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<p class=3DMsoTitle style=3D'margin-top:3.0pt;margin-right:0in;margin-botto=
m:3.0pt;
margin-left:0in'><span style=3D'mso-bidi-font-size:11.0pt;font-family:"Time=
s New Roman"'>PROJECT
SUMMARY<o:p></o:p></span></p>

</div>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Observational and numerical modeling studies have greatly improved =
the
understanding of &#8220;classic&#8221; lake-effect snow storms and led to
improvements in forecasting them. In particular, research focused on the
mechanisms leading to lake-effect convective boundary layer growth and
mesoscale circulations, and how they differ from oceanic marine boundary
layers, has helped stimulate these improvements. In addition, results and t=
ools
from these earlier research studies have allowed for initial investigations=
 of
complex processes associated with &#8220;non-classic&#8221; lake-effect sto=
rms,
where lake-effect systems are modified by synoptic or sub-synoptic phenomen=
a or
upwind airmasses are modified by neighboring lakes. During our previous gra=
nt,
we reported on investigations of several non-classic<span
style=3D'mso-spacerun:yes'>&nbsp; </span>lake-effect systems including (1)
enhanced snowfall caused by seeding of lake-effect clouds by higher-level c=
loud
layers, (2) convective cloud bands that develop over a lake and extend acro=
ss
an intervening land mass to a second downwind lake, and (3) synoptic frontal
modifications resulting from the interaction with a large mid-latitude lake=
. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The proposed collaborative research project seeks to build on past
research results and address unanswered scientific questions using new
observations and numerical models to greatly broaden our understanding of
non-classic lake-effect systems and environments. Our specific research
objectives are to: (1) use unique observations from the GLICAF project to
understand and quantify the relationship of surface fluxes to heterogeneous
pack ice concentrations, (2) use case-study, climatic, and numerical model =
simulations
to understand the structure of multiple-lake bands and the influence of
environmental parameters on their development and evolution, (3) quantify t=
he
influence of environmental conditions on cold frontal structure and evoluti=
on
as synoptic fronts interact with lake-effect systems, (4) use Doppler radar
measurements, accompanied by atmospheric and environmental datasets to
determine the favorable conditions and the organization of mesoscale snow
events associated with lake-effect systems over small mid-latitude lakes, a=
nd
(5) examine cloud and ice spectrum characteristics, as well as radiative fl=
ux
profiles, across a range of lake-effect systems. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Results of this research will give valuable insight into complex
processes that often complicate winter forecasting of mesoscale phenomena
common to the <st1:place w:st=3D"on">Great Lakes</st1:place> region. These
results will be communicated to the meteorological community through journal
and conference articles and to the operational community through regional
workshops and presentations at National Weather Service offices. Based on o=
ur
experiences with previous grants, such workshops and presentations are
beneficial to the forecasting community. In this way, the improved
understanding gained from the proposed research will benefit society as a
result of improved forecasts of lake-effect phenomena. Results of the propo=
sed
studies will provide insights which can impact work on atmospheric response=
 to
heterogeneous surfaces, air-ice-sea interactions, and other areas beyond
lake-effect snow storms. In addition, the next generation of forecasters and
scientists will benefit through a wide range of graduate and undergraduate
educational and training activities. Results will be incorporated into
classroom lessons for both atmospheric science majors and non-majors</span>=
<span
style=3D'font-size:11.0pt;mso-bidi-font-size:12.0pt'>.<o:p></o:p></span></p>

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Times New Roman";
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</span>

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<p class=3DMsoTitle style=3D'margin-top:3.0pt;margin-right:0in;margin-botto=
m:3.0pt;
margin-left:0in;border:none;mso-border-bottom-alt:solid windowtext .5pt;
padding:0in;mso-padding-alt:0in 0in 2.0pt 0in'><span style=3D'mso-bidi-font=
-size:
11.0pt;font-family:"Times New Roman"'>RESULTS FROM PRIOR NSF SUPPORT<o:p></=
o:p></span></p>

