{"id":127,"date":"2019-03-09T11:03:21","date_gmt":"2019-03-09T11:03:21","guid":{"rendered":"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/?post_type=chapter&#038;p=127"},"modified":"2019-04-22T06:48:34","modified_gmt":"2019-04-22T06:48:34","slug":"9-plume-behaviour","status":"publish","type":"chapter","link":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/chapter\/9-plume-behaviour\/","title":{"rendered":"Plume Behaviour"},"content":{"raw":"<div><span style=\"float: right\"><a href=\"https:\/\/youtu.be\/3Sfqw-naSjY\" target=\"_blank\" rel=\"noopener\"><img src=\"http:\/\/epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/2018\/11\/download.png\" alt=\"epgp books\" width=\"75px\" height=\"75px;\" \/><\/a><\/span><\/div>\r\n1. Aim of the module\r\n2. Introduction\r\n3. Atmospheric stability\r\n3.1. Lapse rate\r\n3.2. Types of stability\r\n4. Plume behaviour\r\n5. Air quality models\r\n5.1 Types of air quality models\r\n5.2 Examples of air quality models\r\n6. The point source Gaussian dispersion model\r\n6.1 Line source dispersion model\r\n6.2 Area source dispersion model\r\n6.3 Advanced Gaussian models\r\n6.4 Advantages and limitations of Gaussian model\r\n6.5 Examples of advanced Gaussian models\r\n7. Conclusions\r\n1. Aim of the module\r\n<ol>\r\n \t<li><strong><em>Aim of the module<\/em><\/strong><\/li>\r\n<\/ol>\r\nThe aim of the present module is:\r\n<ul>\r\n \t<li>To familiarize the reader with the concept of atmospheric stability<\/li>\r\n \t<li>To understand plume behaviour and its types<\/li>\r\n \t<li>To understand point-source Gaussian Dispersion model<\/li>\r\n<\/ul>\r\n<ol start=\"2\">\r\n \t<li><strong><em>Introduction<\/em><\/strong><\/li>\r\n<\/ol>\r\n<p style=\"text-align: justify\">In meteorology, we generally study about the movement of air mass (generally horizontal) from one place to the other. Many times, the particles in the air parcel get transported vertically by a process called turbulent diffusion or eddy diffusion (Daly and Zannetti, 2007). This horizontal and vertical motion of air parcels is responsible for various atmospheric processes such as cloud formation and plume behaviour. In this module, we shall study the concept of atmospheric stability and lapse rate; the types of stability, plume behaviour of pollutants released from stack and air quality models. The model shall, however, be limited to point-source Gaussian dispersion model and its application to linear and area source models.<\/p>\r\n\r\n<ol start=\"3\">\r\n \t<li><strong><em> Atmospheric stability<\/em><\/strong><\/li>\r\n<\/ol>\r\n<p style=\"text-align: justify\">The resistance of the atmosphere to vertical motion is called as atmospheric stability. An air parcel in meteorology refers to an air mass having more or less uniform properties. An air parcel will expand and cool as it rises and will compress and warm as it sinks. The reason behind this primarily is that as the air parcel rises, it encounters lower pressure and vice-versa. If we assume that the process is adiabatic, which implies that no exchange of energy of air parcel occurs with the environment; then as the air parcel rises, it will expand and cool since the internal energy is used up during the process. The term \u2018adiabatic\u2019 is derived from the Greek word \u2018<em>impassable<\/em>\u2019, implying a system which does not lose or gain energy. Reverse process occurs when the air parcel sinks and internal energy is released during sinking which warms up the air parcel.<\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\"><strong><em>3.1 Lapse rates<\/em><\/strong><\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\">Lapse rate refers to the rate of change of temperature or pressure with height. In the atmosphere, this rate of change of temperature with altitude is called as Environmental Lapse Rate (ELR) and corresponds to 6.5\u00b0C km-1. This implies that for every kilometer increase in altitude, temperature drops\u00a0 by 6.5\u00b0C. Actual vertical temperature gradients in the atmosphere are thus highly variable, and can even show an increase in temperature with height, a situation known as a temperature inversion.<\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\">If a dry air parcel is considered instead of environment, a linear relationship exists between temperature and altitude for rising or sinking air parcel, which is known as Dry Adiabatic Lapse Rate (DALR) and is equal to 9.8\u00b0C km-1.<\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\">When condensation or evaporation occurs in the air, however, lapse rates of rising or falling air differ from DALR value due to effect of latent heat. As is obvious, latent heat is released by condensation and consumed by evaporation of water. This leads to change in adiabatic lapse rate since energy released by condensation compensates the rate of cooling of rising air. This modified lapse rate is termed the Saturated Adiabatic Lapse Rate (SALR) or Moist Adiabatic Lapse Rate (MALR). Since the concentration of water vapour in air varies from place to place, SALR is non-linear in nature. The average value of SALR in the troposphere is generally 6\u00b0C km-1.<\/p>\r\n&nbsp;\r\n\r\n<strong><em>3.2 Types of stability<\/em><\/strong>\r\n\r\n&nbsp;\r\n\r\nStability of the atmosphere is affected by:\r\n<ul>\r\n \t<li>Temperature of the surrounding environment<\/li>\r\n \t<li>Temperature of the air parcel<\/li>\r\n<\/ul>\r\nAccordingly, the types of stability are as follows:\r\n<ul>\r\n \t<li><strong>Stable<\/strong>: If the air parcel is displaced vertically, and it returns back to its original position, the atmosphere is said to be stable. It usually occurs when the ELR is less than the Adiabatic Lapse Rate (ALR), a phenomenon occurring generally during temperature inversion. If such a parcel of air is uplifted, it will cool to lower temperatures than its new surroundings along the ALR; thus, becoming denser than the surroundings. Hence the air parcel will tend to fall back to its original level.<\/li>\r\n \t<li><strong>Neutrally stable<\/strong>: If the parcel is displaced vertically, it will acquire a new position and continue to remain in its new position. This generally occurs when ELR is more or less equal to ALR.<\/li>\r\n \t<li><strong>Unstable<\/strong>: If the parcel is displaced vertically, it will accelerate away from its original position in the direction of the initial displacement. Such unstable condition occurs when ELR is greater than ALR.<\/li>\r\n<\/ul>\r\n<strong><em>4. Plume behaviour<\/em><\/strong>\r\n\r\n&nbsp;\r\n<p style=\"text-align: justify\">Plume behaviour refers to the dispersal pattern of gaseous pollutants in atmosphere depending upon wind conditions, atmospheric stability and vertical temperature profile. It shows seasonal as well as diurnal variations. Accordingly, there are various types of plume discussed below and represented diagrammatically in figure 1.<\/p>\r\n<img class=\"aligncenter size-full wp-image-128\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-74.png\" alt=\"\" width=\"483\" height=\"554\" \/>\r\n<ol>\r\n \t<li style=\"text-align: justify\"><strong> Looping plume<\/strong>: It takes place when the atmosphere is very unstable, wind speed is greater than 10 ms-1, has super-adiabatic lapse rate and is accompanied with solar heating. It follows a wave like pattern and provides high degree of mixing at lower levels, sometimes reaching the ground.<\/li>\r\n \t<li style=\"text-align: justify\"><strong> Fumigation<\/strong>: It occurs when plume reaches the ground level along the length of the plume and is caused by a super-adiabatic lapse rate beneath an inversion. The super-adiabatic lapse rate at the ground level occurs due to the solar heating and is quite undesirable since the pollutants remain at ground level. This condition is favoured by clear skies and light winds.<\/li>\r\n \t<li style=\"text-align: justify\"><strong> Coning plume<\/strong>: It results when the vertical air temperature gradient occurs between dry adiabatic and isothermal, the air being slightly unstable with some horizontal and vertical mixing occurring. Coning is most likely to occur during cloudy or windy periods.