADJUSTMENT OF ELECTRIC POWER CONSUMPTION FOR TEST RUN CONDITIONS
11 CALCULATION OF AMMONIA SHARE IN MP STEAM CONSUMPTION IN UTILITIES
12 CALCULATION OF AMMONIA SHARE IN ELECTRIC POWER CONSUMPTION IN UTILITIES
13 DETERMINATION OF THE TOTAL ENERGY CONSUMPTION OF THE AMMONIA PLANT OSBL
14 DETERMINATION OF THE TOTAL ENERGY CONSUMPTION OF THE AMMONIA PLANT
Hazop study on sewage treatment plant at educational institutioneSAT Publishing House
IJRET : International Journal of Research in Engineering and Technology is an international peer reviewed, online journal published by eSAT Publishing House for the enhancement of research in various disciplines of Engineering and Technology. The aim and scope of the journal is to provide an academic medium and an important reference for the advancement and dissemination of research results that support high-level learning, teaching and research in the fields of Engineering and Technology. We bring together Scientists, Academician, Field Engineers, Scholars and Students of related fields of Engineering and Technology
Episode 3 : Production of Synthesis Gas by Steam Methane ReformingSAJJAD KHUDHUR ABBAS
Episode 3 : Production of Synthesis Gas by Steam Methane Reforming
History of Synthesis Gas
In 1780, Felice Fontana discovered that combustible gas develops if water vapor is passed over carbon at temperatures over 500 °C. This CO and H2 containing gas was called water gas and mainly used for lighting purposes in the19th century.
As of the beginning of the 20th century, H2/CO-mixtures were used for syntheses of hydrocarbons and then, as a consequence, also called synthesis gas.
Haber and Bosch discovered the synthesis of ammonia from H2 and N2 in 1910 and the first industrial ammonia synthesis plant was commissioned in 1913.
The production of liquid hydrocarbons and oxygenates from syngas conversion over iron catalysts was discovered in 1923 by Fischer and Tropsch.
Much of the syngas conversion processes were being developed in Germany during the first and second world wars at a time when natural resources were becoming scare and alternative routes for hydrogen production, ammonia synthesis, and transportation fuels were a necessity.
In 1943/44, this was applied for large-scale production of artificial fuels from synthesis gas in Germany.
Heat/light/electrical energy is out today’s necessity and has scarcity also. Energy conservation is key requirement of any industry at all times.
In general, industries use heat energy for conservation of raw material to finished product. The source of heat energy is generally saturated or super heated steam. The steam generation is common use one boiler with carity of fuels. Whatever may be the fuel the generation should be as economy as possible which adds to the product cost. Further the usage of steam and recycling steam condensate back to boiler is an art depending on plant layouts.
In this project the steam generator is water tube boiler fired with rice husk. The steam is transferred to the tyre/tube moulds where tyres/tubes are cured while the heat is rejected to the tyres the condensate forms and this condensate is put back to the boiler. While doing so the steam is also stopped back to boiler without rejecting complete heat to the product. This gets flashed into atmosphere at feed water tank. The science of separation of condensate from steam saves energy. Better the separation more the fuel conservation.
In the steam generator the fuel is burnt to heat the water and form steam. This fuel burnt flue gas carries lot of energy, out through chimney. Prior to exhausting through the heat left in flue need to be recovered, through heat recovery mechanisms’. In this project an air-preheater condensate heat recovery unit is the major energy consuming station.
Reactor and Catalyst Design
0 INTRODUCTION/PURPOSE
1 SCOPE
2 FIELD OF APPLICATION
3 DEFINITIONS
4 CATALYST DESIGN
4.1 Equivalent Pellet Diameter
4.2 Voidage
4.3 Pellet Density
5 REACTOR DESIGN
6 CATALYST SUPPORT
6.1 Choice of Support
TABLES
1 CATALYST SUPPORT SHAPES
2 SECONDARY REFORMER SPREADSHEET
FIGURES
1 GRAPH OF EFFECTIVENESS v THIELE MODULUS
2 VARIATION OF COSTS WITH CATALYST SIZE
3 VARIATION OF COSTS WITH CATALYST BED VOIDAGE
4 VARIATION OF COSTS WITH VESSEL DIAMETER
Capacity Enhancement of Ammonia Production By The Revamping of Ammonia.