</div>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'><o:=
p>&nbsp;</o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>NSF=
 ATM
02-02305 </span></b><span style=3D'font-size:11.0pt'>(Kristovich and Laird)=
 <i>Collaborative
Research: Investigations of Non-Classic Lake-Effect Boundary Layer Processe=
s</i>,
06/02 &#8211; 05/05. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>NSF=
 ATM
02-02160</span></b><span style=3D'font-size:11.0pt'> (Hjelmfelt) <i>Collabo=
rative
Research: Investigations of Non-Classic Lake-Effect Boundary Layer Processe=
s</i>,
06/02 &#8211; 05/05.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><span style=3D'font-size:11.0pt'><o:p>&=
nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>Des=
cription
of Results</span></b><span style=3D'font-size:11.0pt'>: <o:p></o:p></span><=
/p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Research described in the current proposal extends and builds on
scientific findings from our previous collaborative grants. The primary
objectives of these grants were to: (1) understand the thermodynamic and
microphysical structure of a lake-effect boundary layer undergoing seeding =
by
snow from higher cloud decks, (2) determine the effects of Lake Michigan on=
 a
cold-frontal passage, (3) examine the frequency and locations of lake-effect
cloud bands extending from one Great Lake to another, and (4) understand the
development and evolution of mesoscale vortices and other inhomogeneities a=
long
snowbands. Results of these investigations are summarized below.<o:p></o:p>=
</span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Rawinsonde, aircraft, and operational radar data collected during t=
he
Lake-Induced Convection Experiment (Lake-ICE, Kristovich et al. 2000), and
numerical model simulations were utilized to understand interactions between
the lake-effect convective boundary layer and higher-level precipitation ba=
nds
generated by a cyclone over the eastern Great Lakes on 5 December 1997. Des=
pite
weak surface thermal forcing, the event produced intense lake-enhanced
snowfall. Schroeder (2002) and Schroeder et al. (2003) found marked increas=
es
in snowfall rates and broadening of the snow particle spectra in regions of
seeding, relative to non-seeded regions. Convective boundary layer growth
across <st1:place w:st=3D"on">Lake Michigan</st1:place> was considerably mo=
re
rapid than in previous studies of lake-effect storms without nearby cyclone=
s,
with deepest boundary layers in regions of seeding. Fitzpatrick (2004) and
Fitzpatrick et al. (2004) reported on MM5 model simulations of this case. T=
hese
simulations reproduced observed interactions between the overlying
precipitating cloud deck and the lake-effect boundary layer. Simulations sh=
owed
that lake-effect clouds were deeper and precipitation amounts were greater =
in
areas with seeding. Simulations with no seeding produced smaller precipitat=
ion
amounts. Those with <st1:place w:st=3D"on">Lake Michigan</st1:place> removed
(synoptic only) produced much smaller amounts. Two manuscripts describing o=
ur
findings are nearing completion for submission to scientific journals.<o:p>=
</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Lake-ICE observations and MM5 model simulations were used by Dreher
(2004) and Dreher et al. (2004a, b) to examine the influence of the <st1:pl=
ace
w:st=3D"on">Great Lakes</st1:place> on the cold frontal snow band of 10 Jan=
uary
1998. A weak area of precipitation was associated with an arctic front prio=
r to
moving across <st1:place w:st=3D"on">Lake Michigan</st1:place>. As the front
crossed the lake, precipitation greatly increased in spatial coverage. A
comparison of with-lake and without-lake simulations revealed that <st1:pla=
ce
w:st=3D"on">Lake Michigan</st1:place> had a substantial impact on the
synoptic-scale front. The lake slowed the progress of the arctic air and
altered the local wind field. In addition, <st1:place w:st=3D"on">Lake Mich=
igan</st1:place>
influences resulted in a deeper, broader frontal zone, increased vertical
velocities, and increased depth of frontal precipitation fields. <i
style=3D'mso-bidi-font-style:normal'>The dramatic change in frontal structu=
re and
motion in this case, as well as the sensitivity of these changes to surface
conditions, indicate that additional investigations are critical to fully
understand these processes and their relationship with environmental condit=
ions.</i><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Cloud bands stretching between at least two of the <st1:place w:st=
=3D"on">Great
 Lakes</st1:place> are known to be important complicating factors when
developing forecasts in the region and can often result in intense unexpect=
ed
precipitation events. Rodriguez (2003) and Hjelmfelt et al. (2004) describe
observational and modeling efforts to understand these lake-to-lake (L2L)
bands. The observational study (Rodriguez 2003) examined the frequency and
locations of L2L bands over the <st1:place w:st=3D"on">Great Lakes</st1:pla=
ce>.
Results showed that L2L bands can extend from any of the <st1:place w:st=3D=
"on">Great
 Lakes</st1:place> up to three days per winter month. A modeling study
examining a L2L snow band extending from southern Lake Superior to northern=
 <st1:place
w:st=3D"on">Lake Michigan</st1:place> on 16 January 2000 was described in
Hjelmfelt et al. (2004). Simulations with and without Lake Superior indicat=
ed
that the warm cloudy boundary layer over Lake Superior crossed the Upper
Peninsula of Michigan and arrived at the northern shore of Lake Michigan
warmer, moister, and deeper than without Lake Superior. This modification
allowed rapid boundary layer development, leading to initiation and
intensification of clouds and precipitation over <st1:place w:st=3D"on">Lake
 Michigan</st1:place>. Differences in boundary layer depth, vertical
velocities, and cloud amounts decreased as air passed further over <st1:pla=
ce
w:st=3D"on">Lake Michigan</st1:place>. However, all values remained higher =
across
the lake for the case with <st1:place w:st=3D"on">Lake Superior</st1:place>
included in the simulation.&nbsp; <i>Since all of the <st1:place w:st=3D"on=
">Great
 Lakes</st1:place> are impacted by L2L snowbands, it is important that
additional studies be performed to better understand the environmental
conditions governing their initiation, structure, and evolution. Such studi=
es
must examine interactions between L2L bands and the boundary layer over the
downwind lake.</i><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>As part of our effort to understand mesoscale circulations along
lake-effect bands, Grim et al. (2004) conducted a detailed case study of a =
line
of small-scale lake-effect vortices. These vortices developed along an inte=
nse
lake-effect snow band over the eastern portions of <st1:place w:st=3D"on">L=
ake
 Michigan</st1:place> on 14 January 2003. Measurements collected by the NWS
Grand Rapids, MI, WSR-88D indicated that the vortices had lifetimes of 2
&#8211; 5 hours, and led to significant structural variations along the snow
band. Measured reflectivities were as high as 35 dBz in the &#8220;braid&#8=
221;
around each vortex and as low as 5 dBz in the &#8220;eye&#8221; regions. The
characteristics of the vortices and the environmental conditions in which t=
hey
developed were similar to those reported by Schoenberger (1986); the only o=
ther
study to provide a quantitative description of small-scale lake-effect vort=
ices.
In both cases, multiple small-scale vortices developed along a shoreline sn=
ow
band associated with a land-breeze front propagating westward into an area =
of
horizontal convective rolls over <st1:place w:st=3D"on">Lake Michigan</st1:=
place>.
Our findings suggest that the production of vertical vorticity by upward
tilting of rolls at the leading edge of the land-breeze was the likely caus=
e of
vortex initiation. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>While the scientific community has gained a substantial understandi=
ng
of lake-effect systems, virtually all research has been based on measuremen=
ts
or model simulations with open-water (i.e., ice free) conditions over the
lakes. The Great Lakes Ice Cover &#8211; Atmospheric Flux (GLICAF) field
project was conducted in February 2004 over Lake Erie, to collect unparalle=
led
new field data to enable a better understanding of surface heat exchange
processes that occur over pack ice fields. GLICAF employed the <st1:place
w:st=3D"on"><st1:PlaceType w:st=3D"on">University</st1:PlaceType> of <st1:P=
laceName
 w:st=3D"on">Wyoming King Air</st1:PlaceName></st1:place> aircraft equipped=
 to
quantify the pack ice concentration (percent of unit area of lake covered by
ice) and near-simultaneous in-situ measurements of turbulent heat exchanges=
 in
the atmospheric boundary layer. A total of six flights were conducted.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>Initial findings of the 26 Februar=
y 2004
case (Gerbush et al. 2005) suggest a surprising amount of spatial variabili=
ty
in state and dynamic characteristics of the boundary layer over Lake Erie, =
as
well as clear relationships between lake surface conditions (ice cover and
surface temperatures), magnitudes of surface fluxes, and thermodynamic
properties of the overlying air. <i style=3D'mso-bidi-font-style:normal'>Fu=
rther
investigation of the GLICAF dataset is a major component of the proposed
research.</i> <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Additional studies carried out with funding from these grants inclu=
de
model simulations of lake-effect boundary layer growth and mesoscale
circulations across Lake Michigan (Hjelmfelt et al. 2003), documentation of=
 the
diurnal evolution of lake-effect precipitation (Kristovich and Spinar 2004)=
, an
examination of the effect of regional-scale environmental conditions on
lake-effect mesoscale response (Laird et al. 2003), and comparison of ideal=
ized
model results with a large database of observed lake-effect events (Laird a=
nd
Kristovich 2004). <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><span style=3D'font-size:11.0pt'><o:p>&=
nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>Jou=
rnal,
Theses, and Scientific Conference Publications</span></b><span
style=3D'font-size:11.0pt'>:<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>During the past two years, research under these grants has resulted=
 in
4 journal articles, 2 Masters Theses, and 13 conference papers. Additional
journal articles and theses are in preparation.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><i style=3D'mso-bidi-font-style=
:normal'><u><span
style=3D'font-size:11.0pt;font-family:"Times New Roman"'>Journal Articles</=
span></u></i><span
style=3D'font-size:11.0pt;font-family:"Times New Roman"'>:<o:p></o:p></span=
></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Grim, Laird, and Kristovich, 2004: Mesoscale
vortices embedded within a lake-effect shoreline band. <i style=3D'mso-bidi=
-font-style:
normal'>Mon. Wea. Rev</i>., <b style=3D'mso-bidi-font-weight:normal'>132</b=
>,
2269-2274.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Laird, Walsh, and Kristovich, 2003: Model
simulations examining the relationship of lake-effect morphology to lake sh=
ape,
wind direction, and wind speed. <i style=3D'mso-bidi-font-style:normal'>Mon=
. Wea.
Rev</i>., <b style=3D'mso-bidi-font-weight:normal'>131</b>, 2101-2111.<o:p>=
</o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Laird and Kristovich, 2004: Comparison of ob=
servations
with idealized model results for a method to resolve winter lake-effect
mesoscale morphology. <i style=3D'mso-bidi-font-style:normal'>Mon. Wea. Rev=
</i>.,
<b style=3D'mso-bidi-font-weight:normal'>132</b>, 1093-1103.<o:p></o:p></sp=
an></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Kristovich and Spinar, 2004: Diurnal variati=
ons
in lake-effect precipitation near the western <st1:place w:st=3D"on">Great =
Lakes</st1:place>.
<i style=3D'mso-bidi-font-style:normal'>J. Hydrometeorology</i>, in press.<=
o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><i style=3D'mso-bidi-font-style=
:normal'><u><span
style=3D'font-size:11.0pt;font-family:"Times New Roman"'>Graduate Theses</s=
pan></u></i><span
style=3D'font-size:11.0pt;font-family:"Times New Roman"'>:<o:p></o:p></span=
></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Dreher, 2004: <i style=3D'mso-bidi-font-styl=
e:
normal'>The Influence of <st1:place w:st=3D"on">Lake Michigan</st1:place> o=
n a
Wintertime Cold Front</i>. M. S. Thesis, Department of Atmospheric Sciences=
, <st1:State
w:st=3D"on">South Dakota</st1:State> <st1:place w:st=3D"on"><st1:PlaceType =
w:st=3D"on">School</st1:PlaceType>
 of <st1:PlaceName w:st=3D"on">Mines</st1:PlaceName></st1:place> and Techno=
logy,
58 pp.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Fitzpatrick, 2004: <i style=3D'mso-bidi-font=
-style:
normal'>Numerical Simulations of Interactions Between Lake-effect Snow and a
Precipitating Synoptic System</i>. M. S. Thesis, Department of Atmospheric
Sciences, <st1:State w:st=3D"on">South Dakota</st1:State> <st1:place w:st=
=3D"on"><st1:PlaceType
 w:st=3D"on">School</st1:PlaceType> of <st1:PlaceName w:st=3D"on">Mines</st=
1:PlaceName></st1:place>
and Technology, 80 pp.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><i style=3D'mso-bidi-font-style=
:normal'><u><span
style=3D'font-size:11.0pt;font-family:"Times New Roman"'>Conference Papers =
and
Presentations</span></u></i><span style=3D'font-size:11.0pt;font-family:"Ti=
mes New Roman"'>:<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Gerbush, Kristovich, and Laird, 2005: <a
href=3D"http://ams.confex.com/ams/Annual2005/techprogram/paper_87628.htm"><=
span
style=3D'color:windowtext;text-decoration:none;text-underline:none'>Surface=
 Heat
Fluxes over Lake Erie Pack Ice Fields</span></a>. Preprints, <i>8th Conf. on
Polar Meteor. and Ocean</i>., Amer. Meteor. Soc., P3.15, in press.<o:p></o:=
p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Dreher, Hjelmfelt, Capehart, and Kristovich,
2004a: The influence of <st1:place w:st=3D"on">Lake Michigan</st1:place> on=
 a
wintertime cold front. <i style=3D'mso-bidi-font-style:normal'>Conf. Numeri=
cal
Weather Prediction</i>, AMS. P1.22, 12pp.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Dreher, Fitzpatrick, Hjelmfelt, Capehart,
Kristovich, and Schroeder, 2004b: Interactions of the winter lake-effect bo=
undary
layer with synoptic systems. <i style=3D'mso-bidi-font-style:normal'>Conf. =
on
Boundary Layers and Turb.</i>, AMS., 11.7, 11pp.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Fitzpatrick, Hjelmfelt, Capehart, and
Kristovich, 2004: Numerically simulated interactions between a precipitating
synoptic system and lake-effect snowbands over <st1:place w:st=3D"on">Lake =
Michigan</st1:place>.
<i style=3D'mso-bidi-font-style:normal'>Conf. Numerical Weather Prediction<=
/i>,
AMS. P2.16, 5pp.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Hjelmfelt, Capehart, and Kristovich, 2003:
Numerical simulation of convective evolution across <st1:place w:st=3D"on">=
Lake
 Michigan</st1:place> during a widespread lake-effect snow event. <i
style=3D'mso-bidi-font-style:normal'>10<sup>th</sup> Conf. on Mesoscale Pro=
cesses</i>,
AMS.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Hjelmfelt, Rodriguez, Kristovich and Hoevet,
2004: Influences of upwind lakes on wintertime lake-effect. <i
style=3D'mso-bidi-font-style:normal'>Conf. on Boundary Layers and Turb.</i>=
, AMS,
P3.3, 7pp.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Kristovich, Schroeder, Laird, and Hjelmfelt,
2003: Lake-ICE: A look inside lake-effect and lake-enhanced snow storms. <i
style=3D'mso-bidi-font-style:normal'>Midwest Severe and Hazardous Weather C=
onf.,</i>
<st1:place w:st=3D"on">Central Illinois</st1:place> AMS.<o:p></o:p></span><=
/p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Kristovich and Spinar, 2004: Observations of=
 the
diurnal evolution of lake-effect precipitation occurrence. <i style=3D'mso-=
bidi-font-style:
normal'>Conf. Applied Climatology</i>, AMS.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Kristovich, Laird, and Gerbush, 2004: Field
observations of the influence of pack ice cover on surface heat fluxes. <i
style=3D'mso-bidi-font-style:normal'>Conf. on Boundary Layers and Turb.</i>=
, AMS,
11.8, *pp.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Laird, 2003: Simulations examining the influ=
ence
of wind shear on the coherent mesoscale structure of intense lake-effect sn=
ow
bands. <i style=3D'mso-bidi-font-style:normal'>10<sup>th</sup> Conf. on Mes=
oscale
Processes</i>, AMS.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Laird and Kristovich, 2003: Determining what
type of lake-effect snowstorm will occur and who will get the snow. <i
style=3D'mso-bidi-font-style:normal'>Midwest Severe and Hazardous Weather C=
onf.,</i>
<st1:place w:st=3D"on">Central Illinois</st1:place> AMS.<o:p></o:p></span><=
/p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Laird and Kristovich, 2004: Utilizing ideali=
zed
mesoscale model simulations to aid the prediction of lake-effect snowstorms=
. <i
style=3D'mso-bidi-font-style:normal'>Conf</i>. <i style=3D'mso-bidi-font-st=
yle:
normal'>Weather Analysis. and Forecasting</i>. AMS.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Laird, Kristovich, Gerbush, Jackman, Kruk,
Rodriguez, and Spinar, 2004: The Great Lakes Ice Cover &#8211; Atmospheric =
Flux
(GLICAF) project: Overview and initial analyses. <i style=3D'mso-bidi-font-=
style:
normal'>Int. Assoc. of Great Lakes Res. Conf. 2004</i>, <st1:place w:st=3D"=
on"><st1:City
 w:st=3D"on">Waterloo</st1:City>, <st1:State w:st=3D"on">ON</st1:State></st=
1:place>
(Presentation only)<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Rodriguez, 2004: Frequency of and environmen=
tal
conditions associated with lake-to-lake snow bands in the Great Lakes regio=
n of
<st1:place w:st=3D"on">North America</st1:place>. <i>American Association of
Geographers Annual Meeting</i>, <st1:place w:st=3D"on"><st1:City w:st=3D"on=
">Washington</st1:City>,
 <st1:State w:st=3D"on">D.C.</st1:State></st1:place> (Presentation only)<o:=
p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.25in;line-height:normal'><span style=3D'font-size:11.0pt;
font-family:"Times New Roman"'>Schroeder, Kristovich, and Hjelmfelt, 2003:
Mesoscale and microscale field observations of a lake-enhanced snowstorm. <i
style=3D'mso-bidi-font-style:normal'>10<sup>th</sup> Conf. on Mesoscale Pro=
cesses</i>,
AMS.<o:p></o:p></span></p>

