direct observations of estuarine dispersion: results of a recent dye experiment

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Direct observations of estuarine dispersion: results of a recent dye experiment. Bob Chant Rutgers University. River. Pritchard’s Paradigm. Seaward at the surface. Pressure gradient and Velocity. But estuaries are often highly 3-dimensional with appreciable - PowerPoint PPT Presentation

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Page 1: Direct observations of  estuarine dispersion: results of a recent dye experiment
Page 2: Direct observations of  estuarine dispersion: results of a recent dye experiment

Direct observations of estuarine dispersion:results of a recent dye experiment

Bob Chant

Rutgers University

Page 3: Direct observations of  estuarine dispersion: results of a recent dye experiment

Pritchard’s Paradigm

Seaward atthe surface

Pressure gradient and Velocity

River

SUA

x

SASU

H

H

x

sK

z

sKwsusFlux Salt HV

xs

Kzs

KwsusFlux Salt HV

sux

sAeff

sss

uuu

Page 4: Direct observations of  estuarine dispersion: results of a recent dye experiment

Not a new question-- But observations are lacking.Current understanding is based on models (Zimmerman, Okubo, Fischer,

Smith) or indirect methods.

But estuaries are often highly 3-dimensional with appreciablecross channel gradients of salinity and velocity.

Do these processes impact stream-wise dispersion?

Page 5: Direct observations of  estuarine dispersion: results of a recent dye experiment

Salinity section May 21, 2001 2-days prior to injection

“Lagrangain studies of secondary circulation and mixing in a stratified channel”

NSF PI’s Chant, Geyer and Houghton.

Page 6: Direct observations of  estuarine dispersion: results of a recent dye experiment

Pilot Dye Study May 23-24, 2001. 4 more experiments planned for May, 2002Pilot study coincided with microstructure measurements by Hartmut Peters.

2002 injectionswill occur at spring and neap tide conditions

Page 7: Direct observations of  estuarine dispersion: results of a recent dye experiment

Figure 2 Study SiteInjection May 23, 2001

9:15-9:30 AMSalinity and velocity crosssections at time of release

Currents and salinityShip Track and Dye Trace

Page 8: Direct observations of  estuarine dispersion: results of a recent dye experiment

Upper layer Lower layer

Dye’s salinity distribution atrelease Currents and salinity

39 kg of fluorecene dye

Page 9: Direct observations of  estuarine dispersion: results of a recent dye experiment

Patch 2 (12:20 - 14:00)

Depth integrated dye

26 kg 1.8 kg

Page 10: Direct observations of  estuarine dispersion: results of a recent dye experiment

40.9

40.94

Cross Channel Sections during Flood2 hours after release

Page 11: Direct observations of  estuarine dispersion: results of a recent dye experiment

Patch 2 (12:20 - 14:00)

Depth integrated dye Integrated dye above 14 psu

26 kg 1.8 kg

Page 12: Direct observations of  estuarine dispersion: results of a recent dye experiment

25 kg

26 kg

Patch 3Patch 2

Page 13: Direct observations of  estuarine dispersion: results of a recent dye experiment

Patch 3 (14:00 - 15:40)

Depth integrated dye Integrated dye above 14 psu

25 kg

2.3 kg

Page 14: Direct observations of  estuarine dispersion: results of a recent dye experiment
Page 15: Direct observations of  estuarine dispersion: results of a recent dye experiment

Patch 4 (15:00 - 17:10)

Depth integrated dye

44 kg

Patch 3 (14:00 - 15:40)

Depth integrated dye

Page 16: Direct observations of  estuarine dispersion: results of a recent dye experiment

A series of cross-channel section during late ebb

Currents from ADCP

Page 17: Direct observations of  estuarine dispersion: results of a recent dye experiment

1

2

3

4

5

6

7

8

1

8

Page 18: Direct observations of  estuarine dispersion: results of a recent dye experiment
Page 19: Direct observations of  estuarine dispersion: results of a recent dye experiment

Patch 4 (15:00 - 17:10)

Depth integrated dye Integrated dye above 14 psu

44 kg16 kg

Page 20: Direct observations of  estuarine dispersion: results of a recent dye experiment

1

0.5

0

Page 21: Direct observations of  estuarine dispersion: results of a recent dye experiment
Page 22: Direct observations of  estuarine dispersion: results of a recent dye experiment