In this project, we find conversion and temperature profile of a two catalyst bed with one interbed heat exchanger ammonia converter and a three catalyst bed with two interbed heat exchanger ammonia converter both have radial flow by using a pseudo homogeneous two dimensional mathematical model on the basis of principle of conservation of mass and energy balance with the help of MATLAB pde solver.We conclude that a three catalyst bed ammonia converter give a higher conversion and lower pressure drop compare to the two catalyst bed ammonia converter for the same volume of catalyst bed and same amount of feed stock.
Flue gas desulfurization is commonly known as FGD and is the technology used for removing sulfur dioxide (SO2) from the exhaust combustion flue gases of power plants that burn coal or oil to produce steam for the turbines that drive their electricity generators.
sufficient method of hydrogen production by water gas shift reactions MUKULsethi5
today energy production in big race, because population and technology increasing rate is very fast,
we discussed hydrogen as good energy source and some synthesis method of hydrogen gas and major focus on water gas shift reaction
#water, #watergasshiftreaction,
#energy
#nanoparticle
#property_of_nanopartical
Hazop study on sewage treatment plant at educational institutioneSAT Publishing House
IJRET : International Journal of Research in Engineering and Technology is an international peer reviewed, online journal published by eSAT Publishing House for the enhancement of research in various disciplines of Engineering and Technology. The aim and scope of the journal is to provide an academic medium and an important reference for the advancement and dissemination of research results that support high-level learning, teaching and research in the fields of Engineering and Technology. We bring together Scientists, Academician, Field Engineers, Scholars and Students of related fields of Engineering and Technology
Episode 3 : Production of Synthesis Gas by Steam Methane ReformingSAJJAD KHUDHUR ABBAS
Episode 3 : Production of Synthesis Gas by Steam Methane Reforming
History of Synthesis Gas
In 1780, Felice Fontana discovered that combustible gas develops if water vapor is passed over carbon at temperatures over 500 °C. This CO and H2 containing gas was called water gas and mainly used for lighting purposes in the19th century.
As of the beginning of the 20th century, H2/CO-mixtures were used for syntheses of hydrocarbons and then, as a consequence, also called synthesis gas.
Haber and Bosch discovered the synthesis of ammonia from H2 and N2 in 1910 and the first industrial ammonia synthesis plant was commissioned in 1913.
The production of liquid hydrocarbons and oxygenates from syngas conversion over iron catalysts was discovered in 1923 by Fischer and Tropsch.
Much of the syngas conversion processes were being developed in Germany during the first and second world wars at a time when natural resources were becoming scare and alternative routes for hydrogen production, ammonia synthesis, and transportation fuels were a necessity.
In 1943/44, this was applied for large-scale production of artificial fuels from synthesis gas in Germany.
Heat/light/electrical energy is out today’s necessity and has scarcity also. Energy conservation is key requirement of any industry at all times.
In general, industries use heat energy for conservation of raw material to finished product. The source of heat energy is generally saturated or super heated steam. The steam generation is common use one boiler with carity of fuels. Whatever may be the fuel the generation should be as economy as possible which adds to the product cost. Further the usage of steam and recycling steam condensate back to boiler is an art depending on plant layouts.
In this project the steam generator is water tube boiler fired with rice husk. The steam is transferred to the tyre/tube moulds where tyres/tubes are cured while the heat is rejected to the tyres the condensate forms and this condensate is put back to the boiler. While doing so the steam is also stopped back to boiler without rejecting complete heat to the product. This gets flashed into atmosphere at feed water tank. The science of separation of condensate from steam saves energy. Better the separation more the fuel conservation.