<p class=3DReferencePara style=3D'margin-top:3.0pt;margin-right:0in;margin-=
bottom:
3.0pt;margin-left:.9in;text-indent:-.7in;line-height:normal'><span
style=3D'font-family:"Times New Roman"'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>Rel=
ation
of previous to proposed work:</span></b><span style=3D'font-size:11.0pt'><o=
:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The results from our earlier research provide important aspects of
understanding non-classic lake-effect storms. Experience gained from these
efforts has given us valuable insight into approaches to address more compl=
ex
scientific issues, such as topics discussed in the current proposal. In this
way, the proposed research expands upon the work carried out under the prev=
ious
grants with the use of new, unprecedented observations and state-of-the-art
mesoscale numerical models. <o:p></o:p></span></p>

<span style=3D'font-size:11.0pt;font-family:"Times New Roman";mso-fareast-f=
ont-family:
"Times New Roman";mso-ansi-language:EN-US;mso-fareast-language:EN-US;
mso-bidi-language:AR-SA'><br clear=3Dall style=3D'mso-special-character:lin=
e-break;
mso-column-break-before:always'>
</span>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><o:p>&nbsp;</o:p></span></p>

<div style=3D'mso-element:para-border-div;border:none;border-bottom:solid w=
indowtext 1.0pt;
mso-border-bottom-alt:solid windowtext .5pt;padding:0in 0in 1.0pt 0in'>

<p class=3DMsoNormal align=3Dcenter style=3D'margin-top:3.0pt;margin-right:=
0in;
margin-bottom:3.0pt;margin-left:0in;text-align:center;border:none;mso-borde=
r-bottom-alt:
solid windowtext .5pt;padding:0in;mso-padding-alt:0in 0in 1.0pt 0in'><b><sp=
an
style=3D'font-size:11.0pt'>PROJECT DESCRIPTION<o:p></o:p></span></b></p>

