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Monroe L. Weber- Shirk School of Civil and Environmental Engineering Turbulent Jets and Plumes
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Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Jan 12, 2016

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Page 1: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Monroe L. Weber-Shirk

School of Civil and Environmental Engineering

Turbulent Jets and PlumesTurbulent Jets and Plumes

Page 2: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Turbulent Jets and PlumesTurbulent Jets and Plumes

Discharge of society’s wastes into the environment smokestacks wastewater discharges automobile exhaust

Natural events volcanoes forest fires dragons

Discharge of society’s wastes into the environment smokestacks wastewater discharges automobile exhaust

Natural events volcanoes forest fires dragons

DragonsDragons

http://www.riverdale.k12.or.us/helens/slides/

slide.htm

Page 3: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Some definitionsSome definitions

momentummomentum

densitydensity

momentummomentum

buoyancybuoyancy

Jet driven by _________ of the source Ex. garden hose submerged in swimming pool

Plume driven by ________ differences Ex. smoke from open fire

Buoyant Jet combination of momentum of source and density Ex. Wastewater discharge into ocean initial flow controlled by _________ far from source controlled by _________

Jet driven by _________ of the source Ex. garden hose submerged in swimming pool

Plume driven by ________ differences Ex. smoke from open fire

Buoyant Jet combination of momentum of source and density Ex. Wastewater discharge into ocean initial flow controlled by _________ far from source controlled by _________

Page 4: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Turbulent Jet and Plume Characteristics

Turbulent Jet and Plume Characteristics

Jet efficient mixing with the ambient fluid kinetic energy is lost to turbulence momentum is conserved

Plume efficient mixing with the ambient fluid potential energy is converted to kinetic energy kinetic energy is lost to turbulence momentum is conserved (but must take body force into

account)

Jet efficient mixing with the ambient fluid kinetic energy is lost to turbulence momentum is conserved

Plume efficient mixing with the ambient fluid potential energy is converted to kinetic energy kinetic energy is lost to turbulence momentum is conserved (but must take body force into

account)

Page 5: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Jet ParametersJet Parameters

initial jet velocity initial turbulence of discharge jet mass flux jet momentum flux jet tracer material

heat salinity contaminant

initial jet velocity initial turbulence of discharge jet mass flux jet momentum flux jet tracer material

heat salinity contaminant

Page 6: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Environmental ParametersEnvironmental Parameters

ambient turbulence levels currents

cross flows co flows counter flows

density stratification thermal salinity

ambient turbulence levels currents

cross flows co flows counter flows

density stratification thermal salinity

Page 7: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Geometrical FactorsGeometrical Factors

jet discharge port shape orientation proximity to adjacent jets proximity to solid boundaries attitude of the jet distance to free surface

jet discharge port shape orientation proximity to adjacent jets proximity to solid boundaries attitude of the jet distance to free surface

Page 8: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

What we’d like to knowWhat we’d like to know

Contaminant concentration as function of distance from source

Velocity of jet or plume as function of distance

Width of jet or plume as function of distance

Contaminant concentration as function of distance from source

Velocity of jet or plume as function of distance

Width of jet or plume as function of distance

3 unknowns, so we need 3 equations!3 unknowns, so we need 3 equations!

Page 9: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Tools to get thereTools to get there

From basic principles conservation of momentum conservation of mass (of tracer) conservation of energy rate of spread of jet (spreading law)?

From dimensional analysis need to identify the important parameters still need spreading law

From basic principles conservation of momentum conservation of mass (of tracer) conservation of energy rate of spread of jet (spreading law)?