In the steam generator the fuel is burnt to heat the water and form steam. This fuel burnt flue gas carries lot of energy, out through chimney. Prior to exhausting through the heat left in flue need to be recovered, through heat recovery mechanisms’. In this project an air-preheater condensate heat recovery unit is the major energy consuming station.
Reactor and Catalyst Design
0 INTRODUCTION/PURPOSE
1 SCOPE
2 FIELD OF APPLICATION
3 DEFINITIONS
4 CATALYST DESIGN
4.1 Equivalent Pellet Diameter
4.2 Voidage
4.3 Pellet Density
5 REACTOR DESIGN
6 CATALYST SUPPORT
6.1 Choice of Support
TABLES
1 CATALYST SUPPORT SHAPES
2 SECONDARY REFORMER SPREADSHEET
FIGURES
1 GRAPH OF EFFECTIVENESS v THIELE MODULUS
2 VARIATION OF COSTS WITH CATALYST SIZE
3 VARIATION OF COSTS WITH CATALYST BED VOIDAGE
4 VARIATION OF COSTS WITH VESSEL DIAMETER
Capacity Enhancement of Ammonia Production By The Revamping of Ammonia.
In this project, we find conversion and temperature profile of a two catalyst bed with one interbed heat exchanger ammonia converter and a three catalyst bed with two interbed heat exchanger ammonia converter both have radial flow by using a pseudo homogeneous two dimensional mathematical model on the basis of principle of conservation of mass and energy balance with the help of MATLAB pde solver.We conclude that a three catalyst bed ammonia converter give a higher conversion and lower pressure drop compare to the two catalyst bed ammonia converter for the same volume of catalyst bed and same amount of feed stock.
Flue gas desulfurization is commonly known as FGD and is the technology used for removing sulfur dioxide (SO2) from the exhaust combustion flue gases of power plants that burn coal or oil to produce steam for the turbines that drive their electricity generators.
sufficient method of hydrogen production by water gas shift reactions MUKULsethi5
today energy production in big race, because population and technology increasing rate is very fast,
we discussed hydrogen as good energy source and some synthesis method of hydrogen gas and major focus on water gas shift reaction
#water, #watergasshiftreaction,
#energy
#nanoparticle
#property_of_nanopartical
Una descripción de la ruta de la investigación desde la perspectiva de la Fesc, que permite entender la importancia de la difusión y la divulgación cientifica
AIR POLLUTION CONTROL course material by Prof S S JAHAGIRDAR,NKOCET,SOLAPUR for BE (CIVIL ) students of Solapur university. Content will be also useful for SHIVAJI and PUNE university students
Application of Dielectric Spectroscopy to Monitor Insulating Materials ahmdfurkan
PDC measurements, it was found that polarization and depolarization currents increase with temperature increase. Also, the shape of polarization current changes as temperature increases
Drying of the transformer shows a significant reduction of the polarization/depolarization currents.
Moisture and aging have great effect on dielectric response of oil-paper insulation in frequency domain both of them will cause the increase of tan δ
Diagnostics of oil-paper insulation based on Frequency Domain Spectroscopy has great advantage over traditional techniques for its simple operation and non-destructive
Impedance Spectroscopy Analysis of a Liquid Tin Anode Fuel Cell in Voltage Re...AEIJjournal2
A concept of a liquid tin anode-indirect carbon air fuel cell (LTA-ICFC) are described. Experimental
setups for analysis of LTA-ICFC polarisations of an operational electrochemical reactor of the LTA-ICFC
are presented. Results from Electrochemical Impedance Spectroscopy (EIS) Analysis of the electrochemical
reactor of the LTA-ICFC are shown and analysed.The rate-determining step of the system is concluded.
The charge-transfer resistance did not show considerable differences at 700-800 °C. This can be implied
that the charge-transfer resistance is not the rate-limiting step of the transport processes of the fuel cell.
The increase of the Warburg impedance concurrently with the resistance to fit mass-transport loss (R3)
suggests that the rate-limiting step for the LTA-ICFC in voltage recovery mode is the diffusion of the oxide
ions through SnO2 layer. The increment of mass transport lost, R3, of the cell causes the slowly increase of
the cell’s voltage over the voltage from 0.7-0.8 V at 700, 750, and 800 °C.