</div>

<p class=3DMsoBodyText align=3Dcenter style=3D'margin-top:3.0pt;margin-righ=
t:0in;
margin-bottom:3.0pt;margin-left:0in;text-align:center'><b><span
style=3D'font-size:11.0pt'>Collaborative Research: Effects of Non-Uniform S=
urface
Conditions on Lake-Effect Systems<o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>1.
Introduction</span></b><span style=3D'font-size:11.0pt'><o:p></o:p></span><=
/p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><span style=3D'mso-spacerun:yes'>&nbsp;</span>Collaborative research
conducted by the Principal Investigators over the last few years, and their
shared contribution to the Lake-Induced Convection Experiment (Lake-ICE), h=
as
led to significant advancements in the understanding of lake-effect snow
storms. Much of this work has been on &#8220;classic&#8221; lake-effect sto=
rms,
where development of clouds and precipitation is directly associated with an
individual lake. By building on techniques and concepts from our earlier
investigations of classic lake-effect storms, research has expanded to incl=
ude
case studies of &#8220;non-classic&#8221; lake-effect storms, where lake-ef=
fect
processes are complicated by the influences of nearby synoptic storms or up=
wind
lakes. Despite advances from our research group and others, the continued n=
eed
for research on lake-effect snow was highlighted in the recently completed
United States Weather Research Program (USWRP) Implementation Plan for Cool
Season Quantitative Precipitation Forecasting (QPF, Rauber and Ralph 2004).
&#8220;Mesoscale boundary layer forcing, particularly orographic and
lake-effects&#8221; was identified as one of five key research areas needed=
 to
improve short-term QPF (Rauber and Ralph 2004). A major scientific issue th=
at
has not been addressed by nearly all previous lake-effect studies is the
response and interaction of the over-lake boundary layer to inhomogeneous l=
ake
surface conditions (such as ice cover and horizontal gradients in lake-surf=
ace
temperature). This proposal seeks to advance the scientific understanding of
important, complex lake-effect processes including the influences of surface
ice on lake-effect boundary layer processes, the structure and evolution of
convective bands extending from one lake to another, interactions between
relatively-warm lakes and frontal systems over a wide range of environmental
conditions, the environments favorable for lake-effect processes and
circulations over small lakes, and the influence of microphysical and radia=
tion
properties on lake-effect systems. Innovative new observations from the Gre=
at
Lakes Ice Cover &#8211; Atmospheric Flux (GLICAF) project, in addition to
Doppler radar, climatic, satellite, and Lake-ICE project datasets, and
state-of-the-art numerical mesoscale models (MM5 and WRF) will be employed =
to
address the scientific objectives of the proposed research.<o:p></o:p></spa=
n></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>2.
Background and Justification<o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>2.1=
 <st1:place
w:st=3D"on">Great Lakes</st1:place> Ice Cover &#8211; Atmospheric Flux (GLI=
CAF)
experiment </span></b><span style=3D'font-size:11.0pt'><o:p></o:p></span></=
p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The development of extensive pack ice fields on the <st1:place w:st=
=3D"on">Great
 Lakes</st1:place> significantly influences lake-effect storms and the
intensification of extratropical cyclones, as well as the regional hydrolog=
ic
cycle and lake levels. The evolution of the ice fields and their impacts on=
 the
atmospheric boundary layer complicates weather forecasters&#8217; ability to
accurately predict late-season lake-effect snows. Experience indicates that
forecasts of significant lake-effect snowstorms can be erroneous due to the
influence of ice on the eastern Great Lakes (personal communications 2004, =
T.
Niziol of NWSFO-<st1:City w:st=3D"on">Buffalo</st1:City>, NY and R. LaPlant=
e of <st1:place
w:st=3D"on"><st1:City w:st=3D"on">NWSFO-Cleveland</st1:City>, <st1:State w:=
st=3D"on">OH</st1:State></st1:place>).
It is thought that part of the reason for these errors is inappropriate
representations of the influences of ice in mesoscale forecast models. It
should be noted that the USWRP also recognized the difficulty of modeling t=
hese
situations and the importance of the substantial spatial and temporal
variations in surface heat and moisture fluxes by non-uniform ice-water sur=
face
conditions and variable surface temperatures (Rauber and Ralph 2004). <o:p>=
</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Much work has been carried out on the influence of ice on surface-a=
ir
heat exchange processes in Arctic regions. The Surface Heat Budget of the
Arctic Ocean (SHEBA) experiment, for example, collected an extensive datase=
t on
oceanic, atmospheric, cryospheric, and biological interrelationships (Uttal=
 et
al. 2002). Observational and related numerical modeling studies associated =
with
<st1:country-region w:st=3D"on"><st1:place w:st=3D"on">SHEBA</st1:place></s=
t1:country-region>
have extensively examined the influence of leads on surface fluxes and
mesoscale circulations. Surface fluxes from leads have been found to play a
crucial role in the heat budget of the <st1:place w:st=3D"on">Arctic</st1:p=
lace>
(e.g., Pinto et al. 1995, Alam and Curry 1995, 1997, 1998). Estimates of he=
at
fluxes from leads depend critically on the size and orientation of the lead,
surface wind characteristics, stability, radiation processes, and ocean-air
temperature differences (e.g., Andreas 1980, Maslanik and Key 1995, Pinto et
al. 1995, Zulauf and Krueger 2003). In addition to SHEBA, other field proje=
cts
have focused on specific processes, such as differing parameterizations for
open and thin ice-covered leads (Semmler et al. 2004), effects of entrainme=
nt
and mixing on surface heat exchanges (e.g., Gultepe et al. 2003), and
atmospheric responses to the complex summertime arctic ocean, with melt pon=
ds,
open oceanic water, and permanent ice cover (e.g., Perovich et al. 2002,
Tjernstr&ouml;m and Mauritson 2004, Tjernstr&ouml;m 2004, Tjernstr&ouml;m et
al. 2004). Clearly, an extensive knowledge of convective boundary layers is
required for an understanding of atmosphere-ice-water interrelationships in
marine environments (Tjernstr&ouml;m and Mauritson 2004).<span
style=3D'mso-spacerun:yes'>&nbsp; </span>However, this knowledge has not be=
en
developed for the <st1:place w:st=3D"on">Great Lakes</st1:place>.<o:p></o:p=
></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Parameterizations for Arctic regions may not adequately describe
surface interchange processes over the <st1:place w:st=3D"on">Great Lakes</=
st1:place>.
Characteristics of wintertime ice on the Great Lakes are quite different th=
an generally
seen in <st1:place w:st=3D"on">Arctic Ocean</st1:place> regions. Ice on the=
 <st1:place
w:st=3D"on">Great Lakes</st1:place> tends to be transient, not as thick, and
spatially and temporally variable (e.g., Assel et al. 1985, 1996). The
transient nature of <st1:place w:st=3D"on">Great Lakes</st1:place> ice cover
makes long-range predictions difficult (Assel et al. 2004) and short-term
predictions challenging (e.g., Rauber and Ralph 2004). Additionally, many
investigations examining surface exchange processes over Arctic ice have
occurred under considerably different environmental conditions than often o=
bserved
in the <st1:place w:st=3D"on">Great Lakes</st1:place> region. For example, =
the
Arctic environment tends to have larger differences between surface and air
temperatures over leads, stronger surface winds, thicker and less transient=
 ice
fields, stronger near-surface static stability, and larger surface albedos.=
 <i>These
significant differences bring into question the appropriateness of applying
parameterizations developed for Arctic regions to the simulation of boundary
layer processes and lake-effect snow events over <st1:place w:st=3D"on">Gre=
at
 Lakes</st1:place> ice fields.</i> <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Recent findings by Laird and Kristovich (2004) suggest that ice cov=
er
in the Great Lakes can lead to a modification of lake-effect snowstorm
morphology and, contrary to conventional thinking, lake-effect cloud patter=
ns
have been observed under conditions with the <i>entire</i> lake covered by a
high concentration of pack ice (Laird and Kristovich 2004, personal
communication with R. LaPlante of NWSFO-Cleveland, OH). <span style=3D'mso-=
bidi-font-style:
italic'>Although currently unknown, i</span>t might be anticipated that sin=
ce
the distribution of ice tends to be more spatially variable in the <st1:pla=
ce
w:st=3D"on">Great Lakes</st1:place>, and surface heat fluxes from areas of =
open
water tend to be less, mechanical heat exchange processes may be more domin=
ant
over convective heat exchange processes than in Arctic regions (Andreas and
Cash 1999).<i style=3D'mso-bidi-font-style:normal'> </i>Limitations in the
current understanding of the influences of variable pack ice concentration =
on
atmospheric modification were highlighted by the research and field studies
working group for the Implementation Plan of the USWRP Cool Season QPF (Rau=
ber and
Ralph 2004).<i style=3D'mso-bidi-font-style:normal'><o:p></o:p></i></span><=
/p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Past <st1:place w:st=3D"on">Great Lakes</st1:place> studies have ex=
amined
ice fields and atmospheric processes independently. <st1:place w:st=3D"on">=
Great
 Lakes</st1:place> ice research investigations have focused on ice extent,
thickness, roughness scales, and dynamics (e.g., Bolsenga 1992, Pilant and
Agarwal 1998). Several <st1:place w:st=3D"on">Great Lakes</st1:place> clima=
te
studies have examined the relationship between the extent of ice cover and
large-scale weather patterns (e.g., Rodionov et al. 2001, Assel et al. 1985,
1996); however, interactions between the atmospheric boundary layer and ice
fields with varied ice concentrations have not been investigated. Ice usual=
ly
begins to form on the <st1:place w:st=3D"on">Great Lakes</st1:place> in Dec=
ember
and January and reaches the maximum spatial coverage in February or early M=
arch
(Assel 1990). The operational forecasting community has found that current
numerical mesoscale models have had difficulty predicting winter weather ev=
ents
when widespread ice cover is present on the <st1:place w:st=3D"on">Great La=
kes</st1:place>.
Many forecast modeling systems, such as the Eta and GFS models, currently
designate each lake grid box as water or ice, but not mixed. Any
water-designated grid box with less than 55% ice coverage is considered
ice-free. For 55% ice coverage or greater, the full grid box is considered
ice-covered with a constant thickness of 3 meters. <i style=3D'mso-bidi-fon=
t-style:
normal'>This simplified treatment of ice cover presents difficulties for
forecasting winter weather in the <st1:place w:st=3D"on">Great Lakes</st1:p=
lace>
region and underscores the need for improved understanding of
atmosphere-ice-lake system interactions. </i><span style=3D'mso-bidi-font-s=
tyle:
italic'>Proposed analyses of GLICAF observations, and associated numerical
modeling results, will provide a better understanding of, and parameterizat=
ions
for, <st1:place w:st=3D"on">Great Lakes</st1:place> pack ice influences.</s=
pan><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>2.2
Lake-to-lake interactions<o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Lake-effect systems that develop over individual <st1:place w:st=3D=
"on">Great
 Lakes</st1:place> are generally not isolated from the influences of
neighboring lakes. These interactions can occur across a range of spatial a=
nd
temporal scales and the level of interaction can be influenced by both phys=
ical
and dynamical processes. An interaction between <st1:place w:st=3D"on">Great
 Lakes</st1:place> regional- (meso-alpha) and individual-lake- (meso-beta)
scales often produces changes in the intensity and location of precipitation
and atmospheric circulations (e.g., Sousounis and Fritsch 1994, Sousounis a=
nd
Mann 2000, Mann et al. 2002). Direct interactions between an upwind lake and
downwind lakes can result in complex boundary layer structure and intense
meso-beta-scale snow bands allowing snowfall to extend great distances from=
 the
original convective source region. Direct influences of upwind lakes on
lake-effect systems over downwind lakes, hereafter referred to as lake-to-l=
ake
(L2L) influences, have proven to be &#8220;<i>a particularly difficult fore=
cast
problem</i>&#8221; (Niziol et al. 1995), and are thus of importance to many
communities in the region. <span style=3D'mso-bidi-font-style:italic'><o:p>=
</o:p></span></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Understanding of the influences of environmental conditions on L2L
interactions has been limited and based on only a few events examined by
previous investigations. Several processes have been hypothesized as import=
ant
to L2L interactions: 1) downwind propagation of heat and moisture plumes (e=
.g.,
Niziol <i>et al</i>. 1995, Ballentine <i>et al</i>. 1998), often reaching t=
he
downwind lake as an elevated mixed layer (Agee and Gilbert 1989, Chang and
Braham 1991, Mann 1999, Rose 2000), 2)&nbsp;extension of lake-induced<span
style=3D'mso-spacerun:yes'>&nbsp; </span>circulations to a downwind lake (e=
.g.,
Niziol <i>et al</i>. 1995, Sousounis and Mann 2000), 3) long wavelength gra=
vity
waves initiated by the upwind lake (Yuen and Young 1986), and 4)&nbsp;inter=
nal
microphysical and radiation processes sustaining over-land structural coher=
ence
(e.g., Byrd <i>et al</i>. 1995). In a numerical modeling study, Rose (2000)
showed the first two processes to be most important in one L2L case. An
investigation of important processes over a wide range of environmental
conditions has not been reported. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The most extensively-explored process is advection of heat and mois=
ture
over the intervening land mass to a downwind lake. Satellite images often
clearly show examples of this advection as an extension of cloud bands from=
 an
upwind to a downwind lake (Byrd et al. 1995, Niziol et al. 1995).<span
style=3D'color:blue'> </span>Our group has developed a preliminary climatol=
ogy of
L2L cloud bands over the <st1:place w:st=3D"on">Great Lakes</st1:place> usi=
ng
five years of satellite observations. The results suggest that L2L cloud ba=
nds
originate over, or impact, each of the <st1:place w:st=3D"on">Great Lakes</=
st1:place>
up to 10% of the October-March time period (Rodriguez 2003). Even if contin=
uous
cloud bands are not visible, studies have shown that heat and moisture
transport from the upwind lakes can decrease stability (Agee and Gilbert 19=
89,
Chang and Braham 1991) and increase moisture content over the downwind lake=
s.
Recent mesoscale model simulations carried out at South Dakota School of Mi=
nes
and Technology (Hjelmfelt et al. 2004) have illustrated the enhancement of
boundary layer and cloud development that occurs as the preconditioned air =
from
Lake Superior reaches Lake Michigan. This preconditioned air, in turn, would