From dimensional analysis need to identify the important parameters still need spreading law

Page 10: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Cases to analyzeCases to analyze

Jet round jet plane jet

Plume round plume plane plume

Jet round jet plane jet

Plume round plume plane plume

Page 11: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Axisymmetric JetAxisymmetric Jet

Geometry round axisymmetric 3-d problem

Ambient water much less shear

than in jet no flow (for this

simple case)

Geometry round axisymmetric 3-d problem

Ambient water much less shear

than in jet no flow (for this

simple case)

ddJet: , Vo, CoJet: , Vo, Co

edge of jet turbulenceedge of jet turbulence

velocity profile(statistical mean)velocity profile(statistical mean)

Ambient: , V=0, C=0Ambient: , V=0, C=0

Page 12: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

bb

Simple Jet SpreadingSimple Jet Spreading

dd

Vu ' Vu '

V

u

ds

db 'V

u

ds

db '

sb sb

velocity fluctuations at any location are proportional to the velocity of the jet at that location

velocity fluctuations at any location are proportional to the velocity of the jet at that location

ss

dsuVdb ' dsuVdb '

Page 13: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Momentum: Axisymmetric JetMomentum: Axisymmetric Jet

2

4bA

2

4bA

jet spreading equationjet spreading equation

02

02 AVAV 0

20

2 AVAV

220

22

44dVbV

22

022

44dVbV

dVVb o dVVb o b

dVV o

b

dVV o

s

dVV o s

dVV o

external forces balance external forces balance b

dd

ss

controlvolumecontrolvolume

substitute for areasubstitute for area

sspp FFFWMM 00 sspp FFFWMM 00

020

20 AVAV 02

02

0 AVAV

sb sb

M term

here?

Page 14: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Concentration of Conservative Tracer: Axisymmetric Jet

Concentration of Conservative Tracer: Axisymmetric Jet

MM 0 MM 0

QCCQ 00 QCCQ 00

QCM QCM

VbAVQ 2

4

VbAVQ 2

4

02

00

4VdVAQo

0

200

4VdVAQo

VCbCVd 200

2

44

VCbCVd 2

002

44

at steady state mass flux [M/T] is constantat steady state mass flux [M/T] is constant

b

dd

ss

Page 15: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Concentration of Conservative Tracer: Axisymmetric Jet

Concentration of Conservative Tracer: Axisymmetric Jet

b

dd

ss

Vb

CVdC

2

002

Vb

CVdC

2

002

s

dVs

CVdC

02

002

s

dVs

CVdC

02

002

s

dVV o s

dVV o

s

dCC 0s

dCC 0

(jet spreading)(jet spreading)

(velocity in jet)(velocity in jet)

VCbCVd 200

2 VCbCVd 200

2

sb sb

Page 16: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Round Jet: Empirical ConstantsRound Jet: Empirical Constants

s

dVV o s

dVV o

s

dCC 0s

dCC 0

sb 107.0 sb 107.0

s

dVV oc 2.6

s

dVV oc 2.6

s

dCC oc 0.5

s

dCC oc 0.5

sb sb

b is defined such that the velocity is ____________ of the centerline velocity

ddJet: , Vo, CoJet: , Vo, CoCenterline velocity and concentration

37% (1/e)37% (1/e)

Page 17: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Plane: (2-D) JetsPlane: (2-D) Jets

Spreading of the jet will be by the same mechanism

Momentum conservation will give a different relationship for centerline velocity

Spreading of the jet will be by the same mechanism

Momentum conservation will give a different relationship for centerline velocity

020

20 bVbV 02

02

0 bVbV

b

bVV o

0 b

bVV o

0 s

bVV o

0 s

bVV o

0 show this for HWshow this for HW

00 MM 00 MM

020

20 AVAV 02

02

0 AVAV

s

bCC o

0s

bCC o

0

sb sb

Per unit lengthPer unit length

Page 18: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Plane Jets: Empirical Coefficients

Plane Jets: Empirical Coefficients

s

bVV o

0 s

bVV o

0

s

bCC o

0s

bCC o

0

sb 116.0 sb 116.0

s

bVV oc

041.2 s

bVV oc

041.2

s

bCC oc

038.2s

bCC oc

038.2

sb sb

Page 19: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Jet Design ProblemJet Design Problem

Given a discharge with an environmental requirement of achieving a high dilution measured at the surface of a body of water. What are the three things you can do to maximize the dilution of the discharge before the jet reaches the water surface?