IMPEDANCE SPECTROSCOPY ANALYSIS OF A LIQUID TIN ANODE FUEL CELL IN VOLTAGE RE...AEIJjournal2
A concept of a liquid tin anode-indirect carbon air fuel cell (LTA-ICFC) are described. Experimental
setups for analysis of LTA-ICFC polarisations of an operational electrochemical reactor of the LTA-ICFC
are presented. Results from Electrochemical Impedance Spectroscopy (EIS) Analysis of the electrochemical
reactor of the LTA-ICFC are shown and analysed.The rate-determining step of the system is concluded.
The charge-transfer resistance did not show considerable differences at 700-800 °C. This can be implied
that the charge-transfer resistance is not the rate-limiting step of the transport processes of the fuel cell.
The increase of the Warburg impedance concurrently with the resistance to fit mass-transport loss (R3)
suggests that the rate-limiting step for the LTA-ICFC in voltage recovery mode is the diffusion of the oxide
ions through SnO2 layer. The increment of mass transport lost, R3, of the cell causes the slowly increase of
the cell’s voltage over the voltage from 0.7-0.8 V at 700, 750, and 800 °C.
Impedance Spectroscopy Analysis of a Liquid Tin Anode Fuel Cell in Voltage Re...AEIJjournal2
A concept of a liquid tin anode-indirect carbon air fuel cell (LTA-ICFC) are described. Experimental
setups for analysis of LTA-ICFC polarisations of an operational electrochemical reactor of the LTA-ICFC
are presented. Results from Electrochemical Impedance Spectroscopy (EIS) Analysis of the electrochemical
reactor of the LTA-ICFC are shown and analysed.The rate-determining step of the system is concluded.
The charge-transfer resistance did not show considerable differences at 700-800 °C. This can be implied
that the charge-transfer resistance is not the rate-limiting step of the transport processes of the fuel cell.
The increase of the Warburg impedance concurrently with the resistance to fit mass-transport loss (R3)
suggests that the rate-limiting step for the LTA-ICFC in voltage recovery mode is the diffusion of the oxide
ions through SnO2 layer. The increment of mass transport lost, R3, of the cell causes the slowly increase of
the cell’s voltage over the voltage from 0.7-0.8 V at 700, 750, and 800 °C.
IMPEDANCE SPECTROSCOPY ANALYSIS OF A LIQUID TIN ANODE FUEL CELL IN VOLTAGE RE...AEIJ journal
A concept of a liquid tin anode-indirect carbon air fuel cell (LTA-ICFC) are described. Experimental setups for analysis of LTA-ICFC polarisations of an operational electrochemical reactor of the LTA-ICFC are presented. Results from Electrochemical Impedance Spectroscopy (EIS) Analysis of the electrochemical reactor of the LTA-ICFC are shown and analysed.The rate-determining step of the system is concluded. The charge-transfer resistance did not show considerable differences at 700-800 °C. This can be implied
that the charge-transfer resistance is not the rate-limiting step of the transport processes of the fuel cell.The increase of the Warburg impedance concurrently with the resistance to fit mass-transport loss (R3) suggests that the rate-limiting step for the LTA-ICFC in voltage recovery mode is the diffusion of the oxide
ions through SnO2 layer. The increment of mass transport lost, R3, of the cell causes the slowly increase of the cell’s voltage over the voltage from 0.7-0.8 V at 700, 750, and 800 °C.
IMPEDANCE SPECTROSCOPY ANALYSIS OF A LIQUID TIN ANODE FUEL CELL IN VOLTAGE RE...aeijjournal
A concept of a liquid tin anode-indirect carbon air fuel cell (LTA-ICFC) are described. Experimental
setups for analysis of LTA-ICFC polarisations of an operational electrochemical reactor of the LTA-ICFC
are presented. Results from Electrochemical Impedance Spectroscopy (EIS) Analysis of the electrochemical
reactor of the LTA-ICFC are shown and analysed.The rate-determining step of the system is concluded.