<\/li>\r\n \t<li style=\"text-align: justify\"><strong> Fanning plume<\/strong>: They spread out horizontally but do not mix vertically. Fanning plumes take place when inversion condition exists in atmosphere, that is, the air temperature increases with altitude. The plume rarely reaches the grounds level unless the inversion is broken by surface heating or a topographical barrier such as a hill. At night, with light winds and clear skies, fanning plumes are quite common.<\/li>\r\n \t<li style=\"text-align: justify\"><strong> Lofting plume<\/strong>: It diffuses upward but not downwards and occurs when there is a super-adiabatic layer above a surface inversion. A lofting plume will generally not reach the ground surface, so there is less pollution at ground level.`<\/li>\r\n \t<li><strong> Trapping: <\/strong>This condition is accompanied by weak lapse below inversion aloft.<\/li>\r\n<\/ol>\r\n<strong><em>5. Air quality models<\/em><\/strong>\r\n\r\n&nbsp;\r\n<p style=\"text-align: justify\">Air quality models use mathematical algorithms to simulate the behaviour of air pollutant as they disperse in the atmosphere and the physical and chemical processes they undergo during dispersion. Usually these models simulate the behaviour of primary pollutants and occasionally the secondary pollutants formed due to chemical reactions of primary pollutants in the atmosphere. Although the inputs for different air quality models vary according to model requirements, certain parameters such as wind speed and direction, temperature and humidity find importance in almost all models. Thus, these models find wide application in agencies involved with management of air quality, site-suitability analysis for establishment of new source as well as predicting future concentration of pollutants.<\/p>\r\n&nbsp;\r\n\r\n<strong><em>5.1 Types of air quality models<\/em><\/strong>\r\n\r\n&nbsp;\r\n\r\nAir quality models can be categorized into four classes.\r\n<ol>\r\n \t<li style=\"text-align: justify\"><strong>Gaussian<\/strong>: Used for estimating the ground-level impact of non-reactive pollutants from stationary sources in a smooth terrain<\/li>\r\n \t<li style=\"text-align: justify\"><strong>Numerical<\/strong>: Used for estimating the impact of reactive and non-reactive pollutants in complex terrain<\/li>\r\n \t<li style=\"text-align: justify\"><strong>Statistical<\/strong>: Employed in situations where physical or chemical processes are not well understoo<\/li>\r\n \t<li style=\"text-align: justify\"><strong>Physical<\/strong>: Involves experimental investigation of source impact in a wind tunnel facility<\/li>\r\n<\/ol>\r\n<strong><em>5.2 Examples of air quality models<\/em><\/strong>\r\n\r\n&nbsp;\r\n\r\nSome examples of air quality models are as follows:\r\n<ol>\r\n \t<li style=\"text-align: justify\"><strong> Dispersion models: <\/strong>These models estimate the concentration of pollutants at specified ground-level receptors in the vicinity of an emissions source. These air quality models are used to determine compliance with National Ambient Air Quality Standards (NAAQS) and other regulatory requirements such as New Source Review (NSR) and Prevention of Significant Deterioration (PSD) regulations.<\/li>\r\n \t<li style=\"text-align: justify\"><strong> Photochemical models: <\/strong>These models estimate pollutant concentrations and deposition of both inert and chemically reactive pollutants such as ozone, particulate matter (PM) and mercury over large spatial scales and are used in regulatory assessments.<\/li>\r\n \t<li style=\"text-align: justify\"><strong> Receptor models: <\/strong>These models use chemical and physical characteristics of gases and particles measured at source and receptor to identify and quantify contribution of atmospheric source to\u00a0\u00a0receptor<\/li>\r\n<\/ol>\r\n<ol start=\"6\">\r\n \t<li><strong><em> The point source Gaussian dispersion model<\/em><\/strong><\/li>\r\n<\/ol>\r\n&nbsp;\r\n<p style=\"text-align: justify\">How do pollutants behave in the atmosphere once they have been emitted? How may we predict their concentrations in the atmosphere? How can we predict the improvement in air quality that must be achieved when new sources are proposed? To help answer these questions, computer models are used. These models use the following inputs:<\/p>\r\n\r\n<ul>\r\n \t<li>\u00fc Predicted emissions<\/li>\r\n \t<li>\u00fc Smokestack heights<\/li>\r\n \t<li>\u00fc Wind data<\/li>\r\n \t<li>\u00fc Atmospheric temperature profiles<\/li>\r\n \t<li>\u00fc Ambient temperatures<\/li>\r\n \t<li>\u00fc Solar insolation<\/li>\r\n \t<li>\u00fc Local terrain features<\/li>\r\n<\/ul>\r\n&nbsp;\r\n<p style=\"text-align: justify\">The point source Gaussian plume model is based on the assumption that the time-averaged pollutant concentration downwind from a source can be modeled using a normal or Gaussian distribution curve. The basic Gaussian dispersion model applies to:<\/p>\r\n\r\n<ul>\r\n \t<li>\u00fc Single point Source: Smokestack<\/li>\r\n \t<li>\u00fc Line Source: Emissions from motor vehicles along a highway<\/li>\r\n \t<li>\u00fc Area Sources: These can be modeled as large number of point sources<\/li>\r\n<\/ul>\r\n&nbsp;\r\n\r\n<img class=\"aligncenter size-full wp-image-129\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-75.png\" alt=\"\" width=\"779\" height=\"476\" \/>\r\n<p style=\"text-align: justify\">Consider a single point source, for example, a smokestack. The coordinate system shows a cross-section of the plume, with \u2018z\u2019 representing vertical direction and \u2018x\u2019 is the distance directly downwind from the source. If we were to observe the plume at any particular instant, it might have some irregular shape, such as the outline of the looping plume shown. A few minutes later, however, the plume might have an entirely different boundary. Thus, time-averaged plume envelope develops over a period of time.<\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\">Since stack emissions have some initial upward velocity and buoyancy, it might be some distance downwind before the plume envelope might begin to look symmetrical about a centerline. The centerline is generally somewhat above the actual stack height. The highest concentration of pollution would be along the centerline, with decreasing concentrations as the distance from this centerline increases. The Gaussian plume model assumes that the pollutant concentration follows a normal distribution about this centerline in both horizontal and vertical directions. It also treats emission as they came from a virtual point source along the plume centerline, at an <em>effective stack height H<\/em>.<\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\">The Gaussian point source dispersion equation relates average, steady state pollutant concentrations to the source strength, wind speed, effective stack height and atmospheric conditions. Its form can be derived from the basic considerations involving gaseous diffusion in three-dimensional space. The following assumptions are incorporated into the analysis:<\/p>\r\n\r\n<ul>\r\n \t<li style=\"text-align: justify\">\u00fc The rate of emissions from the source is constant.<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc The wind speed is constant both in time and with elevation.<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc The pollutant is conservative, i.e., it is not lost by decay, chemical reaction or deposition. On hitting the ground, all is reflected and none is absorbed.<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc The terrain is relatively flat, open country.<\/li>\r\n<\/ul>\r\n<p style=\"text-align: justify\">The three-dimensional coordinate system has the stack at the origin, with distance directly downwind given by x, distance off the downwind axis specified by y, and elevation given by z. Since our concern is people and ecosystems at ground level, the following Gaussian plume equation applies only for z=0.