Dispersant Effectiveness as a Function of Energy ... · Dispersant Effectiveness as a Function of...
Transcript of Dispersant Effectiveness as a Function of Energy ... · Dispersant Effectiveness as a Function of...
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Dispersant Effectiveness as a Function of Energy Dissipation Rate
A collaboration of U.S. Environmental Protection Agency
Fisheries and Oceans Canada Temple University
Louisiana State UniversityCoastal Response Research Center
(National Oceanic and Atmospheric Administration)
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Investigators
• Albert D. Venosa, U.S. EPA, Cincinnati, OH• Kenneth Lee, Fisheries and Oceans Canada• Michel C. Boufadel, Temple University• Scott Miles, Louisiana State University• Zhengkai Li, DFO Canada• Tom King, DFO Canada• Paul Kepkay, DFO Canada
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Goals and Objectives
• Measure energy dissipation rates of a range of wave energiesRegular waveSpilling breakerPlunging breaker
• Quantify natural rates of dispersion of crude oils under these wave conditions
• Quantify effectiveness of 2 dispersants in enhancing dispersion of 2 reference crude oils at the 3 different energy dissipation rates
• Develop analytical tools for monitoring dispersion in the field
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EPA/DFO Wave Tank
• Wave tank originally fabricated 2 years ago (16 m x 2 m x 0.6 m)
• Wave tank doubled in length to 32 m to accommodate more wave types and bigger breakers
• Wave tank is able to generate reproducible breaking waves at precise locations
Methods have been developed that define the energy dissipation rate at various breaking wave energies
• Can be operated in either batch mode or continuous flow to simulate dilution by ocean currents
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5Regular Waves
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6Spilling Breaker
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Plunging Breaker
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Testing Dispersion Effectiveness
• Hypothesis: energy dissipation rate, ε, is sufficient to accurately evaluate dispersant effectiveness (DE)
• Approach: DE measured at 3 different wave periods using 2 dispersants and 2 oils under batch conditions
Dispersants on NCP Product ScheduleC9500SPC1000
Crude oilsWeathered Mesa LightUnweathered ANS
3 different ε’s:Regular waveSpilling breakerPlunging breaker
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11PlungerANSSPC100018
PlungerANSCorexit 17
PlungerANSWater16
PlungerMESASPC100015
PlungerMESACorexit 14
PlungerMESAWater13
SpillerANSSPC100012
SpillerANSCorexit 11
SpillerANSWater10
SpillerMESASPC10009
SpillerMESACorexit 8
SpillerMESAWater7
RegularANSSPC10006
RegularANSCorexit 5
RegularANSWater4
RegularMESASPC10003
RegularMESACorexit 2
RegularMESAWater1
WavesOilsDispersantsTreatment
Summary of Factorial Experimental Design
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General Approach
• Create oil slick on water surface• Start breaking or regular waves• DOR = 1:25 in all experiments• No-dispersant controls are also done, using water as
the sprayed “dispersant”• All experiments done in triplicate• Dispersed oil measured at 3 depths and 4 locations
along the length of the wave tank
Measurements conducted at 5, 30, 60, and 120 min One rep done at 240 min (re-coalescence experiment) under quiescent conditions
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Analytical and Wave Settings
• Oil distribution measurements in tank (3 methods):FluorometryLaser particle analyzer (LSST-100X)Spectrophotometric analysis of grab samples at 4 different locations, 1 upstream and 3 downstream from initial oil slick
• Total analyses: 3 dispersants x 2 oils x 3 wave types x 3 replicates x 4 sampling locations x 3 depths = 864 total analyses
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RESULTS:Dispersant Effectiveness vs. ε
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0
4
8
12
16