The charge-transfer resistance did not show considerable differences at 700-800 °C. This can be implied
that the charge-transfer resistance is not the rate-limiting step of the transport processes of the fuel cell.
The increase of the Warburg impedance concurrently with the resistance to fit mass-transport loss (R3)
suggests that the rate-limiting step for the LTA-ICFC in voltage recovery mode is the diffusion of the oxide
ions through SnO2 layer. The increment of mass transport lost, R3, of the cell causes the slowly increase of
the cell’s voltage over the voltage from 0.7-0.8 V at 700, 750, and 800 °C.
IMPEDANCE SPECTROSCOPY ANALYSIS OF A LIQUID TIN ANODE FUEL CELL IN VOLTAGE RE...AEIJjournal2
This can be implied that the charge-transfer resistance is not the rate-limiting step of the transport processes of the fuel cell. The increase of the Warburg impedance concurrently with the resistance to fit mass-transport loss (R3) suggests that the rate-limiting step for the LTA-ICFC in voltage recovery mode is the diffusion of the oxide ions through SnO2 layer. The increment of mass transport lost, R3, of the cell causes the slowly increase of the cell’s voltage over the voltage from 0.7-0.8 V at 700, 750, and 800 °C.
In this presentation, we discuss ambitious solutions for fighting climate change and present the first results of the Katabata project. The goal of this project was to install weather stations in very windy parts of Greenland, as a first step to harvest wind energy there.
Download a power point version of this presentation with higher quality images at the following address: https://orbi.uliege.be/handle/2268/251827
1. COMPUTER APPLICATION OF
ELECTROSTATIC PRECIPITATOR
PRESENTED BY
VIKAS KUMAR VERMA
M . T E C H 1 ST Y R ( E N . N O - 1 1 5 1 9 0 1 6 )
ENVIRONMENTAL ENGINEERING
SUBMITTED TO
PROF. - U.B. CHITRANSHI
DEPARTMENT OF CIVIL ENGINEERING
INDIAN INSTITUTE OF TECHNOLOGY ROORKEE
11/10/2011
2. What is an Electrostatic Precipitator
A device which separates particles from a gas stream by
passing the carrier
gas between pairs of electrodes across which a
unidirectional, high-voltage
potential is placed. The particles are charged before
passing through the
field and migrate to an oppositely charged electrode.
These devices are
very efficient collectors of small particles, and their use in
removing
particles from power plant plumes and in other industrial
applications is
widespread.
11/10/2011
3. INTRODUCTION
Historically , the practice of collecting and treating waste
water is a relatively recent undertaking
In India there was this inhuman practice of carrying solid
waste by a certain section section of society since time
immemorial which not only had a debilitating effect on their
health but also harmed the social fabric of our country.
The first “modern” sewerage system for waste water collection
was built in Hamburg,Germany,in 1842 by Lindley.
Since then a lot of improvements and innovations have been
applied to make the collection system more efficient and
useful.
11/10/2011
4. A Precipitator is a device that
captures particulates from a gas
stream
11/10/2011
7. Types of ESPs(Dry or Wet Electrostatic Precipitator)
Dry electrostatic precipitator ( ESP ) devices are
employed on hot process exhausts (250 - 850 deg. F)
that operate above the dew point of the gas stream.
Dry electrostatic precipitator devices typically collect dry dust
particles such as wood ash, incinerator ash, or coal ash from
boiler or incinerator applications. Additional dry electrostatic
precipitator applications include carbon anode ovens, cement
kilns, and petroleum cat crackers. Dry electrostatic
precipitator devices are attractive due to their ability to collect
and transport the dust in a dry condition. This eliminates the
use of water and the concerns of pollution, corrosion and
dewatering efforts associated with scrubbers. If the dust
particles can be collected and handled in a dry condition it is
always more advantageous to employ a Dry ESP.