Given a discharge with an environmental requirement of achieving a high dilution measured at the surface of a body of water. What are the three things you can do to maximize the dilution of the discharge before the jet reaches the water surface?

s

dCC oc 0.5

s

dCC oc 0.5

s

bCC oc

038.2s

bCC oc

038.2

round jetround jet

plane jetplane jetIncrease depth of submergenceIncrease depth of submergence

Decrease port size (multiple ports!)Decrease port size (multiple ports!)

Discharge at an angleDischarge at an angle

Page 20: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

PlumesPlumes

less well defined boundary between plume and ambient (billows)

full description of velocities and concentrations is very complex

time averaged shape of plume similar to jet (same spreading law)

momentum still conserved but with inclusion of a ____ force (due to buoyancy)

less well defined boundary between plume and ambient (billows)

full description of velocities and concentrations is very complex

time averaged shape of plume similar to jet (same spreading law)

momentum still conserved but with inclusion of a ____ force (due to buoyancy)bodybody

Page 21: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Plume ExercisePlume Exercise

What parameters are important in determining the time averaged centerline velocity in the plume?

Develop an expression for centerline velocity that is dimensionally correct.

Does your expression make sense?

What parameters are important in determining the time averaged centerline velocity in the plume?

Develop an expression for centerline velocity that is dimensionally correct.

Does your expression make sense?

Page 22: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Round Plume:Equation Development

Round Plume:Equation Development

),( sBfV ),( sBfV

3

4

][T

LB

3

4

][T

LB

3/1

s

BV

3/1

s

BV

QCCQ 00 QCCQ 00VCbCQ 2

00

4

VCbCQ 2

00

4

Vb

CQC

2

004

Vb

CQC

2

004

sb sb

DimensionalanalysisDimensionalanalysis

tracer mass conservationtracer mass conservation

3/1

s

BV

3/1

s

BV

0gQB 0gQB

3/1

2

004

s

Bs

CQC

3/1

2

004

s

Bs

CQC

3/13/5

00

Bs

CQC

3/13/5

00

Bs

CQC

Buoyancy fluxBuoyancy flux

Page 23: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Plume coefficientsPlume coefficients

round plumeround plume plane plumeplane plume

sb 1.0 sb 1.0

3/13/5

001.9Bs

CQCc

3/13/5

001.9Bs

CQCc

3/1

7.4

s

BVc

3/1

7.4

s

BVc

sb 12.0 sb 12.0

3/166.1 BVc 3/166.1 BVc

3/1

0038.2sB

CqCc

3/1

0038.2sB

CqCc

q0 discharge per unit lengthq0 discharge per unit length

gQBa gQBa gqB

a gqBa

Independent of s!

Page 24: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Buoyant JetsBuoyant Jets

A jet whose density differs from the receiving water

Jet-like characteristics close to the source Plume-like characteristics far from the

source the plume-like characteristics always win!

Examples

A jet whose density differs from the receiving water

Jet-like characteristics close to the source Plume-like characteristics far from the

source the plume-like characteristics always win!

Examples

Page 25: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

CORMIXCORMIX

Simulation of turbulent buoyant jet mixing behavior in the… near-field (the initial jet characteristics of momentum flux, buoyancy

flux, and outfall geometry influence the jet trajectory and mixing) far-field (density current region followed by a passive diffusion

region) The hydrodynamic simulation system contains a collection of

regional flow models based on… Integral (conservation of mass, heat, and momentum) length scale (based on dimensional analysis) passive diffusion (turbulence in the ambient environment becomes the

dominating mixing mechanism)

CORMIX

Page 26: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Jets and Plumes:Summary

Jets and Plumes:Summary

Simple analytical equations describe time averaged values for velocity and concentrations in jets and plumes

