Observed aerosol effects on marine cloud nucleation and supersaturation
Lynn M. Russell, Armin Sorooshian, John H. Seinfeld, Bruce A. Albrecht, Athanasios Nenes, W. Richard Leaitch
, Anne Marie Macdonald, Lars Ahlm, Yi-Chun Chen, Matthew Coggon, Ashley Corrigan, Jill S. Craven, Richard
C. Flagan, Amanda A. Frossard, Lelia N. Hawkins, Haflidi Jonsson, Eunsil Jung, Jack J. Lin, Andrew R. Metcalf,
Robin Modini, Johannes Mülmenstädt, Greg C. Roberts, Taylor Shingler, Siwon Song, Zhen Wang, and Anna
Wonaschütz
Citation: AIP Conference Proceedings
1527
, 696 (2013); doi: 10.1063/1.4803366
View online: http://dx.doi.org/10.1063/1.4803366
View Table of Contents: http://scitation.aip.org/content/aip/proceeding/aipcp/1527?ver=pdfcov
Published by the AIP Publishing
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Observed
Aerosol
Effects on Marine
Cloud
Nucleation and Supersaturation
Lynn M. Russell
a
, Armin Sorooshian
c
,
g
, John H. Seinfeld
b
, Bruce A. Albrecht
e
,
Athanasios Nenes
d
,
W. Richard Leaitch
k
, Anne Marie Macdonald
k
,
Lars Ahlm
a
, Yi
-
Chun Chen
b
, Matthew Coggon
b
,
Ashley Corrigan
a
, Jill S. Craven
b
, Richard C. Flagan
b
,
Amanda A. Frossard
a
,
Lelia N. Hawkins
l
,
Haflidi Jonsson
f
, Eunsil Jung
e
, Jack J. Lin
d
,
Andrew R. Metcalf
b
,
j
, Robin Modini
a
, Johannes Mülmenstädt
a
, Greg C. Roberts
a
,
i
,
Taylor Shingler
c
, Siwon Song
e
, Zhe
n Wang
c
, Anna Wonaschütz
g
a
Scripps Institution of Oceanography, University of California, San Diego, La Jolla, CA.
b
California Institute of Technology, Pasadena, CA.
c
Department of Chemical and Environmental Engineering, University of Arizona, Tucson, AZ.
d
School of Earth and Atmospheric Sciences, Georgia Institute of Technology, Atlanta, GA.
e
Rosenstiel School of Marine Sciences, University of Miami, Miami, FL.
f
Center Interdisciplinary Remotely
-
Piloted Aerosol Studies, Marina, CA.
g
Department of Atmospher
ic Sciences, University of Arizona, Tucson, AZ.
h
Department of Chemical and Biomolecular Engineering, Georgia Institute of Technology, Atlanta, GA.
i
Centre National de la Recherche Scientifique, Toulouse, France.
j
Now at Combustion Research Facility, Sandi
a National Laboratories, Livermore, CA.
k
Environment Canada, Toronto, Canada.
l
Harvey Mudd College, Claremont, CA.
Abstract.
Aerosol particles in the marine boundary layer include primary organic and salt
particles from sea spray and combustion
-
derived par
ticles from ships and coastal cities. These
particle types serve as nuclei for marine cloud droplet activation, although the particles that
activate depend on the particle size and composition as well as the supersaturation that results
from cloud updraft
velocities
. The Eastern Pacific Emitted Aerosol Cloud Experiment (E
-
PEACE) 2011 was a targeted aircraft campaign
to assess how different particle types nucleate
cloud droplets. As part of E
-
PEACE 2011, we studied the role of marine particles as cloud
drop
let nuclei and used
emitted particle sources to separate particle
-
induced feedbacks from
d
ynamical variability. The emitted particle sources included
shipboard smoke
-
generated
particles with 0.05
-
1 μm diameters (which produced tracks measured by satellite
and had drop
composition charac
teristic of organic smoke) and
combustion particles from container ships with
0.05
-
0.2 μm diameters (which were measured in a variety of conditions with droplets containing
both org
anic and sulfate components)
[1]
. Three central aspects of the collaborative E
-
PEACE
results are: (1) the size and chemical composition of the emitted smoke particles compared to
ship
-
track
-
forming cargo ship emissions as well as backg
round marine particles, with particular
attention to the role of organic particles, (2) the characteristics of cloud track formation for
smoke and cargo ships, as well as the role of multi
-
layered low clouds, and (3) the implications
of these findings for
quantifying aerosol indirect effects. For comparison with the E
-
PEACE
results, the preliminary results of the Stratocumulus Observations of Los
-
Angeles Emissions
Derived Aerosol
-
Droplets (SOLEDAD) 2012 provided evidence of the cloud
-
nucleating roles of
bo
th marine organic particles and coastal urban pollution, with simultaneous measurements of
the effective supersaturations of the clouds in the California coastal region. .