11/10/2011
9. Wet electrostatic precipitator ( ESP )
This is old technology originally designed in the 1920's to collect sulfuric acid
mist using lead collection tubes. Today, ESP devices are employed on gas
streams that include oily and sticky particulates or gas streams that must be
cooled to saturation in order to condense aerosols that were formerly in the gas
phase. Due to the different characteristics of the collected precipitate, the
mechanical removal systems (rappers and vibrators) in Dry electrostatic
precipitator devices are not effective. Consequently, the Wet electrostatic
precipitator uses a water flushing system to remove the particles from the
collecting surface. The gas stream is either saturated before entering the
collection area or the collecting surface is continually wetted to prevent
agglomerations from forming. Some mist aerosols simply gravity flow down the
collecting surfaces. These devices are effective on acid mist, oil and tar based
condensed aerosols or applications where dry dust particles combine with
condensables to form paste like residues. Due to the wet environment of wet
electrostatic precipitator devices, they are typically fabricated out of corrosion
resistant materials such as stainless steel or special alloys.
11/10/2011
18. • Turbulent flow: uniformly mixing
• Perfect Collection
• The fraction of the particles removed in
unit time = the ratio of the area traveled
by drift velocity in unit time to the total
cross-section
Deutsch-Anderson
Equation
dN 2 RVTE dt 2VTE dt
N R2 R
N (t ) 2VTE t
exp( )
N0 R
VTE Ac
1 P 1 exp Ac/Q: Specific Collection Area (SCA)
Q
11/10/2011
19. Charging Mechanism: Diffusion Charging
Random collisions between
ions and particles
The total number of charges on a particle
d p kT d p ci e 2 N i t
n ln 1 (ci ~ 2.4 104 cm/s)
2e 2 2kT
Use esu, not SI units.
The total charges on a particle
q ne
Q: Does q depend on time?
Does q depend on dp?
11/10/2011
21. ELectrical Mobility vs dp
10 Diffusion charging
Field Charging
Combined Charging
Z (stC.s/g)
1
Typical fly ash
size distribution
0.1
0.01 0.1 1 10
dp (um)
Q: If the ESP is used to collect the
fly ash, how will the particle size
distribution at ESP outlet look like?
11/10/2011
22. Resistivity/Conductivity
Impact of particles’ resistivity on ESP’s
performance: is desired
109 - 1010 ohm-cm
Factors: temperature, composition
Flue gas conditioning
Q: How does resistivity affect an ESP’s performance?
11/10/2011
23. Effects of sulfur content and temperature on resistivity
Q: Is S in coal good or bad? 11/10/2011
25. Effective drift velocity as a function of resistivity by measurement
Use the same Deutsch-Anderson Equation with new we.
Q: Estimate the total collection area required for a 95% efficient fly-ash ESP
that treats 8000 m3/min. The ash resistivity is 1.6 1010 ohm-cm.
11/10/2011
27. High Efficiency ESP (>95%)
Q: In designing a high
efficiency ESP, a smaller
drift velocity is to be used.
Why?
Matts-Ohnfeldt Equation
k
AC
1 exp we
Q
Use k = 1 for fly ash
k = 0.5 or 0.6 for
industrial category
Rule of Thumb
• Below 95%, use Deutsch-Anderson Equation
• Above 99%, use Matts-Ohnfeldt Equation
• Between them, use an average
11/10/2011
28. Power Consumption
Corona power
PC ICVavg
Drift velocity
kPC
we
AC
Efficiency vs. Corona Power
Power density ~ 1-2 W/ft2
kPC
1 exp
Q
k = 0.55 for Pc/Q in W/cfs up to 98.5%
11/10/2011
30. Computer Model Structure of ESP
INPUT DATA: Operator experience
METEROLOGY EMISSIONS RECEPTORS
Model does calculations
Model Output: Estimates of Concentrations
at Receptors
11/10/2011
31. Atmospheric
Chemistry
Emissions Numerical Pollutant
Inputs Routines Distributions
Meteorologic
Emissions al Fields Effects
Modeling
Visualization
Meteorologic
Inputs:
Population al Modeling
Economics
Roads Inputs:
Land Use Topography Controls
Industry Observed
Meteorology Meteorology
Solar
insolation
11/10/2011
32. Softwares using To Control Air Pollution By
ESP
ADAM
By US Environmental Protection Agency, Office of Air Quality
Planning and Standards (OAQPS). Air Force Dispersion Assessment
Model (ADAM) is a modified box and Gaussian dispersion model
AERMAP
By USEPA, Office of Air Quality Planning and Standards (OAQPS). A
terrain preprocessor for AERMOD. AERMAP processes commercially
available Digital Elevation Data and creates a file suitable for use
within an AERMOD control file
AERMOD Modeling System
By USEPA, Office of Air Quality Planning and Standards (OAQPS). A
steady-state plume model that incorporates air dispersion based on
planetary boundary layer turbulence structure and scaling
concepts, including treatment of both surface and elevated
sources, and both simple and complex terrain.