<\/p>\r\n&nbsp;\r\n\r\n<img class=\"aligncenter size-full wp-image-130\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-76.png\" alt=\"\" width=\"800\" height=\"115\" \/>\r\n\r\n&nbsp;\r\n<p style=\"text-align: justify\">Where, C(x,y) = concentration at ground level at the point (x,y), \u00b5g m-3 y= horizontal distance from the plume centerline, m Q= emission rate of pollutants, \u00b5g\/s<\/p>\r\n<p style=\"text-align: justify\">H= effective stack height, m (H=h+\u0394h, where, h= actual stack height, and \u0394h= plume rise)<\/p>\r\n<p style=\"text-align: justify\">uH = average wind speed at the effective height of the stack, ms-1<\/p>\r\n<p style=\"text-align: justify\">\u03c3y = horizontal dispersion coefficient (standard deviation), m \u03c3z = vertical dispersion coefficient (standard deviation), m<\/p>\r\n&nbsp;\r\n\r\nFrom Equation (1), the following points are clear:\r\n\r\n&nbsp;\r\n<ul>\r\n \t<li style=\"text-align: justify\">\u00fc Ground level pollution concentration is directly proportional to the source strength Q, so that the amount of source reduction required to achieve a desired decrease in downwind concentration can be determined.<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc Ground level pollution decreases when taller stacks are used, although relationship is not linear.<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc There is no explicit relationship between emission rate, Q, and downwind distance, x.<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc Downwind concentration appears to be inversely proportional to the wind speed, and is slightly modified by the dependence of plume rise \u0394h on wind speed.<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc The Gaussian plume equation is based on both theory and actual measured data, and its prediction is accurate to \u00b150%. However, it is still very useful due to its universal acceptance, easy to use and allows comparison between estimates made by different modelers in varying situations.<\/li>\r\n<\/ul>\r\n<strong><em>6.2.<\/em><\/strong>\u00a0\u00a0<strong><em>Line source dispersion model<\/em><\/strong>\r\n\r\n&nbsp;\r\n<p style=\"text-align: justify\">In some circumstances, it is appropriate to model sources distributed along a line as if they formed a continuously emitting, infinite line source. Examples of the same include motor vehicles travelling along a straight section of highway, agricultural burning along the edge of a field, or a line of industrial sources on the banks of a river. Under conditions of an infinite-length source at ground level, with winds blowing perpendicular to the line; the ground-level concentration of pollutant at perpendicular distance \u2018x\u2019 from the line source can be described by the following equation:<\/p>\r\n\u00a0\u00a0<img class=\"aligncenter size-full wp-image-617\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-312.png\" alt=\"\" width=\"285\" height=\"48\" \/>\r\n\r\n&nbsp;\r\n\r\nwhere, q = emission rate per unit of distance along the line (gm-1-s-1)\r\n\r\n<img class=\"aligncenter size-full wp-image-131\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-77.png\" alt=\"\" width=\"372\" height=\"223\" \/>\r\n\r\n<strong><em>6.3.<\/em><\/strong>\u00a0<strong><em>Area source dispersion models<\/em><\/strong>\r\n\r\n&nbsp;\r\n<p style=\"text-align: justify\">For distributed sources, various methodologies can be applied to estimate pollutant concentrations. If there are a modest number of point sources, it is reasonable to use the point source Gaussian plume equation for each source to predict its individual contribution. Then, by superposition, find the total concentration at a given location by summing the individual contributions. Another approach could be multiple use of Gaussian line-source equation. By dividing an area into a series of parallel strips and then treating each strip as a line source, the total concentration on any strip can be estimated.<\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\">Another approach involves estimating pollutant concentrations over an area, such as a city, by using the box model concept. Consider the airshed over an urban area to be represented by a rectangular box with base dimensions L and W and height H. The box is oriented such that wind speed \u2018u\u2019 is normal to one side of the box. The height of the box is determined by mixing depth and emissions per unit area will be represented by qs (gm-2s-1).<\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\">Consider the air blowing into the box on the upwind side to have pollutant concentration Cin, and assume that no pollutant is lost from the box along the sides parallel to the wind or from the top. It is assumed that the pollutants are rapidly and completely mixed in the box creating a uniform average concentration C. Also the pollutants are assumed to be conservative in nature, i.e., they do not react, decay or fall out of air stream.<\/p>\r\n&nbsp;\r\n\r\n<img class=\"aligncenter size-full wp-image-132\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-78.png\" alt=\"\" width=\"737\" height=\"448\" \/>\r\n<p style=\"text-align: justify\">Thus, the amount of pollutants in the box is the volume of the box times the concentration, LWHC. The rate at which air is entering and leaving the box is the area of either end times the windspeed, WHu, so the rate at which pollutants is entering the box is WHuCin. The rate at which it leaves the box is WHuC. If we assume the pollutant is conservative, then the mass balance equation for the box may be written as:<\/p>\r\n&nbsp;\r\n<p style=\"text-align: justify\">(Rate of change of pollution in the box) = (Rate of pollution entering the box) - (Rate of pollution leaving the box)<\/p>\r\n&nbsp;\r\n\r\n<img class=\"aligncenter size-full wp-image-133\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-79.png\" alt=\"\" width=\"565\" height=\"249\" \/>\r\n\r\nL= length of airshed, m\r\n\r\nW= width of airshed, m\r\n\r\nu= average windspeed against one edge of the box, m s-1\r\n\r\nThe steady state solution to equation (3) can be obtained by setting dC\/dt = 0, so that\r\n\r\n&nbsp;\r\n\r\n<img class=\"aligncenter size-full wp-image-134\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-80.png\" alt=\"\" width=\"835\" height=\"361\" \/>\r\n<p style=\"text-align: justify\">When t = L\/u, the exponential function becomes e-1 and the concentration reaches about 63% of its final value. This is called time constant, the ventilation time, the residence time, or the e-folding time.<\/p>\r\n&nbsp;\r\n\r\n<strong><em>6.4.<\/em><\/strong>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <strong><em>Advantages and limitations of Gaussian model<\/em><\/strong>\r\n\r\n&nbsp;\r\n\r\n&nbsp;\r\n\r\n<strong>Advantages:<\/strong>\r\n<ul>\r\n \t<li style=\"text-align: justify\">\u00fc Fast response time<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc Easy to calculate<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc Can be applied to real-time GIS-based decision support software<\/li>\r\n \t<li style=\"text-align: justify\">\u00fc Can be successfully used for a wide range of studies of air quality in urban and industrial areas<\/li>\r\n<\/ul>\r\n<strong>Limitations:<\/strong>\r\n<ul>\r\n \t<li>\u00fc Does not incorporate meteorological parameters<\/li>\r\n \t<li>\u00fc Unsatisfactory performance in industrial incidents such as Bhopal and Chernobyl disaster<\/li>\r\n<\/ul>\r\n<strong><em>6.5.<\/em><\/strong>\u00a0\u00a0<strong><em>Examples of advanced Gaussian models<\/em><\/strong>\r\n<ol>\r\n \t<li style=\"text-align: justify\">AERMOD: It is an open-source Gaussian air dispersion model developed by the <em>US Environmental<\/em> <em>Protection Agency <\/em>(EPA) to carry out impact studies of planned or existing industrial sites. It has built-in models to handle complex terrain and urban boundary layer. Besides, although AERMOD uses the steady-state approximation for the flow and the source, it can be used within 10\u2013100 km distance using its meteorological pre-processor, AERMET.