allow for deeper convection, lower cloud bases, and provide a greater suppl=
y of
moisture for snow production (e.g., Byrd et al. 1995, Niziol et al. 1995, R=
ose
et al. 1998, Rose 2000, Ballentine et al. 1998, Nicosia et al. 1999, Sousou=
nis
and Mann 2000). <i>Investigations providing quantitative information about =
the
modification of the upwind airmasses needed for a significant impact on
downwind lake-effect storm development have not been reported.</i><o:p></o:=
p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Several studies have suggested that mesoscale circulations generated
over an upwind lake can contribute to organizing convection over a downwind
lake. Niziol et al. (1995) found that a L2L convergence zone could remain
coherent even though a cloud or precipitation band is no longer visible,
despite the destructive influences of atmospheric turbulence and viscosity =
on
extended cloud bands (e.g., Sch&auml;r and Smith 1993, Young and Sikora 200=
3,
Sikora and Halverson 2002). In some cases, these convergence bands may be
augmented by &#8220;pseudo-fronts&#8221; which develop near the ends of the
lakes due to differential heating between the lake and nearby land areas (e=
.g.,
Baker 1976, Evans and Wagenmaker 2000). In our research group, Rose et al. =
(1998)
and Rose (2000) performed model simulations of an intense lake-effect snow
event over Lake Erie and found that a convergence zone downstream of Lake
Michigan played a significant role in deepening the convective boundary lay=
er
and increasing clouds and snow over <st1:place w:st=3D"on">Lake Erie</st1:p=
lace>.
Additionally, Ballentine et al. (1998), in a discussion of the complex
influence of topography on L2L interactions, pointed out that specific
intervening topography may act to channel heat and moisture to the downwind
lake. <i style=3D'mso-bidi-font-style:normal'>The limited number of studies
addressing L2L interactions has not resulted in a thorough investigation wh=
ich
examines the influence of an array of factors on the coherence of L2L
convective circulations</i>. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The proposed research seeks to address these needs through the use =
of
observations and numerical models. Investigations will examine the
environmental conditions and cloud and radiation properties that govern the
continuity of L2L interactions across intervening land surfaces and their
resulting impact on the development of lake-effect systems over the downwind
lake.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>2.3
Lake-effect systems over small lakes </span></b><span style=3D'font-size:11=
.0pt'><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Past research studies investigating the development of mesoscale
circulations associated with lake-effect snowstorms have predominantly focu=
sed
on systems over large water bodies, such as the Great Lakes (e.g., Kristovi=
ch
and Steve 1995) and the Great Salt Lake (e.g., Steenburgh et al. 2000). Lake
effect snowfalls and mesoscale circulations associated with small lakes, wi=
th
fetches less than 40 km, have received less attention. Cairns et al. (2001)=
 and
Huggins et al. (2001) examined events over Lake Tahoe and <st1:PlaceName w:=
st=3D"on">Pyramid</st1:PlaceName>
<st1:PlaceType w:st=3D"on">Lake</st1:PlaceType> in <st1:State w:st=3D"on">N=
evada</st1:State>,
Wilken (1997) described an event over <st1:PlaceName w:st=3D"on">Bull</st1:=
PlaceName>
<st1:PlaceName w:st=3D"on">Shoals</st1:PlaceName> <st1:PlaceType w:st=3D"on=
">Lake</st1:PlaceType>
in <st1:State w:st=3D"on">Arkansas</st1:State>, and more recently Schultz e=
t al.
(2004) presented an event that produced lake-effect snow bands over several
small lakes in <st1:State w:st=3D"on">Oklahoma</st1:State>, <st1:State w:st=
=3D"on">Missouri</st1:State>,
<st1:State w:st=3D"on">Arkansas</st1:State>, and <st1:State w:st=3D"on"><st=
1:place
 w:st=3D"on">Kentucky</st1:place></st1:State>. While the spatial scale of t=
hese
systems is smaller than those that develop over larger lakes, Cairns et al.
(2001) showed that these small lake events have the ability to produce
considerable snowfalls (53 cm within a two-day period) and have a significa=
nt
impact on the general public. These studies, all conducted within the last 8
years, have only provided a limited examination of the necessary environmen=
tal
conditions associated with lake-effect systems over small lakes.<o:p></o:p>=
</span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><i><span
style=3D'font-size:11.0pt'>The frequency and intensity of small-lake events=
 and
the environmental conditions that favor their development have not been
systematically investigated.</span></i><span style=3D'font-size:11.0pt'> The
degree that the favorable conditions and the resulting mesoscale circulation
systems associated with small lakes are similar or different than their
large-lake counterparts is not known. While new understanding will be provi=
ded
by the proposed investigation of small lake events, the studies may also of=
fer
scientific insight into the processes and environments that exist near small
heterogeneous surfaces over large mid-latitude and Polar ice-covered water
bodies. In some cases, the physical processes associated with open-water ar=
eas
of small lakes during cold air outbreaks may be comparable with those linke=
d to
intense surface temperature and moisture gradients in the Great Lakes and <=
st1:place
w:st=3D"on">Polar regions</st1:place> (e.g., leads and polynyas). Segal and
Arritt (1992) suggested that non-classic mesoscale circulations caused by
surface heat flux gradients may exhibit a reduced intensity in many situati=
ons
because of a large imbalance of the spatial scales of the small areas provi=
ding
the surface forcing compared to the surrounding areas. Extreme events can s=
till
occur, however (Cairns et al. 2001). The comparative intensity of, and the
influence of environmental conditions on, lake-effect systems over small la=
kes
have not been investigated. Segal and Arritt (1992) concluded that an <i>em=
phasis
on observations was essential for further progress in quantification of
&#8220;real-world&#8221; mesoscale circulations associated with small regio=
ns
of intense surface heat flux gradients.</i><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The New York State (NYS) <st1:place w:st=3D"on">Finger Lakes</st1:p=
lace>
region is an ideal laboratory for investigating the environmental conditions
that lead to the development of lake-effect snow bands over small lakes and=
 the
intensity and structure of the associated mesoscale circulations. Cosgrove =
et
al. (1996) and Watson et al. (1998) conducted mesoscale model simulations to
examine three cases where snow bands were observed to have developed in the=
 NYS
Finger Lakes region. The results showed that the NYS Finger Lakes can great=
ly
influence snowfall in <st1:place w:st=3D"on">Central New York</st1:place> a=
nd
that the models were able to capture some of the mesoscale features of the =
snow
bands. Although NYS Finger Lakes snow bands can have a significant impact in
the vicinity of each lake, the morphology and evolution of these events is =
not
well known. The proposed research seeks to investigate lake-effect systems =
that
have developed in the NYS Finger Lakes region over the past decade to gain a
scientific understanding and quantify the frequency, intensity, and conditi=
ons
favorable for lake-effect systems associated with small lakes.<span
style=3D'color:#3366FF'><o:p></o:p></span></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>2.4
Lake-effect and synoptic front interactions </span></b><span style=3D'font-=
size:
11.0pt'><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Few studies have focused on the influence of the <st1:place w:st=3D=
"on">Great
 Lakes</st1:place> on larger-scale phenomena, despite recognition of their
influences on sub-synoptic phenomena such as frontal systems (Rauber and Ra=
lph
2004). Though the potential for lake-effect enhancement of synoptic scale
precipitation has long been recognized, most studies (e.g., Dewey 1979) have
excluded such situations in order to concentrate on better defined
&#8220;classic&#8221; lake-effect systems. Some studies that have made prog=
ress
on these issues include Kelly (1984), who suggested a measurable enhancement
of<span style=3D'mso-spacerun:yes'>&nbsp; </span>larger-scale snow falls do=
wnwind
of Lake Michigan, and Sousounis and Fritsch (1994) and their related series=
 of
studies, who looked at the aggregate effects of the Great Lakes on regional
weather and climate. Gallus and Segal (1999) studied changes in a shallow c=
old
front, with a strong temperature gradient, as it moved from north to south
across <st1:place w:st=3D"on">Lake Michigan</st1:place>. The case dealt wit=
h a
lake surface that was cooler than the atmospheric boundary layer. Gallus and
Segal (1999) indicated that two competing mechanisms are responsible for
modification of the movement and intensity of a surface cold front over a
lake.<span style=3D'mso-spacerun:yes'>&nbsp; </span>The first is through a =
change
in the frontal temperature gradient caused by changes in diabatic heating
between land and water. A second mechanism is through changes in surface
roughness between the lake and land.<span style=3D'mso-spacerun:yes'>&nbsp;
</span>Gallus and Segal (1999) found that the front accelerated and that the
frontal temperature gradient strengthened as it progressed across the smoot=
her
and cooler <st1:place w:st=3D"on">Lake Michigan</st1:place> surface.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>Recently, Dreher (2004) and Dreher=
 et al
(2004a, b) presented preliminary results of a study, conducted under our
current grants, of effects of Lake Michigan on a winter cold front observed
during the Lake-ICE field experiment. Our results indicate that the front m=
oved
more slowly over the lake than over adjacent land areas south of the lake a=
nd
precipitation was more widespread and intense downwind of the lake. Numeric=
al
sensitivity studies suggested that the enhanced mixing due to the warm lake
dominated over the effects of reduced surface friction to retard frontal
progress.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><span style=3D'mso-tab-count:1'>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; </sp=
an>Further
research is needed to understand cold season interactions between
synoptic-scale fronts and relatively warm lakes. <i>The frequency of frontal
crossings of each of the <st1:place w:st=3D"on">Great Lakes</st1:place> in
wintertime is not well documented, but must obviously occur with some
regularity.<span style=3D'mso-spacerun:yes'>&nbsp; </span>Impacts of lake-e=
ffect
interactions with fronts on frontal structure and precipitation are not well
understood.</i><span style=3D'mso-spacerun:yes'>&nbsp; </span>The focus of =
our
study will be to establish a climatology of potentially-lake-effected front=
al
crossings over the <st1:place w:st=3D"on">Great Lakes</st1:place>, and exam=
ine
impacts of the lakes on the frontal speed and precipitation characteristics=
 in
relation to environmental conditions and frontal properties. Examination of
physical processes involved will be carried out using both observational
analyses and numerical simulations.<span style=3D'color:blue'><o:p></o:p></=
span></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>2.5
Cloud, Precipitation, and Radiative Processes</span></b><span style=3D'font=
-size:
11.0pt'><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Cloud, precipitation, and radiation processes have important influe=
nces
on the structure of marine atmospheric boundary layers (e.g., Albrecht 1993,
Stevens et al. 1998, Boers and Melfi 1987, etc.). Model simulations of
lake-effect boundary layers indicate that latent heat release by cloud and
precipitation formation can affect both the magnitude of vertical motions a=
nd,
in some cases, mesoscale convective structures within the boundary layer. F=
or
example, numerical model results by Hjelmfelt and Braham (1983) and Cooper =
et
al. (2000) indicated that vertical motions doubled when latent heat release=
 was
included. The influence of latent heat release on mesoscale convective
organization appears to be highly dependent on environmental conditions.
Hjelmfelt (1990) found that latent heat release influences the initiation o=
f land
breezes and Rao and Agee (1996) found two-dimensional convective organizati=
ons
were more likely when precipitation was present. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><span style=3D'mso-spacerun:yes'>&nbsp;</span>Despite the importanc=
e of
cloud and precipitation processes identified by numerical models, documenta=
tion
of their properties in lake-effect boundary layers has lagged behind that of
other types of marine boundary layers. Indeed, this mirrors the suggestion =
by
the USWRP that field studies should provide ice microphysical observations
using aircraft (Rauber and Ralph 2004). Only a few studies have reported
results from aircraft-obtained microphysical data in lake-effect environmen=
ts.
Braham (1990) examined aircraft observations of near-surface snow particles=
 and
gave the range of observed spectral parameters. Kristovich and Braham (1998)
derived profiles of water contents and fluxes throughout the depth of the
lake-effect boundary layer. Several studies were devoted to estimating snow=
fall
rates over <st1:place w:st=3D"on">Lake Michigan</st1:place> (Braham et al. =
1992,
Braham and Dungey 1995). The large amount of microphysical data collected
during the Lake-ICE project has seen very limited use. Beard et al. (2004)
examined charges on cloud droplets to improve understanding of its influenc=
e on
droplet spectrum evolution, and Schroeder (2002) documented broadening of t=
he
snowfall spectra in lake-effect clouds in a case with natural cloud seeding
from higher-level clouds. Although Lake-ICE aircraft flights were designed,=
 in
part, to understand in-cloud microphysical processes, the robust <i>Lake-ICE
dataset has not been used to examine snow or cloud characteristics and their
relationship with convective structures in lake-effect boundary layers.</i>=
 In
addition, radiation processes have been shown to have a significant impact =
on
the heat budgets of internal lake-effect boundary layers (Chang and Braham
1991). Other studies speculated that radiation processes may play roles in
lake-to-lake band maintenance (Byrd et al. 1995), or in the diurnal evoluti=
on
of lake-effect precipitation rates (Kristovich and Spinar 2004). <i>Despite=
 the
suggested importance of these processes, however, the spatial and vertical
characteristics and variability of the radiation field in lake-effect bound=
ary
layers have not been investigated.</i><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>We propose to examine cloud and precipitation characteristics, their
relationship to convective motions in the boundary layer, and associated
radiative fluxes, in several lake-effect cases using data collected during
Lake-ICE. Initially, the proposed research will focus on comparing observat=
ions
taken on two &#8220;classic&#8221; lake-effect cases, lake-enhanced episode=
s,
and a nocturnal case. <o:p></o:p></span></p>