11/10/2011
33. AFTOX
By USEPAgency, Office of Air Quality Planning and Standards
(OAQPS). A Gaussian dispersion model that will handle
continuous or instantaneous liquid or gas elevated or surface
releases from point or area sources.
AP-42: Compilation of Air Pollutant Emission Factors (Mobile
Sources)
By USEPAgency of Mobile Sources. "Compilation of Air
Pollutant Emission Factors, Volume II: Mobile Sources"
(commonly referred to as "AP-42") has two sections, I -
Highway Vehicles and II - Nonroad Mobile Sources.
ASPEN
USEPAgency of Air Quality Planning and Standards (OAQPS).
The Assessment System for Population Exposure Nationwide
(ASPEN) consists of a dispersion and a mapping module.
BLP
By US E P Agency, Office of Air Quality Planning and Standards
(OAQPS). A Gaussian plume dispersion model designed to
handle unique modeling problems associated with aluminum
reduction plants, and other industrial sources where plume rise
and downwash effects from stationary line sources are
important.
11/10/2011
34. BlueSky
By US Department of Agriculture, Forest Service. A modeling
framework designed to predict cumulative impacts of smoke
from forest, agricultural, and range fires. The BlueSky smoke
modeling framework combines emissions, meteorology, and
dispersion models to generate predictions of smoke impacts
across the landscape.
CALINE4 (California LINE Source Dispersion Model)
By California Department of Transportation. A modeling
program to assess air quality impacts near transportation
facilities. It is based on the Gaussian diffusion equation and
employs a mixing zone concept to characterize pollutant
dispersion over the roadway
CAMEO
By US Environmental Protection Agency and National Oceanic
and Atmospheric Administration. CAMEO (Computer-Aided
Management of Emergency Operations) is a software suite of
applications that includes: CAMEO, ALOHA, and MARPLOT. It
supports government and industry chemical emergency
management with chemical safety and emergency response
data, digitized mapping, and air dispersion modeling.
11/10/2011
35. DEGADIS
By USEPA, Office of Air Quality Planning and Standards (OAQPS).
Simulates the atmospheric dispersion at ground-level of area source
dense gas (or aerosol) clouds released with zero momentum into the
atmospheric boundary layer over flat, level terrain. The model
describes the dispersion processes which accompany the ensuing
gravity-driven flow and entrainment of the gas into the boundary
layer.
Industrial Waste Air Model (IWAIR)
By USEPA, Office of Solid Waste. Evaluates inhalation risk and
estimates whether specific wastes and management practices may
pose an unacceptable risk to human health.
Internet Geographical Exposure Modeling System (IGEMS)
By USEPA, Office of Pollution Prevention and Toxics (OPPT). IGEMS
is a modernization of OPPT's older GEMS and PCGEMS tools. IGEMS
brings together in one system several EPA environmental fate and
transport models and some of the environmental data needed to run
them. IGEMS includes models and data for ambient air, surface
water, soil, and ground water, and makes the models much easier to
use than their stand-alone counterparts. IGEMS will have graphics
and (GIS) capabilities for displaying environmental modeling results.