20
5 30 60 120 180 2400
4
8
12
16
20
Regular Wave
Spiller
Plunger
No Dispersant ControlANS
MESA
Time, Min
Ave
rage
Plu
me
Con
cent
ratio
n, m
g/L
Recoalescence Zone
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0
8
16
24
32
40
0
4
8
12
16
20
5 30 60 120 180 2400
4
8
12
16
20
5 cm
75 cm
140 cm
No Dispersant-Regular Wave
No Dispersant-Spiller
No Dispersant-Plunger
Time, Min
Ave
rage
Plu
me
Con
cent
ratio
n, m
g/L
Variability with Depth--ANS
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0
4
8
12
16
20
5 30 60 120 180 2400
4
8
12
16
20
Regular Wave
Spiller
Plunger
Corexit 9500ANS
MESA
Time, Min
Ave
rage
Plu
me
Con
cent
ratio
n, m
g/L
Recoalescence Zone
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0
4
8
12
16
20
5 30 60 120 180 2400
4
8
12
16
20
Regular Wave
Spiller
Plunger
SPC 1000ANS
MESA
Time, Min
Ave
rage
Plu
me
Con
cent
ratio
n, m
g/L
Recoalescense Zone
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RESULTS:Particle Size Distribution
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No Dispersant Control
115
75
45
15
Tim
e (m
in)
4080
120
Depth cm
0
50
100
150
200
250
300
350
MM
D (µ
m)
40
80
120
Corexit 9500
115
75
45
15
Tim
e (m
in)
4080
120
Depth (cm)
0
50
100
150
200
250
300
350
MM
D (µ
m)
near surfacemiddlenear bottom
Mass Mean Diameter under Regular Non-Breaking Waves (8m downstream)
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No Dispersant Control
115
75
45
15
Tim
e (m
in)
4080
120
Depth cm
0
50
100
150
200
250
300
350
MM
D (µ
m)
40
80
120
Corexit 9500
115
75
45
15
Tim
e (m
in)
4080
120
Depth (cm)
0
50
100
150
200
250
300
350
MM
D (µ
m)
near surfacemiddlenear bottom
Mass Mean Diameter under SpillingBreaking Waves (8m downstream)
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No Dispersant Control
115
75
45
15
Tim
e (m
in)
4080
120
Depth cm
0
50
100
150
200
250
300
350
MM
D (µ
m)
40
80
120
Corexit 9500
115
75
45
15
Tim
e (m
in)
4080
120
Depth (cm)
0
50
100
150
200
250
300
350
MM
D (µ
m)
near surfacemiddlenear bottom
Mass Mean Diameter under PlungingBreaking Waves (8m downstream)
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Results: Fluorometry
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240 260 280 300 320 340
300
400
500
600
0
8
16
24
240 260 280 300 320 340
Emis
sion
(nm
)
Excitation (nm)
Brent Brent plus Corexit
Contour plots of EEMs (excitation-emission matrix spectra) of Brent Blend crude in seawater.
J.Bugden, W. Yeung, P Kepkay & K. Lee (2007)Mar. Poll. Bull. (submitted)
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QA Question About Sample Storage
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0 10 20 30 40 50 60 70
time, days
5
6
7
8
9
10
Oil
Con
cent
ratio
n, m
g/L
Effect of Refrigerator Storage Time on Oil Concentration in Samples
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SUMMARY AND PRELIMINARY CONCLUSIONS
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SUMMARY AND CONCLUSIONS (preliminary)
• Breaking waves are important for effective and lasting dispersion
Breaking waves shear oil slick into tiny droplets that don’t easily recoalesceBreakers push oil downwards into water column where currents maycarry the dispersed oil away (to be verified next)
• Regular waves disperse oil somewhat but do not impart sufficientenergy to break up the oil into small droplets or push the droplets down deeply into the water column
• Chemical dispersants cause a huge difference in total dispersed oil and particle size distribution compared to no dispersant for all 3 wave conditions
• Correlations between DE and ε will enable more meaningful explanations of the data presented
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Acknowledgement
Funding for this project was provided by the Coastal Response Research Center
www.crrc.unh.edu
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Acknowledgment
Cost sharing also provided by theU.S. Environmental Protection Agency (EPA) and
Fisheries and Oceans Canada (DFO)
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Thank you. Questions?