<p class=3DCellBody style=3D'margin-top:3.0pt;margin-right:0in;margin-botto=
m:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.
Research Proposal <o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.1
Research Objectives<span style=3D'mso-tab-count:1'>&nbsp;&nbsp;&nbsp;&nbsp;=
&nbsp;&nbsp;&nbsp;&nbsp; </span><o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The primary goals of the proposed research are to investigate the
following scientific issues:<b><o:p></o:p></b></span></p>

<ul style=3D'margin-top:0in' type=3Ddisc>
 <li class=3DMsoNormal style=3D'margin-top:3.0pt;margin-bottom:3.0pt;text-a=
lign:
     justify;mso-list:l4 level1 lfo3;tab-stops:list .5in'><b><i
     style=3D'mso-bidi-font-style:normal'><span style=3D'font-size:11.0pt'>=
Influence
     of lake ice cover on rates of surface heat fluxes<o:p></o:p></span></i=
></b></li>
</ul>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:.5in;text-align:justify'><i><span style=3D'font-size:11.0pt'>Our
proposed research seeks to use unique measurements from the</span></i><i
style=3D'mso-bidi-font-style:normal'><span style=3D'font-size:11.0pt;mso-bi=
di-font-weight:
bold'> GLICAF field study to understand the atmosphere-ice-lake surface
exchange processes and quantify the relationship between turbulent heat flu=
xes
and pack ice concentrations and arrangements.</span></i><span style=3D'font=
-size:
11.0pt'><o:p></o:p></span></p>

<ul style=3D'margin-top:0in' type=3Ddisc>
 <li class=3DMsoNormal style=3D'margin-top:3.0pt;margin-bottom:3.0pt;text-a=
lign:
     justify;mso-list:l4 level1 lfo3;tab-stops:list .5in'><st1:place w:st=
=3D"on"><b><i
      style=3D'mso-bidi-font-style:normal'><span style=3D'font-size:11.0pt'=
>Lake-to-lake</span></i></b></st1:place><b><i
     style=3D'mso-bidi-font-style:normal'><span style=3D'font-size:11.0pt'>
     interactions<o:p></o:p></span></i></b></li>
</ul>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:.5in;text-align:justify'><i><span style=3D'font-size:11.0pt'>Our
proposed research seeks to use case study and climatic analyses, and numeri=
cal
modeling simulations, to determine the evolution of the convective boundary
layer, as well as microphysical and dynamical characteristics of lake-to-la=
ke
convective bands.</span></i><span style=3D'font-size:11.0pt'><o:p></o:p></s=
pan></p>

<ul style=3D'margin-top:0in' type=3Ddisc>
 <li class=3DMsoNormal style=3D'margin-top:3.0pt;margin-bottom:3.0pt;text-a=
lign:
     justify;mso-list:l4 level1 lfo3;tab-stops:list .5in'><b><i
     style=3D'mso-bidi-font-style:normal'><span style=3D'font-size:11.0pt'>=
Lake-effect
     systems over small lakes<o:p></o:p></span></i></b></li>
</ul>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:.5in;text-align:justify'><i><span style=3D'font-size:11.0pt'>Our
proposed research seeks to use Doppler radar observations, accompanied by
atmospheric and environmental datasets to advance the understanding of
lake-effect mesoscale systems linked to small lakes by examining their
structure, frequency, and intensity and the environmental conditions leadin=
g to
their development.<o:p></o:p></span></i></p>

<ul style=3D'margin-top:0in' type=3Ddisc>
 <li class=3DMsoNormal style=3D'margin-top:3.0pt;margin-bottom:3.0pt;text-a=
lign:
     justify;mso-list:l4 level1 lfo3;tab-stops:list .5in'><b><i
     style=3D'mso-bidi-font-style:normal'><span style=3D'font-size:11.0pt'>=
Lake-effect
     and synoptic front interactions<o:p></o:p></span></i></b></li>
</ul>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:.5in;text-align:justify'><i><span style=3D'font-size:11.0pt'>Our
proposed research seeks to utilize observations and numerical model simulat=
ions
to quantify the influence of surface exchanges on the structure, evolution,=
 and
motion of frontal systems passing over the <st1:place w:st=3D"on">Great Lak=
es</st1:place>.
</span></i><span style=3D'font-size:11.0pt'><o:p></o:p></span></p>

<ul style=3D'margin-top:0in' type=3Ddisc>
 <li class=3DMsoNormal style=3D'margin-top:3.0pt;margin-bottom:3.0pt;text-a=
lign:
     justify;mso-list:l4 level1 lfo3;tab-stops:list .5in'><b><i
     style=3D'mso-bidi-font-style:normal'><span style=3D'font-size:11.0pt'>=
Lake-Effect
     cloud, precipitation, and radiative processes<span
     style=3D'mso-spacerun:yes'>&nbsp; </span><o:p></o:p></span></i></b></l=
i>
</ul>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:.5in;text-align:justify'><i><span style=3D'font-size:11.0pt'>Our
proposed research seeks to examine cloud and ice spectrum properties, as we=
ll
as radiative flux profile characteristics, and their relationship with
circulations in lake-effect and lake-enhanced boundary layers. </span></i><=
span
style=3D'font-size:11.0pt'><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.2
Observational and Numerical Modeling Resources<o:p></o:p></span></b></p>