<\/li>\r\n \t<li style=\"text-align: justify\"><em>Complex Terrain Dispersion Model <\/em>(CTDM) - This has also been developed by EPA to estimate concentration patterns in mountain regions.<\/li>\r\n \t<li style=\"text-align: justify\">ADMS: The ADMS (Atmospheric Dispersion Modeling System) model has been developed in Europe for air quality simulations. It incorporates meteorological effects like coastal circulations, complex terrain, deposition processes and radioactive decay.<\/li>\r\n \t<li style=\"text-align: justify\">CERC: UK Met Office <em>and<\/em> Cambridge Environmental Research Consultants (CERC) also developed the ADMS-Urban module that aims to provide air quality forecasts for cities.<\/li>\r\n \t<li style=\"text-align: justify\">Other Gaussian models: There are several other Gaussian models used for impact and health risk studies such as CALINE3 (for highway air pollution), OCD for coastal areas, BLP and ISC for industrial sites or ALOHA for accidental and heavy gas releases. They are widely used by authorities, environmental protection organizations and industry investigations.<\/li>\r\n<\/ol>\r\n&nbsp;\r\n\r\n<strong><em>7. Conclusions<\/em><\/strong>\r\n\r\n&nbsp;\r\n<p style=\"text-align: justify\">At the end of this module, the reader shall be able to understand the types of atmospheric stability, how it affects the plume behaviour, types and examples of air quality models with special reference to point-source Gaussian dispersion model. These models find wide application in management of air quality as well as predicting future scenarios of air quality. This is relevant due to rising air pollution levels all over the globe and provides a fast, simplistic and cost-effective solution at local level, especially at sites where air quality monitoring is difficult due to experimental difficulties.<\/p>\r\n&nbsp;\r\n<table>\r\n<tbody>\r\n<tr>\r\n<td><span style=\"font-size: 16px\">you can view video on Plume Behaviour<\/span><\/td>\r\n<td><a style=\"font-size: 16px\" href=\"https:\/\/youtu.be\/3Sfqw-naSjY\" target=\"_blank\" rel=\"noopener\"><span style=\"color: #333333\"><img class=\"alignnone wp-image-120\" src=\"http:\/\/epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/2018\/11\/download.png\" alt=\"\" width=\"36\" height=\"36\" \/><\/span><\/a><\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<strong>References<\/strong>\r\n\r\n&nbsp;\r\n<ul>\r\n \t<li style=\"text-align: justify\">Daly, A. and P. Zannetti. 2007. Air Pollution Modeling \u2013 An Overview. Chapter 2 of AMBIENT AIR POLLUTION (P. Zannetti, D. Al-Ajmi, and S. Al-Rashied, Editors). Published by The Arab School for Science and Technology (ASST) (http:\/\/www.arabschool.org.sy) and The EnviroComp Institute (<a href=\"http:\/\/www.envirocomp.org\/\">http:\/\/www.envirocomp.org\/<\/a>).<\/li>\r\n \t<li style=\"text-align: justify\">Gilbert M. Masters &amp; Wendell P. Ela (2003). Introduction to Environmental Engineering. Prentice Hall.Venugopala Rao (2002). Textbook of Environmental Engineering. PHI Learning Pvt. Ltd., pp. 184<\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/modeling-applications-and-tools<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/photochemical-modeling-applications<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/photochemical-modeling-tools<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/dispersion-modeling-applications<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/dispersion-modeling-applications<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/multipollutant-modeling-applications<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/air-quality-models<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/meteorological-data-and-processors<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><em>https:\/\/www3.epa.gov\/scram001\/dispersionindex.htm<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><a href=\"http:\/\/elte.prompt.hu\/sites\/default\/files\/tananyagok\/AtmosphericChemistry\/ch10s03.html\"><em>http:\/\/elte.prompt.hu\/sites\/default\/files\/tananyagok\/AtmosphericChemistry\/ch10s03.html<\/em><\/a><\/li>\r\n \t<li style=\"text-align: justify\"><a href=\"http:\/\/people.math.sfu.ca\/~stockie\/atmos\/paper.pdf\"><em>http:\/\/people.math.sfu.ca\/~stockie\/atmos\/paper.pdf<\/em><\/a><\/li>\r\n \t<li style=\"text-align: justify\"><a href=\"https:\/\/www.ready.noaa.gov\/READY_gaussian.php\"><em>https:\/\/www.ready.noaa.gov\/READY_gaussian.php<\/em><\/a><\/li>\r\n \t<li style=\"text-align: justify\"><em>http:\/\/www.rrcap.ait.asia\/male\/Documents\/manual\/national\/04Chapter4.pdf<\/em><\/li>\r\n \t<li style=\"text-align: justify\"><a href=\"http:\/\/nptel.ac.in\/courses\/Webcourse-contents\/IIT-Delhi\/Environmental%20Air%20Pollution\/air%20pollution%20(Civil)\/Module-4\/1.htm\"><em>http:\/\/nptel.ac.in\/courses\/Webcourse-contents\/IIT-<\/em><\/a><a href=\"http:\/\/nptel.ac.in\/courses\/Webcourse-contents\/IIT-Delhi\/Environmental%20Air%20Pollution\/air%20pollution%20(Civil)\/Module-4\/1.htm\"><em>Delhi\/Environmental%20Air%20Pollution\/air%20pollution%20(Civil)\/Module-4\/1.htm<\/em><\/a><\/li>\r\n \t<li style=\"text-align: justify\"><a href=\"http:\/\/site.iugaza.edu.ps\/afoul\/files\/2010\/02\/chapter_7.pdf\"><em>http:\/\/site.iugaza.edu.ps\/afoul\/files\/2010\/02\/chapter_7.pdf<\/em><\/a><\/li>\r\n \t<li style=\"text-align: justify\"><a href=\"http:\/\/elte.prompt.hu\/sites\/default\/files\/tananyagok\/AtmosphericChemistry\/ch10s03.html\"><em>http:\/\/elte.prompt.hu\/sites\/default\/files\/tananyagok\/AtmosphericChemistry\/ch10s03.html<\/em><\/a><\/li>\r\n \t<li style=\"text-align: justify\"><a href=\"http:\/\/atoc.colorado.edu\/~saraht\/atoc1050\/Lecture_Notes\/chapter6-notes.pdf\"><em>http:\/\/atoc.colorado.edu\/~saraht\/atoc1050\/Lecture_Notes\/chapter6-notes.pdf<\/em><\/a><\/li>\r\n<\/ul>","rendered":"<div><span style=\"float: right\"><a href=\"https:\/\/youtu.be\/3Sfqw-naSjY\" target=\"_blank\" rel=\"noopener\"><img decoding=\"async\" src=\"http:\/\/epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/2018\/11\/download.png\" alt=\"epgp books\" width=\"75px\" height=\"75px;\" \/><\/a><\/span><\/div>\n<p>1. Aim of the module<br \/>\n2. Introduction<br \/>\n3. Atmospheric stability<br \/>\n3.1. Lapse rate<br \/>\n3.2. Types of stability<br \/>\n4. Plume behaviour<br \/>\n5. Air quality models<br \/>\n5.1 Types of air quality models<br \/>\n5.2 Examples of air quality models<br \/>\n6. The point source Gaussian dispersion model<br \/>\n6.1 Line source dispersion model<br \/>\n6.2 Area source dispersion model<br \/>\n6.3 Advanced Gaussian models<br \/>\n6.4 Advantages and limitations of Gaussian model<br \/>\n6.5 Examples of advanced Gaussian models<br \/>\n7. Conclusions<br \/>\n1. Aim of the module<\/p>\n<ol>\n<li><strong><em>Aim of the module<\/em><\/strong><\/li>\n<\/ol>\n<p>The aim of the present module is:<\/p>\n<ul>\n<li>To familiarize the reader with the concept of atmospheric stability<\/li>\n<li>To understand plume behaviour and its types<\/li>\n<li>To understand point-source Gaussian Dispersion model<\/li>\n<\/ul>\n<ol start=\"2\">\n<li><strong><em>Introduction<\/em><\/strong><\/li>\n<\/ol>\n<p style=\"text-align: justify\">In meteorology, we generally study about the movement of air mass (generally horizontal) from one place to the other. Many times, the particles in the air parcel get transported vertically by a process called turbulent diffusion or eddy diffusion (Daly and Zannetti, 2007). This horizontal and vertical motion of air parcels is responsible for various atmospheric processes such as cloud formation and plume behaviour. In this module, we shall study the concept of atmospheric stability and lapse rate; the types of stability, plume behaviour of pollutants released from stack and air quality models. The model shall, however, be limited to point-source Gaussian dispersion model and its application to linear and area source models.