Nucleation and Atmospheric Aerosols
AIP Conf. Proc. 1527, 696-701 (2013); doi: 10.1063/1.4803366
© 2013 AIP Publishing LLC 978-0-7354-1152-4/$30.00
696
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Keywords:
Atmospheric Aerosol, Marine Aerosol, Cl
oud Properties, Aerosol
-
Cloud
Interactions, Marine Boundary Layer.
PACS:
92.60.Mt, 92.60.Nv.
EASTERN PACIFIC EMIT
TED AEROSOL CLOUD
EXPERIMENT (E
-
PEACE) 2011
E
-
PEACE combined a targeted aircraft campaign off the coast of Monterey,
California, in July and A
ugust 2011, with embedded ship
(Fig.
1)
and satellite
observations and modeling studies. Atmospheric conditions in the northeastern Pacific
during July are ideal for formation of homogeneous layers of persistent stratocumulus
clouds. The layers observed h
ave consistent diurnal characteristics, cloud thicknesses
of 100 to 300 m, and cloud top heights typically below 500 m. We employed the R/V
Point Sur
to measure the aerosol below cloud and as a platform for well
-
characterized
smoke emissions to produce a
uniquely identifiable cloud signature. The Center for
Interdisciplinary Remotely
-
Piloted Aircraft Studies (CIRPAS) Twin Otter aircraft was
used with a full
payload of instruments
to measure particle and clou
d number, mass,
and composition.
FIGURE
1
.
R/V
Point Sur
from the CIRPAS Twin Otter during E
-
PEACE 2011, showing the
persistence of the plume of smoke generated on the ship in the atmosphere and some of the aircraft
instruments for
measuring particles and clouds (Photo
graph modified from Russell et al.
[1]
).
The Twin Otter aircraft flew into
clouds behind the emissions from ships
. Figure
2
shows
one example of measurements of
the number of particles below
cloud and
droplets in cloud, and the pie graphs show that these droplets were almost entirely
organic components with trace amounts of sulfate. The measured ship and marine
characteristics of the organic components during E
-
PEACE were used to quantify th
e
widespread contributions of ship emissions to the marine boundary layer aerosol
[2]
.
The counterflow virtual impactor (CVI) was used as an inlet for evaporating droplets
as they were b
rought into the aircraft, allowing sampling of droplet chemical
composition
[3]
.
The large organic fraction in Fig.
2
A is characteristic of smoke
emitted from the generators on the R/V
Point Sur
and contrasts with the composition
697
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of droplets in the cloud not affected by t
he smoke (Fig.
2
C), which are made up of
three
-
quarters sulfate and
few
organic components.
FIGURE 2.
Examples of particle and droplet number distributions and mass
-
based non
-
refractory
chemical composition, from measurements below (bottom panel) and i
n (top panel) cloud, for the
smoke generator on the R/V
Point Sur
on 16 July (
panel A) and for the stack emissions of a c
argo ship
on 10 August (
panel B). The background particle and droplet concentrations are shown for
16 July and
10 August (
panels C and
D, respectively). The size distributions are plotted at the measured relative
humidity, wet for s
upermicron droplets in cloud (triangles
-
up
: 3
μ
m < CDP < 50
μ
m for 16 July and 1
μ
m < CAS < 50
μ
m for 10 August), with passive heating for submicron particle
s in (in
terstitial) and
below cloud (triangles
-
down
: 0.1
μ
m < PCASP < 2
μ
m), and dried below cloud (diamonds
: 0.01
μ
m <
Scanning DMA < 0.9
μ
m). The pies show composition of the droplets in cloud measured by AMS for
submicron particles below cloud (bottom p
anel) and for the residuals of cloud droplets (top panel) that
are left after drying in a counterflow virtual impactor (11
μ
m < CVI), with
light grey for
organi
c
components and dark grey for
sulfate). Refractory chemical components (such as Sea Salt) were
not
measured behind the CVI and are not included in the pie graphs. The measurements were collected on
the CIRPAS Twin Otter on 10 August for the cargo ship (1651
-
1831) and 16 July for the smoke
generators (1704
-
1801)
. (Reproduc
ed from Russell et al.
[2]
,
u
sed with permission
.
©
American
Meteorological
Society
)
698
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It is interesting that the background cloud droplets also have 10
-
30% organic
components. Since the organic composition
outside of
the smoke and ship plumes was
very similar to characteristic organic functional groups associated with marine sources
[4]
, it is likely that this organic fraction was of marine origin. The presence of a
similar organic fraction in the droplet residuals shows that this organic mass also acted
as CCN in nucleating
cloud drops.
To understand the differences in the two days shown in Fig. 2, we compared the
measured updraft velocity and estimated the maximum supersaturation by comparing
the cloud drop number (CDN) concentration with the cloud condensation nuclei
(CCN)
spectra. The results for the two days are given in Table 1, which is taken from
Russell et al.