11/10/2011
36. OBODM
Intended for use in evaluating the potential air quality impacts
of the open burning and detonation (OB/OD) of obsolete
munitions and solid propellants.
OZIPR
A one-dimensional photochemical box model that is an
alternative version of the OZIP model that deals with air toxic
pollutants.
PLUVUEII
A model used for estimating visual range reduction and
atmospheric discoloration caused by plumes resulting from the
emissions of particles, nitrogen oxides, and sulfur oxides from a
single source. The model predicts the
transport, dispersion, chemical reactions, optical effects and
surface deposition of point or area source emissions.
TSCREEN
Toxics Screening Model (TSCREEN) is a Gaussian model that
implements the procedures to correctly analyze toxic emissions
and their subsequent dispersion from one of many different
types of possible releases for superfund sites. It contains 3
models: SCREEN3, PUFF, and RVD (Relief Valve Discharge).
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37. C Programs of Parallel Plate ESP,Cylindrical ESP
//Design of parallel plate ESP , cylindrical ESP//
#include<stdio.h>
#include<math.h>
#include<conio.h>
#define permi 8.85*pow(10,-12)
#define u 0.000018
void cylin (double vt1);
void main ()
{
int i;
float size ,field, con;
double vt, vt1;
clrscr ();
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38. // Calculation of Drift Velocity //
printf(“Enter the size of the particle in mn”);
scanf(“%f”,&size);
printf(“Enter the field strength in KV/mn”);
scanf(“%f”,&field);
field = field*1000;
con=0.75;
printf(“Permi %e”, permi);
vt=(size*permi*field*con);
vt1=(vt/u);
printf(“nThe drift velocity is %e m/s n”,vt1);
printf(“ESP CALCULATIONn”);
printf(“1. Parallel plate ESPn”);
printf(“2. Cylindrical ESPn”);
printf(“Enter your choicen”);
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40. printf(“Enter the percent efficiency n”);
scanf(“%f”, &eff);
eff=eff/100;
printf(“Enter the length of plate in m n”);
scanf(“%f”, &len);
printf(“Enter the height of plate in m n”);
scanf(“%f” &hgt);
printf(“Enter the spacing of plate in m n”);
scanf(“%f”, &space);
A=(-rate/vt1);
area=len*hgt*space;
number=A/area;
printf(“The number of plates required is %fn”,number);
volume=number*len*space;
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41. printf(“The volume of the ESP in %f cu.mn”,volume);
getch();
}
void cylin(double vt1)
{
float len, dia, eff, A, number, area, rate;
printf(“Enter the present efficiency n”);
scanf(“%f”, &eff);
eff=eff/100;
printf(“Enter the length of plate in m n”);
scanf(“%f”, &len);
printf(“Enter the dia of plate in m n”);
scanf(“%f”, &dia);
A=(-rate/vt1);
area=len*dia*3.14;
number=A/area;
printf(The number of plates required is %fn”, number);
getch ();
}
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42. CONCLUSION
Seeing the emerging pollution along with increasing power demands in
India, Government of India has decided to set up nuclear power plants in
India.Thus, installations of ESPs( Electro-Static-Precipitators) has been made a
compulsion for the manufacturers of power plant boilers and equipments.
ESPs all over India, catering to a variety of customer needs and providing cost
effective solution for oil mist and dry smoke problems on various metalworking
(metal-cutting & metal-forming) and heat treatment processes / applications
An Electrostatic Precipiptator applies separation forces directly to the particles to
be collected. This is much more efficient than trying to apply separation force to
the entire gas stream, as is the case for venturi scrubbers or bag houses. The
substantial savings in operating cost can pay for the equipment in only 2-3 years.
The precipitator can operate at temperatures up to 750 deg. F providing durable
advantages over fabric filters.
In INDIA 99% of the Power Plant using ESPs. So its widely used process for dust
removal having 99.99% efficiency.
Now-a-days we collecting only Dry Fly Ash it used in cement making it maintain
same quality of cement.
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