<\/p>\n<ol start=\"3\">\n<li><strong><em> Atmospheric stability<\/em><\/strong><\/li>\n<\/ol>\n<p style=\"text-align: justify\">The resistance of the atmosphere to vertical motion is called as atmospheric stability. An air parcel in meteorology refers to an air mass having more or less uniform properties. An air parcel will expand and cool as it rises and will compress and warm as it sinks. The reason behind this primarily is that as the air parcel rises, it encounters lower pressure and vice-versa. If we assume that the process is adiabatic, which implies that no exchange of energy of air parcel occurs with the environment; then as the air parcel rises, it will expand and cool since the internal energy is used up during the process. The term \u2018adiabatic\u2019 is derived from the Greek word \u2018<em>impassable<\/em>\u2019, implying a system which does not lose or gain energy. Reverse process occurs when the air parcel sinks and internal energy is released during sinking which warms up the air parcel.<\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\"><strong><em>3.1 Lapse rates<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">Lapse rate refers to the rate of change of temperature or pressure with height. In the atmosphere, this rate of change of temperature with altitude is called as Environmental Lapse Rate (ELR) and corresponds to 6.5\u00b0C km-1. This implies that for every kilometer increase in altitude, temperature drops\u00a0 by 6.5\u00b0C. Actual vertical temperature gradients in the atmosphere are thus highly variable, and can even show an increase in temperature with height, a situation known as a temperature inversion.<\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">If a dry air parcel is considered instead of environment, a linear relationship exists between temperature and altitude for rising or sinking air parcel, which is known as Dry Adiabatic Lapse Rate (DALR) and is equal to 9.8\u00b0C km-1.<\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">When condensation or evaporation occurs in the air, however, lapse rates of rising or falling air differ from DALR value due to effect of latent heat. As is obvious, latent heat is released by condensation and consumed by evaporation of water. This leads to change in adiabatic lapse rate since energy released by condensation compensates the rate of cooling of rising air. This modified lapse rate is termed the Saturated Adiabatic Lapse Rate (SALR) or Moist Adiabatic Lapse Rate (MALR). Since the concentration of water vapour in air varies from place to place, SALR is non-linear in nature. The average value of SALR in the troposphere is generally 6\u00b0C km-1.<\/p>\n<p>&nbsp;<\/p>\n<p><strong><em>3.2 Types of stability<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p>Stability of the atmosphere is affected by:<\/p>\n<ul>\n<li>Temperature of the surrounding environment<\/li>\n<li>Temperature of the air parcel<\/li>\n<\/ul>\n<p>Accordingly, the types of stability are as follows:<\/p>\n<ul>\n<li><strong>Stable<\/strong>: If the air parcel is displaced vertically, and it returns back to its original position, the atmosphere is said to be stable. It usually occurs when the ELR is less than the Adiabatic Lapse Rate (ALR), a phenomenon occurring generally during temperature inversion. If such a parcel of air is uplifted, it will cool to lower temperatures than its new surroundings along the ALR; thus, becoming denser than the surroundings. Hence the air parcel will tend to fall back to its original level.<\/li>\n<li><strong>Neutrally stable<\/strong>: If the parcel is displaced vertically, it will acquire a new position and continue to remain in its new position. This generally occurs when ELR is more or less equal to ALR.<\/li>\n<li><strong>Unstable<\/strong>: If the parcel is displaced vertically, it will accelerate away from its original position in the direction of the initial displacement. Such unstable condition occurs when ELR is greater than ALR.<\/li>\n<\/ul>\n<p><strong><em>4. Plume behaviour<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">Plume behaviour refers to the dispersal pattern of gaseous pollutants in atmosphere depending upon wind conditions, atmospheric stability and vertical temperature profile. It shows seasonal as well as diurnal variations. Accordingly, there are various types of plume discussed below and represented diagrammatically in figure 1.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-128\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-74.png\" alt=\"\" width=\"483\" height=\"554\" srcset=\"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-74.png 483w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-74-262x300.png 262w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-74-65x75.png 65w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-74-225x258.png 225w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-74-350x401.png 350w\" sizes=\"auto, (max-width: 483px) 100vw, 483px\" \/><\/p>\n<ol>\n<li style=\"text-align: justify\"><strong> Looping plume<\/strong>: It takes place when the atmosphere is very unstable, wind speed is greater than 10 ms-1, has super-adiabatic lapse rate and is accompanied with solar heating. It follows a wave like pattern and provides high degree of mixing at lower levels, sometimes reaching the ground.<\/li>\n<li style=\"text-align: justify\"><strong> Fumigation<\/strong>: It occurs when plume reaches the ground level along the length of the plume and is caused by a super-adiabatic lapse rate beneath an inversion. The super-adiabatic lapse rate at the ground level occurs due to the solar heating and is quite undesirable since the pollutants remain at ground level. This condition is favoured by clear skies and light winds.<\/li>\n<li style=\"text-align: justify\"><strong> Coning plume<\/strong>: It results when the vertical air temperature gradient occurs between dry adiabatic and isothermal, the air being slightly unstable with some horizontal and vertical mixing occurring. Coning is most likely to occur during cloudy or windy periods.<\/li>\n<li style=\"text-align: justify\"><strong> Fanning plume<\/strong>: They spread out horizontally but do not mix vertically. Fanning plumes take place when inversion condition exists in atmosphere, that is, the air temperature increases with altitude. The plume rarely reaches the grounds level unless the inversion is broken by surface heating or a topographical barrier such as a hill. At night, with light winds and clear skies, fanning plumes are quite common.<\/li>\n<li style=\"text-align: justify\"><strong> Lofting plume<\/strong>: It diffuses upward but not downwards and occurs when there is a super-adiabatic layer above a surface inversion. A lofting plume will generally not reach the ground surface, so there is less pollution at ground level.`<\/li>\n<li><strong> Trapping: <\/strong>This condition is accompanied by weak lapse below inversion aloft.<\/li>\n<\/ol>\n<p><strong><em>5. Air quality models<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">Air quality models use mathematical algorithms to simulate the behaviour of air pollutant as they disperse in the atmosphere and the physical and chemical processes they undergo during dispersion. Usually these models simulate the behaviour of primary pollutants and occasionally the secondary pollutants formed due to chemical reactions of primary pollutants in the atmosphere. Although the inputs for different air quality models vary according to model requirements, certain parameters such as wind speed and direction, temperature and humidity find importance in almost all models. Thus, these models find wide application in agencies involved with management of air quality, site-suitability analysis for establishment of new source as well as predicting future concentration of pollutants.<\/p>\n<p>&nbsp;<\/p>\n<p><strong><em>5.1 Types of air quality models<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p>Air quality models can be categorized into four classes.