Interactions with the environment (boundaries, cross flows, density differences) complicate the description of jets and plumes

Computer based expert system developed at Cornell (CORMIX) can be used to predict interaction of jets and plumes with the environment

Predictions based on combination of theory and empirical studies using dimensional analysis

Simple analytical equations describe time averaged values for velocity and concentrations in jets and plumes

Interactions with the environment (boundaries, cross flows, density differences) complicate the description of jets and plumes

Computer based expert system developed at Cornell (CORMIX) can be used to predict interaction of jets and plumes with the environment

Predictions based on combination of theory and empirical studies using dimensional analysis

Page 27: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Dragon Day Plume

Page 28: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Mount Saint HelensMount Saint Helens

http://www.riverdale.k12.or.us/helens/slides/slide.htm

Page 29: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Integrated Forest Fire Management Project

(IFFM)Indonesia

Integrated Forest Fire Management Project

(IFFM)Indonesia

Page 30: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Slurry PlumesSlurry Plumes

slurry plumes for three increasing sizes of near-uniform sand diffusing in an ambient. The smallest size is around

0.2mm

slurry plumes for three increasing sizes of near-uniform sand diffusing in an ambient. The smallest size is around

0.2mm

http://maligne.civil.ualberta.ca/water/research/restopics/arbind/slplume.html

Page 31: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Momentum of DischargeMomentum of Discharge

small portsmall port momentummomentum jet mixingjet mixing

large portlarge port momentummomentum jet mixingjet mixing

Page 32: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Multiport Diffuser ValvesMultiport Diffuser Valves

http://www.redvalve.com/brochure/diffuser.html

Page 33: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Boston HarborBoston Harbor

http://crusty.er.usgs.gov/

Page 34: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Massachusetts Bay Massachusetts Bay

http://crusty.er.usgs.gov/

Page 35: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Tidal Flushing of Boston Harbor

Tidal Flushing of Boston Harbor

http://crusty.er.usgs.gov/

Boston Harbor tidal cycles

Simulation of tidal exchange in Boston Harbor , based on a high-resolution (100 m grid spacing) depth-averaged computer model. Water in Boston Harbor is dyed red, and tracked over three tidal cycles. Colors between red and blue represent mixing of Boston Harbor water with Massachusetts Bay water (dyed blue). Due to the jet-like behavior of the ebb tidal currents, water is expelled from the harbor in pulses, leading to effective flushing of the harbor over several days.

Page 36: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Spring Freshet in Massachusetts Bay: April-May 1992

Spring Freshet in Massachusetts Bay: April-May 1992

Spring Freshet

Near-surface salinity (2 m depth) is tracked during May 1992, revealing a plume of fresh water from the Merrimack River that moves into Massachusetts Bay. The yellow arrow that flops around indicates the wind direction and speed. Note that a snapshot of the salinity on May 22 (as one might sample from a monthly CTD cruise) would give the distinct visual impression of a large plume from Boston Harbor, when in fact most of this water came from the Merrimack River!

http://crusty.er.usgs.gov/

Page 37: Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Turbulent Jets and Plumes.

Boston Harbor Sewage Outfalls Effluent Concentration

Boston Harbor Sewage Outfalls Effluent Concentration

Effect of new Boston Outfall

Simulation of effluent dilution from the existing and future Boston Sewage effluent outfalls based on a three-dimensional circulation model of Massachusetts Bay during Jan-Mar 1990 and Jun-Aug 1990. Isosurfaces (three-dimensional contours) of effluent concentration are shown representing 1 part effluent to 200 parts seawater. This is a level below which nutrient inputs due to the outfall should be hard to distinguish above background fluctuations. During both the winter and summer months the effluent from the future outfall (represented by the blue isosurface) covers a smaller region than the effluent from the existing outfall (represented by the purple isosurface).

These simulations were used as evidence to assess the impact of the future outfall on endangered right whales.

http://crusty.er.usgs.gov/