<p class=3DMsoBodyTextIndent style=3D'margin-top:3.0pt;margin-right:0in;mar=
gin-bottom:
3.0pt;margin-left:.25in;text-indent:0in'><b><span style=3D'mso-bidi-font-si=
ze:
11.0pt'>3.2.1 GLICAF and Lake-ICE datasets<o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The proposed research will rely heavily on data collected during two
field projects led by the Principal Investigators of this proposal. The Gre=
at
Lakes Ice Cover &#8211; Atmospheric Flux (GLICAF) experiment, led by Dr. La=
ird,
was conducted over <st1:place w:st=3D"on">Lake Erie</st1:place> in February=
 2004.
Data collected by the <st1:place w:st=3D"on"><st1:PlaceType w:st=3D"on">Uni=
versity</st1:PlaceType>
 of <st1:PlaceName w:st=3D"on">Wyoming King Air</st1:PlaceName></st1:place>
aircraft provide an unprecedented opportunity to examine atmospheric respon=
ses
to pack-ice-covered lakes. Additional information on project goals and data=
sets
can be found at the project website; <a
href=3D"http://glicaf.atmos.uiuc.edu/glicaf-index.html">http://glicaf.atmos=
.uiuc.edu/glicaf-index.html</a>.
The Lake-Induced Convection Experiment (Lake-ICE), led by Dr. Kristovich,
collected a wide range of data on lake-effect processes ranging from
microphysical to meso-alpha scales. Much of the data collected during this
project remains unanalyzed. Details of the goals and datasets from Lake-ICE=
 are
described in Kristovich et al. (2000). Lake-ICE data will primarily be used=
 to
investigate lake-to-lake interactions and the influence of microphysical and
radiation processes on lake-effect storms. Drs. Kristovich and Laird have
extensive experience in analysis of measurements collected in lake-effect
environments and during these field projects<span
style=3D'mso-spacerun:yes'>&nbsp; </span>(see references and vitas). <o:p><=
/o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoBodyTextIndent style=3D'margin-top:3.0pt;margin-right:0in;mar=
gin-bottom:
3.0pt;margin-left:.25in;text-indent:0in'><b><span style=3D'mso-bidi-font-si=
ze:
11.0pt'>3.2.2 WSR-88D radar dataset <o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><!--[if gte vml 1]><v=
:shapetype
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</v:shapetype><v:shape id=3D"_x0000_s1091" type=3D"#_x0000_t202" style=3D'p=
osition:absolute;
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:172.8pt;
 text-indent:0;z-index:-2;mso-position-horizontal:left' wrapcoords=3D"-73 0=
 -73 21506 21600 21506 21600 0 -73 0"
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 <v:textbox style=3D'mso-next-textbox:#_x0000_s1091'>
  <![if !mso]>
  <table cellpadding=3D0 cellspacing=3D0 width=3D"100%">
   <tr>
    <td><![endif]>
    <div>
    <p class=3DMsoNormal><v:shapetype id=3D"_x0000_t75" coordsize=3D"21600,=
21600"
     o:spt=3D"75" o:preferrelative=3D"t" path=3D"m@4@5l@4@11@9@11@9@5xe" fi=
lled=3D"f"
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     <v:stroke joinstyle=3D"miter"/>
     <v:formulas>
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     <v:path o:extrusionok=3D"f" gradientshapeok=3D"t" o:connecttype=3D"rec=
t"/>
     <o:lock v:ext=3D"edit" aspectratio=3D"t"/>
    </v:shapetype><v:shape id=3D"_x0000_i1025" type=3D"#_x0000_t75" style=
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     height:140.25pt' o:ole=3D"">
     <v:imagedata src=3D"proposal_description_041202_files/image001.emz" o:=
title=3D""/>
    </v:shape><![if gte mso 9]><o:OLEObject Type=3D"Embed"
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tent"
     ObjectID=3D"_1225189503">
    </o:OLEObject>
   <![endif]></p>
    <p class=3DMsoNormal><span style=3D'font-size:11.0pt'>Fig. 1. Finger La=
kes
    region of <st1:place w:st=3D"on"><st1:PlaceName w:st=3D"on">New York</s=
t1:PlaceName>
     <st1:PlaceType w:st=3D"on">State</st1:PlaceType></st1:place>, showing =
KBGM
    radar coverage area.<o:p></o:p></span></p>
    </div>
    <![if !mso]></td>
   </tr>
  </table>
  <![endif]></v:textbox>
 <w:wrap type=3D"square"/>
</v:shape><![endif]--><![if !vml]><img width=3D304 height=3D234
src=3D"proposal_description_041202_files/image002.gif" align=3Dleft hspace=
=3D12
alt=3D"Text Box:  &#13;&#10;Fig. 1. Finger Lakes region of New York State, =
showing KBGM radar coverage area.&#13;&#10;"
v:shapes=3D"_x0000_s1091"><![endif]><span style=3D'font-size:11.0pt'>The pr=
oposed
investigations of lake-effect systems over small lakes and the interactions=
 of
synoptic fronts with lake-effect systems will utilize WSR-88D radar dataset=
s.
Lake-effect events in the New York State (NYS) Finger Lakes region will be
identified using radar reflectivity from all available 0.5&deg; elevation s=
cans
of the National Weather Service (NWS) WSR-88D radar located in <st1:place
w:st=3D"on"><st1:City w:st=3D"on">Binghamton</st1:City>, <st1:State w:st=3D=
"on">New
  York</st1:State></st1:place> (KBGM). The KBGM coverage in the targeted re=
gion
is shown in Figure 1. WSR-88D level-II radar data has been archived by KBGM
since September 1995. This provides a substantial radar data set to be exam=
ined
for this study (i.e., 10 years for the months October through March). The
reflectivity data generally has temporal resolution of every 6 (10) min when
the radar operated in precipitation (clear-air) mode and has a spatial
resolution of 1&deg; </span><span style=3D'font-size:11.0pt;font-family:Sym=
bol;
mso-ascii-font-family:"Times New Roman";mso-hansi-font-family:"Times New Ro=
man";
mso-char-type:symbol;mso-symbol-font-family:Symbol'><span style=3D'mso-char=
-type:
symbol;mso-symbol-font-family:Symbol'>&acute;</span></span><span
style=3D'font-size:11.0pt'> 1 km. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Investigations of the influences of lakes on synoptic fronts will
incorporate WSR-88D observations to examine both changes in precipitation r=
ates
associated with, and vertical structures of, frontal systems as they cross =
the
lakes. These investigations will use archived level II data from several si=
tes
around the <st1:place w:st=3D"on">Great Lakes</st1:place> region. Previous
investigations by Dreher (2004) and Dreher et al. (2004a,b) of synoptic fro=
ntal
modification by lake-effects showed the usefulness of these radar data. <o:=
p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The WSR-88D level-II data necessary for these investigations are fr=
eely
available through FTP transfer from the HDSS Access System at the <st1:place
w:st=3D"on"><st1:PlaceName w:st=3D"on">National</st1:PlaceName> <st1:PlaceN=
ame
 w:st=3D"on">Climatic</st1:PlaceName> <st1:PlaceName w:st=3D"on">Data</st1:=
PlaceName>
 <st1:PlaceType w:st=3D"on">Center</st1:PlaceType></st1:place>. Archived KB=
GM
Level-II data will be examined using the WSR-88D Algorithm Testing And Disp=
lay
System (WATADS), Integrated Data Viewer (IDV) software, or the recently
developed GRW88Level2 package from Gibson Ridge Software. Quantitative
investigations using reflectivity data will be performed with the <st1:place
w:st=3D"on"><st1:PlaceName w:st=3D"on">National</st1:PlaceName> <st1:PlaceT=
ype
 w:st=3D"on">Center</st1:PlaceType></st1:place> for Atmospheric Research PP=
I-MMM
radar display and analysis software and Geographic Information Systems (GIS)
software. All three PIs have extensive expertise in analysis of radar data,
including WSR-88D measurements, for investigations of lake-effect processes
(e.g., Laird et al. 2001, Kristovich et al. 2003, Grim et al. 2004).<span
style=3D'color:red'><o:p></o:p></span></span></p>