<\/p>\n<ol>\n<li style=\"text-align: justify\"><strong>Gaussian<\/strong>: Used for estimating the ground-level impact of non-reactive pollutants from stationary sources in a smooth terrain<\/li>\n<li style=\"text-align: justify\"><strong>Numerical<\/strong>: Used for estimating the impact of reactive and non-reactive pollutants in complex terrain<\/li>\n<li style=\"text-align: justify\"><strong>Statistical<\/strong>: Employed in situations where physical or chemical processes are not well understoo<\/li>\n<li style=\"text-align: justify\"><strong>Physical<\/strong>: Involves experimental investigation of source impact in a wind tunnel facility<\/li>\n<\/ol>\n<p><strong><em>5.2 Examples of air quality models<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p>Some examples of air quality models are as follows:<\/p>\n<ol>\n<li style=\"text-align: justify\"><strong> Dispersion models: <\/strong>These models estimate the concentration of pollutants at specified ground-level receptors in the vicinity of an emissions source. These air quality models are used to determine compliance with National Ambient Air Quality Standards (NAAQS) and other regulatory requirements such as New Source Review (NSR) and Prevention of Significant Deterioration (PSD) regulations.<\/li>\n<li style=\"text-align: justify\"><strong> Photochemical models: <\/strong>These models estimate pollutant concentrations and deposition of both inert and chemically reactive pollutants such as ozone, particulate matter (PM) and mercury over large spatial scales and are used in regulatory assessments.<\/li>\n<li style=\"text-align: justify\"><strong> Receptor models: <\/strong>These models use chemical and physical characteristics of gases and particles measured at source and receptor to identify and quantify contribution of atmospheric source to\u00a0\u00a0receptor<\/li>\n<\/ol>\n<ol start=\"6\">\n<li><strong><em> The point source Gaussian dispersion model<\/em><\/strong><\/li>\n<\/ol>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">How do pollutants behave in the atmosphere once they have been emitted? How may we predict their concentrations in the atmosphere? How can we predict the improvement in air quality that must be achieved when new sources are proposed? To help answer these questions, computer models are used. These models use the following inputs:<\/p>\n<ul>\n<li>\u00fc Predicted emissions<\/li>\n<li>\u00fc Smokestack heights<\/li>\n<li>\u00fc Wind data<\/li>\n<li>\u00fc Atmospheric temperature profiles<\/li>\n<li>\u00fc Ambient temperatures<\/li>\n<li>\u00fc Solar insolation<\/li>\n<li>\u00fc Local terrain features<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">The point source Gaussian plume model is based on the assumption that the time-averaged pollutant concentration downwind from a source can be modeled using a normal or Gaussian distribution curve. The basic Gaussian dispersion model applies to:<\/p>\n<ul>\n<li>\u00fc Single point Source: Smokestack<\/li>\n<li>\u00fc Line Source: Emissions from motor vehicles along a highway<\/li>\n<li>\u00fc Area Sources: These can be modeled as large number of point sources<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-129\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-75.png\" alt=\"\" width=\"779\" height=\"476\" srcset=\"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-75.png 779w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-75-300x183.png 300w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-75-768x469.png 768w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-75-65x40.png 65w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-75-225x137.png 225w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-75-350x214.png 350w\" sizes=\"auto, (max-width: 779px) 100vw, 779px\" \/><\/p>\n<p style=\"text-align: justify\">Consider a single point source, for example, a smokestack. The coordinate system shows a cross-section of the plume, with \u2018z\u2019 representing vertical direction and \u2018x\u2019 is the distance directly downwind from the source. If we were to observe the plume at any particular instant, it might have some irregular shape, such as the outline of the looping plume shown. A few minutes later, however, the plume might have an entirely different boundary. Thus, time-averaged plume envelope develops over a period of time.<\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">Since stack emissions have some initial upward velocity and buoyancy, it might be some distance downwind before the plume envelope might begin to look symmetrical about a centerline. The centerline is generally somewhat above the actual stack height. The highest concentration of pollution would be along the centerline, with decreasing concentrations as the distance from this centerline increases. The Gaussian plume model assumes that the pollutant concentration follows a normal distribution about this centerline in both horizontal and vertical directions. It also treats emission as they came from a virtual point source along the plume centerline, at an <em>effective stack height H<\/em>.<\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">The Gaussian point source dispersion equation relates average, steady state pollutant concentrations to the source strength, wind speed, effective stack height and atmospheric conditions. Its form can be derived from the basic considerations involving gaseous diffusion in three-dimensional space. The following assumptions are incorporated into the analysis:<\/p>\n<ul>\n<li style=\"text-align: justify\">\u00fc The rate of emissions from the source is constant.<\/li>\n<li style=\"text-align: justify\">\u00fc The wind speed is constant both in time and with elevation.<\/li>\n<li style=\"text-align: justify\">\u00fc The pollutant is conservative, i.e., it is not lost by decay, chemical reaction or deposition. On hitting the ground, all is reflected and none is absorbed.<\/li>\n<li style=\"text-align: justify\">\u00fc The terrain is relatively flat, open country.<\/li>\n<\/ul>\n<p style=\"text-align: justify\">The three-dimensional coordinate system has the stack at the origin, with distance directly downwind given by x, distance off the downwind axis specified by y, and elevation given by z. Since our concern is people and ecosystems at ground level, the following Gaussian plume equation applies only for z=0.<\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-130\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-76.png\" alt=\"\" width=\"800\" height=\"115\" srcset=\"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-76.png 800w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-76-300x43.png 300w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-76-768x110.png 768w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-76-65x9.png 65w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-76-225x32.png 225w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-76-350x50.png 350w\" sizes=\"auto, (max-width: 800px) 100vw, 800px\" \/><\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">Where, C(x,y) = concentration at ground level at the point (x,y), \u00b5g m-3 y= horizontal distance from the plume centerline, m Q= emission rate of pollutants, \u00b5g\/s<\/p>\n<p style=\"text-align: justify\">H= effective stack height, m (H=h+\u0394h, where, h= actual stack height, and \u0394h= plume rise)<\/p>\n<p style=\"text-align: justify\">uH = average wind speed at the effective height of the stack, ms-1<\/p>\n<p style=\"text-align: justify\">\u03c3y = horizontal dispersion coefficient (standard deviation), m \u03c3z = vertical dispersion coefficient (standard deviation), m<\/p>\n<p>&nbsp;<\/p>\n<p>From Equation (1), the following points are clear:<\/p>\n<p>&nbsp;<\/p>\n<ul>\n<li style=\"text-align: justify\">\u00fc Ground level pollution concentration is directly proportional to the source strength Q, so that the amount of source reduction required to achieve a desired decrease in downwind concentration can be determined.