Canarina software for analysis of air pollution in environment: environmental engineering, environmental consultancy service, environment simulation, environmental modeling and environmental impact assessment.

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Plume Rise Formulas

The plume height is used in the calculation of the Vertical Term. The distance dependent momentum plume rise equations are used to determine if the plume is affected by the wake region for building downwash calculations. 

Stack-tip Downwash

In order to consider stack-tip downwash, modification of the physical stack height is performed. The modified physical stack height hs is found from:

hs’=hs+2ds[(vs/us)-1.5]   for  vs<1.5us      (5)

or

hs’=hs                   for vs> o =1.5us   (6)

where hs is physical stack height (m), vs is stack gas exit velocity (m/s), and ds is stack top diameter (m). If stack tip downwash is not considered, hs’= hs in the following equations.

Buoyancy and Momentum Fluxes

For most plume rise situations, the value of the Briggs buoyancy flux parameter, Fb (m4/s3), is needed

Fb=gvsds2(DT/4Ts)    (7)

where DT = Ts - Ta, Ts is stack gas temperature (K), and Ta is ambient air temperature (K).

For determining plume rise, the momentum flux parameter, Fm (m4/s2), is calculated based on the following formula:

Fm=gvs2ds2(Ta/4Ts)    (8)

Unstable or Neutral - Crossover Between Momentum and Buoyancy

For cases with stack gas temperature greater than or equal to ambient temperature, it must be determined whether the plume rise is dominated by momentum or buoyancy. The crossover temperature difference, (DT)c, is determined as follows:

for Fb < 55,

(DT)c=0.0297 Ts(vs/ds2)1/3      (9)

and for Fb >= 55,

(DT)c=0.00575 Ts(vs2/ds)1/3     (10)

If DT, exceeds or equals (DT)c, plume rise is assumed to be buoyancy dominated, otherwise plume rise is assumed to be momentum dominated.

Unstable or Neutral - Buoyancy Rise

For situations where DT exceeds (DT)c as determined above, buoyancy is assumed to dominate. The distance to final rise, xf, is assumed to be 3.5x*, where x* is the distance at which atmospheric turbulence begins to dominate entrainment. The value of xf is calculated as follows:

for Fb < 55:

xf=49Fb5/8      (11)

and for Fb >= 55:

xf=119Fb2/5     (12)

The final effective plume height, he (m), is determined as

for Fb < 55:

he=hs+(21.425 Fb3/4/us)    (13)

and for Fb = 55:

he=hs+(38.71 Fb3/5/us)          (14)

Unstable or Neutral - Momentum Rise

For situations where the stack gas temperature is less than or equal to the ambient air temperature, the assumption is made that the plume rise is dominated by momentum. If DT is less than (DT)c, the assumption is also made that the plume rise is dominated by momentum. The plume height is calculated as:

he=hs+3ds(vs/us)     (15)

Briggs suggests that this equation is most applicable when vs/us is greater than 4.

Stability Parameter

For stable situations, the stability parameter, s, is calculated:

s=g[(dT/dz)/Ta]         (16)

As a default approximation, for stability class E (or 5) dT/dz is taken as 0.020 K/m, and for class F (or 6), dT/dz is taken as 0.035 K/m.

Stable - Crossover Between Momentum and Buoyancy

For cases with stack gas temperature greater than or equal to ambient temperature, it must be determined whether the plume rise is dominated by momentum or buoyancy. The (DT)c  is determined and solving for DT, as follows:

(DT)c=0.019582 Ts vs s1/2      (17)

If the difference between DT exceeds or equals (DT)c, plume rise is assumed to be buoyancy dominated, otherwise plume rise is assumed to be momentum dominated.

Stable - Buoyancy Rise

For situations where DT exceeds (DT)c as determined above, buoyancy is assumed to dominate. The distance xf is determined by

xf=2.0715 us s-1/2        (18)

The plume height, he, is determined by

he=hs+2.6 [Fb/(uss)]1/3         (19)

Stable - Momentum Rise

Where the stack gas temperature is less than or equal to the ambient air temperature, the assumption is made that the plume rise is dominated by momentum. Then,

he=hs+1.5[Fm/(uss1/2)]1/3       (20)

The equation for unstable-neutral momentum rise is also evaluated. The lower result of these two equations is used as the resulting plume height.

 

Algorithms I - Algorithms II - Algorithms III - Algorithms IV - Algorithms V

 

 

 

Air pollution map (XY-Plane) produced by continuous discharge in time (three stacks). The red colour represents high pollutant concentrations. Wind: SE (135 degrees).

 

 

Air pollution map (XY-Plane) produced by continuous discharge in time. The fucshia lines represents a stacks in the XY-Plane. The red colour represents high pollutant concentrations. Winds: E (90 dregrees) and 70 degrees.

 

Canarina Algoritmos Numéricos, S.L.

Environmental software solutions

                    

                          

Canary Islands, Spain

e-mail: info1@canarina.com

 

 

 

European network on pollution · European Union

Member of MAPO: European network on Marine Pollution. Project

funded by the European Commission through the

6th Framework Programme for Research and Development

 

air pollution control

 

                 

Air pollution dispersion · DISPER - Software solutions - Software advantages - Price - Input data I - Input data II - Input data III - Input data IV - Average - Import data - Software commands - Math. algorithms I - Math. algorithms II - Math. algorithms III - Math. algorithms IV - Math. algorithms V - Emissions - Pollutants I - Pollutants II - Graphs I - Graphs II

 

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