2zst

ssK

zst

sw

z

sKsw

v

e

ve

Vertical mixing estimates

Page 23: Direct observations of  estuarine dispersion: results of a recent dye experiment

we=0.09 mm/sKv=2.3* 10-3 m2/s

<S>=15.8

<S>=15.4

H > 10 m

<S>=15.5

<S>=15.2

we=0.05 mm/sKv= 1.0-3 m2/s

H < 10mMax Flood

we=0.05 mm/sKv=1.7* 10-3 m2/s

we=0.3 mm/sKv=1.3* 10-2 m2/s

<S>=15.2

<S>=14.2

Max Ebbwe=0.31 mm/sKv=1.1* 10-2 m2/s

we=0.28 mm/sKv=1.0* 10-2 m2/s

<S>=14.4

<S>=13.3

Page 24: Direct observations of  estuarine dispersion: results of a recent dye experiment
Page 25: Direct observations of  estuarine dispersion: results of a recent dye experiment

1

0.5

0

Slack before floodDay 1

Slack before ebbDay 2 ?

Page 26: Direct observations of  estuarine dispersion: results of a recent dye experiment
Page 27: Direct observations of  estuarine dispersion: results of a recent dye experiment

30 hours after release End of Ebb

m/s

+.5

-1.0

Current

12 16

May 24

Page 28: Direct observations of  estuarine dispersion: results of a recent dye experiment

FLOODAlong Channel sections during ebb

14:00 - 14:30

14:54 - 15:21

15:41 - 16:30

Dye Contour Intervals 0.2, 0.5, 1.0 2.0

Page 29: Direct observations of  estuarine dispersion: results of a recent dye experiment

Patch 5 (15:45 - 18:45)

Depth integrated dye Integrated dye above 14 psu

40 kg 20 kg

Page 30: Direct observations of  estuarine dispersion: results of a recent dye experiment
Page 31: Direct observations of  estuarine dispersion: results of a recent dye experiment

Conclusions

1) Lateral iso-pycnal advection of dye on flood

2) Mixing rates on flood are 10-3 and confined to bbm, suggestive of weak entrainment rates and thickening of BBL is due to flow convergence.

3) Mixing increases an order of magnitude on ebb. Diapycnaltransport occurs primarily on flank

4) Perfect dispersive process-- coupling between secondaryflow spatial variations in mixing and strong ebb shears. Suggestsartificial decomposition of diffusive processes is ...

5) Dye distribution after one tidal cycle is not consistent with simpletidal straining ideas.

6) While spread of dye is consistent with advection by estuarine flows (but mixingmay not be correct) observations clearly show that dispersion of dye is due to a 3-D tidal straining effect. Are estuarine flows then influenced by this mixing process?

7) Closure over-entrains on flood.

Page 32: Direct observations of  estuarine dispersion: results of a recent dye experiment

Salty

Fresh

Page 33: Direct observations of  estuarine dispersion: results of a recent dye experiment

Max 35

36 kg

1

16 kg

1

2

26 kg

2

3

25 kg

3

4

44 kg

4

5

40 kg

5

Page 34: Direct observations of  estuarine dispersion: results of a recent dye experiment

Simulation of Dye Release in Hudson

*Simulation by Rocky Geyer

Ebb Flood

Page 35: Direct observations of  estuarine dispersion: results of a recent dye experiment

Patch 1 (11:00 - 12:15)

Depth integrated dye Integrated dye above 14 psu

16 kg 0.6 kg

Page 36: Direct observations of  estuarine dispersion: results of a recent dye experiment

* H > 10m* H < 10m

Dye weighted salinity of each cast

Page 37: Direct observations of  estuarine dispersion: results of a recent dye experiment

.. Or is it driven by secondarycirculation and mixing on

the margins?

Is diapycnal transport primarily associatedwith vertical mixing?

“Lagrangain studies of secondary circulation and mixing in a

stratified channel”NSF PI’s Chant, Geyer (WHOI)

and Houghton (LDEO)

Note: May dominate diapycnalmixing process in global ocean

Page 38: Direct observations of  estuarine dispersion: results of a recent dye experiment

End of Flood

End of Ebb

End of Flood

Page 39: Direct observations of  estuarine dispersion: results of a recent dye experiment

30 hours after release

xssu

A

TLA

eff

eff

/2

Two crude estimates of effective horizontal dispersion….

…both suggest Aeff=1000 m2/s