<\/li>\n<li style=\"text-align: justify\">\u00fc Ground level pollution decreases when taller stacks are used, although relationship is not linear.<\/li>\n<li style=\"text-align: justify\">\u00fc There is no explicit relationship between emission rate, Q, and downwind distance, x.<\/li>\n<li style=\"text-align: justify\">\u00fc Downwind concentration appears to be inversely proportional to the wind speed, and is slightly modified by the dependence of plume rise \u0394h on wind speed.<\/li>\n<li style=\"text-align: justify\">\u00fc The Gaussian plume equation is based on both theory and actual measured data, and its prediction is accurate to \u00b150%. However, it is still very useful due to its universal acceptance, easy to use and allows comparison between estimates made by different modelers in varying situations.<\/li>\n<\/ul>\n<p><strong><em>6.2.<\/em><\/strong>\u00a0\u00a0<strong><em>Line source dispersion model<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">In some circumstances, it is appropriate to model sources distributed along a line as if they formed a continuously emitting, infinite line source. Examples of the same include motor vehicles travelling along a straight section of highway, agricultural burning along the edge of a field, or a line of industrial sources on the banks of a river. Under conditions of an infinite-length source at ground level, with winds blowing perpendicular to the line; the ground-level concentration of pollutant at perpendicular distance \u2018x\u2019 from the line source can be described by the following equation:<\/p>\n<p>\u00a0\u00a0<img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-617\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-312.png\" alt=\"\" width=\"285\" height=\"48\" srcset=\"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-312.png 285w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-312-65x11.png 65w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-312-225x38.png 225w\" sizes=\"auto, (max-width: 285px) 100vw, 285px\" \/><\/p>\n<p>&nbsp;<\/p>\n<p>where, q = emission rate per unit of distance along the line (gm-1-s-1)<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-131\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-77.png\" alt=\"\" width=\"372\" height=\"223\" srcset=\"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-77.png 372w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-77-300x180.png 300w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-77-65x39.png 65w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-77-225x135.png 225w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-77-350x210.png 350w\" sizes=\"auto, (max-width: 372px) 100vw, 372px\" \/><\/p>\n<p><strong><em>6.3.<\/em><\/strong>\u00a0<strong><em>Area source dispersion models<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">For distributed sources, various methodologies can be applied to estimate pollutant concentrations. If there are a modest number of point sources, it is reasonable to use the point source Gaussian plume equation for each source to predict its individual contribution. Then, by superposition, find the total concentration at a given location by summing the individual contributions. Another approach could be multiple use of Gaussian line-source equation. By dividing an area into a series of parallel strips and then treating each strip as a line source, the total concentration on any strip can be estimated.<\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">Another approach involves estimating pollutant concentrations over an area, such as a city, by using the box model concept. Consider the airshed over an urban area to be represented by a rectangular box with base dimensions L and W and height H. The box is oriented such that wind speed \u2018u\u2019 is normal to one side of the box. The height of the box is determined by mixing depth and emissions per unit area will be represented by qs (gm-2s-1).<\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">Consider the air blowing into the box on the upwind side to have pollutant concentration Cin, and assume that no pollutant is lost from the box along the sides parallel to the wind or from the top. It is assumed that the pollutants are rapidly and completely mixed in the box creating a uniform average concentration C. Also the pollutants are assumed to be conservative in nature, i.e., they do not react, decay or fall out of air stream.<\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-132\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-78.png\" alt=\"\" width=\"737\" height=\"448\" srcset=\"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-78.png 737w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-78-300x182.png 300w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-78-65x40.png 65w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-78-225x137.png 225w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-78-350x213.png 350w\" sizes=\"auto, (max-width: 737px) 100vw, 737px\" \/><\/p>\n<p style=\"text-align: justify\">Thus, the amount of pollutants in the box is the volume of the box times the concentration, LWHC. The rate at which air is entering and leaving the box is the area of either end times the windspeed, WHu, so the rate at which pollutants is entering the box is WHuCin. The rate at which it leaves the box is WHuC. If we assume the pollutant is conservative, then the mass balance equation for the box may be written as:<\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">(Rate of change of pollution in the box) = (Rate of pollution entering the box) &#8211; (Rate of pollution leaving the box)<\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-133\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-79.png\" alt=\"\" width=\"565\" height=\"249\" srcset=\"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-79.png 565w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-79-300x132.png 300w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-79-65x29.png 65w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-79-225x99.png 225w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-79-350x154.png 350w\" sizes=\"auto, (max-width: 565px) 100vw, 565px\" \/><\/p>\n<p>L= length of airshed, m<\/p>\n<p>W= width of airshed, m<\/p>\n<p>u= average windspeed against one edge of the box, m s-1<\/p>\n<p>The steady state solution to equation (3) can be obtained by setting dC\/dt = 0, so that<\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-134\" src=\"http:\/\/esp08.epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-80.png\" alt=\"\" width=\"835\" height=\"361\" srcset=\"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-80.png 835w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-80-300x130.png 300w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-80-768x332.png 768w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-80-65x28.png 65w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-80-225x97.png 225w, https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-content\/uploads\/sites\/172\/2019\/03\/Untitled-80-350x151.png 350w\" sizes=\"auto, (max-width: 835px) 100vw, 835px\" \/><\/p>\n<p style=\"text-align: justify\">When t = L\/u, the exponential function becomes e-1 and the concentration reaches about 63% of its final value. This is called time constant, the ventilation time, the residence time, or the e-folding time.<\/p>\n<p>&nbsp;<\/p>\n<p><strong><em>6.4.<\/em><\/strong>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <strong><em>Advantages and limitations of Gaussian model<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><strong>Advantages:<\/strong><\/p>\n<ul>\n<li style=\"text-align: justify\">\u00fc Fast response time<\/li>\n<li style=\"text-align: justify\">\u00fc Easy to calculate<\/li>\n<li style=\"text-align: justify\">\u00fc Can be applied to real-time GIS-based decision support software<\/li>\n<li style=\"text-align: justify\">\u00fc Can be successfully used for a wide range of studies of air quality in urban and industrial areas<\/li>\n<\/ul>\n<p><strong>Limitations:<\/strong><\/p>\n<ul>\n<li>\u00fc Does not incorporate meteorological parameters<\/li>\n<li>\u00fc Unsatisfactory performance in industrial incidents such as Bhopal and Chernobyl disaster<\/li>\n<\/ul>\n<p><strong><em>6.5.