[1]
.
While there is uncertainty in using the maximum supersaturation
calculated from the measur
ed average CDN and the CCN spectra, the calculated
updraft velocities were consistent with the measured maximum updraft velocities (in
cloud) of 0.94 m s
-
1
(respectively) on 16 July and
1.2 m s
-
1
(respectively) on 10
Aug
ust.
TABLE
1
.
Particle and droplet characteristics for below and in
-
cloud measurements shown in Fig. 2.
Measured Maximum Updraft
Velocity [m s
-
1
]
Calculated Maximum
Supersaturation [%]
16 July 2011 (generator smoke)
0.94
0.09
10 August 2011 (cargo ship)
1.22
0.25
STRATOCUMULUS OBSERV
ATIONS OF LOS
-
ANGELES
EMISSIONS DERIVED AE
ROSOL
-
DROPLETS (SOLEDAD) 2
012
Stratocumulus Observations of Los
-
Angeles Emissions Derived Aerosol
-
Droplets
(SOLEDAD) 2012 took place during May and June in La Jolla, California. Aerosol
parti
cles were sampled at Scripps pier and at the peak of Mount Soledad, 1.5 mi from
the pier sampling location and 250 m above sea level. Stratocumulus clouds were
observed frequently at levels between 100 and 500 m, and there were several
nighttime cloud lay
ers during which the mountaintop site was in cloud. One such
event is shown in Fig. 3. These events tended to be characterized by onshore winds
and CDN concentrations below 100 cm
-
3
, suggesting that the clouds were similar to
the marine stratocumulus sam
pled during E
-
PEACE 2011.
The SOLEDAD 2012 campaign provided the opportunity to measure drop
formation in coastal conditions and to calculate supersaturation by a second method.
In this campaign, several hours of sampling in cloud allowed us to use measur
ements
of CCN concentration behind the counterflow virtual impactor to compare the
measured supersaturation of the droplet residuals to the CDN concentration. With this
approach, we measured a distribution of supersaturations during up to 6 hr of sampling
in each cloud event. The values ranged from below 0.1% to above 0.7%, although
most were below 0.4%. It is possible that the larger supersaturations reflect the
contributions of scavenged components to the droplet composition, but it is also likely
that
this range reflects the variability in updraft velocities.
699
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FIGURE
3
.
Instrumented van on Mount Soledad during a stratocumulus cloud measured as part of
SOLEDAD 2012. The picture shows the rotating aerosol inlet, the counterflow virtual impactor, in
-
cloud spectrometers, and an active
-
flow cloud water collector.
CLOUD NUCLEATION AND
SUPERSATURATION
For both campaigns, online measurements of non
-
refractory components in aerosol
particles below cloud and droplet residual in cloud show very similar compo
sitions
–
in other words the similarity of droplet and submicron aerosol composition in multiple
marine stratocumulus cloud events suggests that that the accumulation mode mass is
responsible for most of the nucleating droplets. While some droplet composi
tions will
be changed by scavenging of interstitial particles, the very similar fractions of
different components suggests that the nucleated particles are largely the same as the
submicron particles in composition. A striking example is provided by the dr
op
residuals composed of generated smoke nuclei, since their composition indicates the
ability of very “fresh” hydrocarbon emissions to nucleate cloud droplets at low
supersaturations with negligible hygroscopic uptake by sulfate.
These results were found
for clouds with a range of supersaturations typical of
marine stratocumulus, from below 0.1% up to 0.4%. We estimated these effective
supersaturations in two ways, both by directly comparing the activated droplet
population to the measured CCN spectra an
d by measuring the CCN spectra of the
700
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131.215.71.79 On: Mon, 10 Mar 2014 17:28:35
droplet residuals. Interestingly, this variability is comparable to the values used to
calculate that in
-
cloud sulfate formation could contribute to new CCN
[5]
.
ACKNOWLEDGMENTS
The E
-
PEACE 2011 field campaign and modeling studies were funded by the
National Science
Foundation (AGS
-
1013423; AGS
-
1008848; AGS
-
1013381; AGS
-
1013319; ATM
-
0744636; AGS
-
0821599; ATM
-
0349015) and the Office of Naval
Research (N00014
-
11
-
1
-
0783; N00014
-
10
-
1
-
0811; N00014
-
10
-
1
-
0200; N00014
-
08
-
1
-
0465). Sea Spray Research, Inc., provided oil for th
e operation of the smoke
generators. The authors gratefully acknowledge the crews of the CIRPAS Twin Otter
and the R/V
Point Sur
for their assistance during the field campaign, Tom Maggard
who revived and tirelessly maintained the smoke generators during t
he cruise, and
Spyros Pandis for providing the CCN spectrometer. The SOLEDAD 2012 field
measurements shown here were a collaboration of Scripps Institution of
Oceanography and Environment Canada.
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-
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