<\/em><\/strong>\u00a0\u00a0<strong><em>Examples of advanced Gaussian models<\/em><\/strong><\/p>\n<ol>\n<li style=\"text-align: justify\">AERMOD: It is an open-source Gaussian air dispersion model developed by the <em>US Environmental<\/em> <em>Protection Agency <\/em>(EPA) to carry out impact studies of planned or existing industrial sites. It has built-in models to handle complex terrain and urban boundary layer. Besides, although AERMOD uses the steady-state approximation for the flow and the source, it can be used within 10\u2013100 km distance using its meteorological pre-processor, AERMET.<\/li>\n<li style=\"text-align: justify\"><em>Complex Terrain Dispersion Model <\/em>(CTDM) &#8211; This has also been developed by EPA to estimate concentration patterns in mountain regions.<\/li>\n<li style=\"text-align: justify\">ADMS: The ADMS (Atmospheric Dispersion Modeling System) model has been developed in Europe for air quality simulations. It incorporates meteorological effects like coastal circulations, complex terrain, deposition processes and radioactive decay.<\/li>\n<li style=\"text-align: justify\">CERC: UK Met Office <em>and<\/em> Cambridge Environmental Research Consultants (CERC) also developed the ADMS-Urban module that aims to provide air quality forecasts for cities.<\/li>\n<li style=\"text-align: justify\">Other Gaussian models: There are several other Gaussian models used for impact and health risk studies such as CALINE3 (for highway air pollution), OCD for coastal areas, BLP and ISC for industrial sites or ALOHA for accidental and heavy gas releases. They are widely used by authorities, environmental protection organizations and industry investigations.<\/li>\n<\/ol>\n<p>&nbsp;<\/p>\n<p><strong><em>7. Conclusions<\/em><\/strong><\/p>\n<p>&nbsp;<\/p>\n<p style=\"text-align: justify\">At the end of this module, the reader shall be able to understand the types of atmospheric stability, how it affects the plume behaviour, types and examples of air quality models with special reference to point-source Gaussian dispersion model. These models find wide application in management of air quality as well as predicting future scenarios of air quality. This is relevant due to rising air pollution levels all over the globe and provides a fast, simplistic and cost-effective solution at local level, especially at sites where air quality monitoring is difficult due to experimental difficulties.<\/p>\n<p>&nbsp;<\/p>\n<table>\n<tbody>\n<tr>\n<td><span style=\"font-size: 16px\">you can view video on Plume Behaviour<\/span><\/td>\n<td><a style=\"font-size: 16px\" href=\"https:\/\/youtu.be\/3Sfqw-naSjY\" target=\"_blank\" rel=\"noopener\"><span style=\"color: #333333\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-120\" src=\"http:\/\/epgpbooks.inflibnet.ac.in\/wp-content\/uploads\/2018\/11\/download.png\" alt=\"\" width=\"36\" height=\"36\" \/><\/span><\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><strong>References<\/strong><\/p>\n<p>&nbsp;<\/p>\n<ul>\n<li style=\"text-align: justify\">Daly, A. and P. Zannetti. 2007. Air Pollution Modeling \u2013 An Overview. Chapter 2 of AMBIENT AIR POLLUTION (P. Zannetti, D. Al-Ajmi, and S. Al-Rashied, Editors). Published by The Arab School for Science and Technology (ASST) (http:\/\/www.arabschool.org.sy) and The EnviroComp Institute (<a href=\"http:\/\/www.envirocomp.org\/\">http:\/\/www.envirocomp.org\/<\/a>).<\/li>\n<li style=\"text-align: justify\">Gilbert M. Masters &amp; Wendell P. Ela (2003). Introduction to Environmental Engineering. Prentice Hall.Venugopala Rao (2002). Textbook of Environmental Engineering. PHI Learning Pvt. Ltd., pp. 184<\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/modeling-applications-and-tools<\/em><\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/photochemical-modeling-applications<\/em><\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/photochemical-modeling-tools<\/em><\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/dispersion-modeling-applications<\/em><\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/dispersion-modeling-applications<\/em><\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/multipollutant-modeling-applications<\/em><\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/air-quality-models<\/em><\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www.epa.gov\/scram\/meteorological-data-and-processors<\/em><\/li>\n<li style=\"text-align: justify\"><em>https:\/\/www3.epa.gov\/scram001\/dispersionindex.htm<\/em><\/li>\n<li style=\"text-align: justify\"><a href=\"http:\/\/elte.prompt.hu\/sites\/default\/files\/tananyagok\/AtmosphericChemistry\/ch10s03.html\"><em>http:\/\/elte.prompt.hu\/sites\/default\/files\/tananyagok\/AtmosphericChemistry\/ch10s03.html<\/em><\/a><\/li>\n<li style=\"text-align: justify\"><a href=\"http:\/\/people.math.sfu.ca\/~stockie\/atmos\/paper.pdf\"><em>http:\/\/people.math.sfu.ca\/~stockie\/atmos\/paper.pdf<\/em><\/a><\/li>\n<li style=\"text-align: justify\"><a href=\"https:\/\/www.ready.noaa.gov\/READY_gaussian.php\"><em>https:\/\/www.ready.noaa.gov\/READY_gaussian.php<\/em><\/a><\/li>\n<li style=\"text-align: justify\"><em>http:\/\/www.rrcap.ait.asia\/male\/Documents\/manual\/national\/04Chapter4.pdf<\/em><\/li>\n<li style=\"text-align: justify\"><a href=\"http:\/\/nptel.ac.in\/courses\/Webcourse-contents\/IIT-Delhi\/Environmental%20Air%20Pollution\/air%20pollution%20(Civil)\/Module-4\/1.htm\"><em>http:\/\/nptel.ac.in\/courses\/Webcourse-contents\/IIT-<\/em><\/a><a href=\"http:\/\/nptel.ac.in\/courses\/Webcourse-contents\/IIT-Delhi\/Environmental%20Air%20Pollution\/air%20pollution%20(Civil)\/Module-4\/1.htm\"><em>Delhi\/Environmental%20Air%20Pollution\/air%20pollution%20(Civil)\/Module-4\/1.htm<\/em><\/a><\/li>\n<li style=\"text-align: justify\"><a href=\"http:\/\/site.iugaza.edu.ps\/afoul\/files\/2010\/02\/chapter_7.pdf\"><em>http:\/\/site.iugaza.edu.ps\/afoul\/files\/2010\/02\/chapter_7.pdf<\/em><\/a><\/li>\n<li style=\"text-align: justify\"><a href=\"http:\/\/elte.prompt.hu\/sites\/default\/files\/tananyagok\/AtmosphericChemistry\/ch10s03.html\"><em>http:\/\/elte.prompt.hu\/sites\/default\/files\/tananyagok\/AtmosphericChemistry\/ch10s03.html<\/em><\/a><\/li>\n<li style=\"text-align: justify\"><a href=\"http:\/\/atoc.colorado.edu\/~saraht\/atoc1050\/Lecture_Notes\/chapter6-notes.pdf\"><em>http:\/\/atoc.colorado.edu\/~saraht\/atoc1050\/Lecture_Notes\/chapter6-notes.pdf<\/em><\/a><\/li>\n<\/ul>\n","protected":false},"author":3,"menu_order":9,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":["dr-puneeta-pandey"],"pb_section_license":""},"chapter-type":[],"contributor":[65],"license":[],"class_list":["post-127","chapter","type-chapter","status-publish","hentry","contributor-dr-puneeta-pandey"],"part":3,"_links":{"self":[{"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/pressbooks\/v2\/chapters\/127","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/wp\/v2\/users\/3"}],"version-history":[{"count":9,"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/pressbooks\/v2\/chapters\/127\/revisions"}],"predecessor-version":[{"id":620,"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/pressbooks\/v2\/chapters\/127\/revisions\/620"}],"part":[{"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/pressbooks\/v2\/parts\/3"}],"metadata":[{"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/pressbooks\/v2\/chapters\/127\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/wp\/v2\/media?parent=127"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/pressbooks\/v2\/chapter-type?post=127"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/wp\/v2\/contributor?post=127"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/ebooks.inflibnet.ac.in\/esp08\/wp-json\/wp\/v2\/license?post=127"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}