<p class=3DMsoBodyTextIndent style=3D'margin-top:3.0pt;margin-right:0in;mar=
gin-bottom:
3.0pt;margin-left:.25in;text-indent:0in'><b><span style=3D'mso-bidi-font-si=
ze:
11.0pt'>3.2.3 Numerical Models<o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Numerical simulations will employ well-established community models.
These are non&#8209;hydrostatic, cloud-resolving mesoscale models, which may
include detailed boundary layer and surface schemes, and thus are well suit=
ed
for the proposed studies. Dr. Hjelmfelt and his colleague Dr. Capehart have
experience with both the MM5 and ARPS models, and have used them for a vari=
ety
of studies including lake-effect simulations (see references and vitas). Bo=
th
also attended the Weather Research and Forecasting model (WRF) tutorial in =
June
2004 and are employing the model at South Dakota School of Mines and
Technology. WRF is an advanced mesoscale research and forecasting model bei=
ng
developed to be a next-generation national model by a national team involvi=
ng
the research and operational meteorological communities (additional informa=
tion
can be found at</span><span style=3D'font-size:10.0pt;font-family:"Courier =
New";
mso-bidi-font-family:"Times New Roman"'> </span><span class=3DMsoHyperlink>=
<span
style=3D'font-size:11.0pt'><a
href=3D"http://www.mmm.ucar.edu/wrf/users/user_main.html">http://www.mmm.uc=
ar.edu/wrf/users/user_main.html</a></span></span><span
style=3D'font-size:11.0pt'>).</span><span style=3D'font-size:10.0pt;font-fa=
mily:
"Courier New";mso-bidi-font-family:"Times New Roman"'> </span><span
style=3D'font-size:11.0pt'>As development continues, WRF will be used, as
appropriate. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
10.0pt;font-family:"Courier New";mso-bidi-font-family:"Times New Roman"'>&n=
bsp;</span><span
style=3D'font-size:11.0pt'>A major research activity at SDSMT has been the
coupling of ARPS and MM5 to a variety of advanced surface models to study t=
he
effects of surface processes (including snow processes and sub-grid scale
inhomogeneities) on local scale cloud and hydrologic processes (Capehart et=
 al.
2000, Wang et al. 2003).<span style=3D'mso-spacerun:yes'>&nbsp;
</span>Specifically, different approaches of aggregating sub-grid land-water
inhomogeneities to fine resolution NWP grid scales have been investigated
(Capehart et al. 2001a, b). The experience gained by these investigations is
important for our proposed research.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.3
Approach<o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.3=
.1
GLICAF Analyses and related Numerical Simulations</span></b><span
style=3D'font-size:11.0pt'><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><!--[if gte vml 1]><v=
:shape
 id=3D"_x0000_s1092" type=3D"#_x0000_t202" style=3D'position:absolute;left:=
0;
 text-align:left;margin-left:0;margin-top:69pt;width:4in;height:210pt;
 text-indent:0;z-index:5;mso-position-horizontal:left' stroked=3D"f">
 <v:textbox style=3D'mso-next-textbox:#_x0000_s1092'>
  <![if !mso]>
  <table cellpadding=3D0 cellspacing=3D0 width=3D"100%">
   <tr>
    <td><![endif]>
    <div>
    <p class=3DMsoNormal align=3Dcenter style=3D'text-align:center'><span
    style=3D'font-size:10.0pt'><v:shape id=3D"_x0000_i1026" type=3D"#_x0000=
_t75"
     style=3D'width:288.75pt;height:162pt'>
     <v:imagedata src=3D"proposal_description_041202_files/image003.wmz" o:=
title=3D"GLICAF flight plan"/>
    </v:shape></span><span class=3DmsoIns><ins cite=3D"mailto:laird"
    datetime=3D"2004-11-24T14:58"><o:p></o:p></ins></span></p>
    <p class=3DMsoNormal align=3Dcenter style=3D'text-align:center;text-ind=
ent:0in;
    mso-text-indent-alt:0in;mso-list:none;mso-list-ins:laird 20041124T1458'=
><span
    style=3D'font-size:10.0pt'><span class=3DmsoDel><del cite=3D"mailto:lai=
rd"
    datetime=3D"2004-11-24T14:58"><o:p>&nbsp;</o:p></del></span></span></p>
    <p class=3DMsoNormal style=3D'margin-left:.5in;text-indent:-.5in;mso-te=
xt-indent-alt:
    -.5in;mso-list:none;mso-list-ins:laird 20041124T1458'><span
    style=3D'font-size:11.0pt'>Fig. 2. GOES visible image of <st1:place w:s=
t=3D"on">Lake
     Erie</st1:place> ice field with flight plan for 27 February 2004.</spa=
n><span
    style=3D'font-size:10.0pt'><o:p></o:p></span></p>
    </div>
    <![if !mso]></td>
   </tr>
  </table>
  <![endif]></v:textbox>
 <w:wrap type=3D"square"/>
</v:shape><![endif]--><![if !vml]><img width=3D388 height=3D284
src=3D"proposal_description_041202_files/image004.gif" align=3Dleft hspace=
=3D12
alt=3D"Text Box:  &#13;&#10;&#13;&#10;Fig. 2. GOES visible image of Lake Er=
ie ice field with flight plan for 27 February 2004.&#13;&#10;"
v:shapes=3D"_x0000_s1092"><![endif]><span style=3D'font-size:11.0pt'>Spatia=
l and
temporal variations in atmospheric conditions and surface fluxes over Lake =
Erie
pack ice will be examined using data from the <st1:place w:st=3D"on"><st1:P=
laceType
 w:st=3D"on">University</st1:PlaceType> of <st1:PlaceName w:st=3D"on">Wyomi=
ng King
  Air</st1:PlaceName></st1:place> aircraft, collected during the recent GLI=
CAF
project (Gerbush et al. 2005). Additional observations taken by operational
agencies (NWS, NOAA, and<span style=3D'mso-spacerun:yes'>&nbsp;
</span>Environment Canada) will also be used. King Air research flights were
conducted over <st1:place w:st=3D"on">Lake Erie</st1:place> on six dates in
February 2004. A typical GLICAF flight plan is shown in Figure 2. Several
flight stacks were flown over the lake (bold lines), each consisting of thr=
ee
flight legs of 60-80 km length. Two sequential flight legs were flown at
approximately 50 m above the lake surface (minimum altitude allowed by flig=
ht
safety considerations), and the third was flown at approximately 500 m. The=
 two
low-altitude flight legs were conducted to maximize the sample of surface-l=
ayer
heat fluxes. The 500 m flight leg was conducted to obtain digital video
observations of ice cover<span style=3D'mso-spacerun:yes'>&nbsp;
</span>distribution near the locations of the two 50 m altitude flight legs.
Spiral soundings were conducted at the beginning and end of each flight sta=
ck
(circles in Fig. 2) to gain information on the vertical structure of the lo=
wer
atmosphere. More information on the GLICAF flights and goals can be found a=
t <a
href=3D"http://glicaf.atmos.uiuc.edu/glicaf-index.html">http://glicaf.atmos=
.uiuc.edu/glicaf-index.html</a>.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Detailed analyses will examine the spatial and temporal variations =
of
atmospheric conditions near the surface and aloft. This is critical to
understanding flux observations and their relationship to surface condition=
s.
Preliminary analysis of conditions on 26 February 2004, summarized in Gerbu=
sh
et al. (2005), suggest that significant spatial variations of dynamic and
thermodynamic conditions were present. Particular care will be taken to
quantify and account for such variations in analyses of surface fluxes. Sur=
face
fluxes of heat and moisture will be estimated with eddy correlation techniq=
ues
applied to aircraft observations, as successfully demonstrated by numerous
researchers, including the PIs (e.g., Kristovich et al. 2003, Kristovich and
Braham 1998). While preliminary analyses suggest that atmospheric conditions
and surface heat fluxes are linked to ice cover (Gerbush et al. 2005), it is
critical to carefully assess the quality of the observations used in
eddy-correlation calculations of heat fluxes, and to confirm adequate sampl=
ing
of the turbulent eddies most responsible for vertical fluxes. Eddy-correlat=
ion
and appropriate filtering techniques, discussed in several recent papers (e=
.g.,
Caramori et al. 1994, Lenschow et al. 1994, Sun et al. 1996, Durand et al.
1995, Vickers and Mahrt 2004), will be employed as appropriate.<span
style=3D'mso-spacerun:yes'>&nbsp; </span><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Observations of ice cover were obtained through the use of a downwa=
rd
viewing digital video camera. The video gave continuous observations of sur=
face
conditions with the typical field of view of 350 m x 260 m with an image pi=
xel
resolution of about 0.5 m for an aircraft altitude of 500 m. We plan to use
digital thresholds of brightness as a first attempt at quantifying ice cover
amount. We have experience with this method, which was used to resolve cloud
features in Rauber et al. (1996).<span style=3D'mso-spacerun:yes'>&nbsp;
</span>Additional data were obtained with a Heimann downward-pointing
radiometer (Heimann KT-19.85), with a nominal accuracy of 0.5&deg;C.
Inter-comparisons between digital video images and Heimann data are highly
encouraging. Use of both datasets should provide reliable estimates of ice =
cover
distribution and concentration near the location of surface flux observatio=
ns. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Numerical studies will focus on the simulation of fluxes from the
broken-ice, water, and thin-ice covered lake and the resulting potential im=
pact
on lake-effect snow. Methods of aggregating the surface fluxes to fine-grid
numerical weather prediction scales will be examined using advanced land
surface models (for example, NCAR-LSM; Bonan, 1996).&nbsp;Very high-resolut=
ion
simulations resolving flux and surface inhomogeneities will be compared with
simulations using land surface models run at higher resolution than the
atmospheric model.&nbsp; This work will be a natural outgrowth of previous
scaling studies (Capehart and Gillies 1996, Capehart et al. 2001a,b).&nbsp;=
High
resolution simulations of case studies from GLICAF will be used to examine =
and
compare the utility of different aggregation approaches, using the advanced
surface and boundary layer schemes and parameterizations based on <st1:coun=
try-region
w:st=3D"on"><st1:place w:st=3D"on">SHEBA</st1:place></st1:country-region> a=
nd other
arctic studies.&nbsp;Detailed comparisons with the observations and sensiti=
vity
studies of the impact on forecasts of lake effects will be made.<o:p></o:p>=
</span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.3=
.2
Lake-to-lake interactions<o:p></o:p></span></b></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><!--[if gte vml 1]><v=
:shape
 id=3D"_x0000_s1087" type=3D"#_x0000_t202" style=3D'position:absolute;left:=
0;
 text-align:left;margin-left:0;margin-top:27pt;width:270.1pt;height:162pt;
 text-indent:0;z-index:-5;mso-position-horizontal:left' wrapcoords=3D"-60 0=
 -60 21500 21600 21500 21600 0 -60 0"
 stroked=3D"f">
 <v:textbox style=3D'mso-next-textbox:#_x0000_s1087'>
  <![if !mso]>
  <table cellpadding=3D0 cellspacing=3D0 width=3D"100%">
   <tr>
    <td><![endif]>
    <div>
    <p class=3DMsoNormal align=3Dcenter style=3D'text-align:center'><span
    style=3D'font-size:10.0pt'><v:shape id=3D"_x0000_i1027" type=3D"#_x0000=
_t75"
     style=3D'width:234.75pt;height:139.5pt'>
     <v:imagedata src=3D"proposal_description_041202_files/image005.emz" o:=
title=3D""
      cropright=3D"11826f"/>
    </v:shape></span></p>
    <p class=3DMsoNormal align=3Dcenter style=3D'text-align:center'><span
    style=3D'font-size:11.0pt'>Fig. 3. Two-year L2L band climatology (Rodri=
guez
    2003).<o:p></o:p></span></p>
    </div>
    <![if !mso]></td>
   </tr>
  </table>
  <![endif]></v:textbox>
 <w:wrap type=3D"square"/>
</v:shape><![endif]--><![if !vml]><img width=3D364 height=3D220
src=3D"proposal_description_041202_files/image006.gif" align=3Dleft hspace=
=3D12
alt=3D"Text Box:  &#13;&#10;Fig. 3. Two-year L2L band climatology (Rodrigue=
z 2003).&#13;&#10;"
v:shapes=3D"_x0000_s1087"><![endif]><span style=3D'font-size:11.0pt'>The
observational investigations of lake-to-lake (L2L) interactions will follow=
 two
avenues. First, a case study will be conducted of a L2L band that extended
between Lakes Superior and <st1:State w:st=3D"on"><st1:place w:st=3D"on">Mi=
chigan</st1:place></st1:State>
during the Lake-ICE project. Second, a climatological analysis will be
performed to provide information on the range of environmental conditions
conducive for L2L band occurrence, building on research conducted under the
previous grant.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Several cases of L2L bands were identified during the Lake-ICE proj=
ect.
Based on visible satellite, WSR-88D, and aircraft data, the 20 December 1997
and 19 January 1998 cases appear to be particularly appropriate for further
study. For example, preliminary analyses of the 19 January case suggest that
the UW King Air collected data on a growing internal convective boundary la=
yer
near the western <st1:place w:st=3D"on"><st1:PlaceType w:st=3D"on">shore</s=
t1:PlaceType>
 of <st1:PlaceName w:st=3D"on">Lake Michigan</st1:PlaceName></st1:place> an=
d the
vertical structure of the heavy L2L snowband near the eastern shore. These
observations will be used to document band structure and evolution, as well=
 as
give critical information for comparison with associated numerical model
simulations.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Climatological analyses using five years of visible satellite image=
ry
to determine the frequency and location of L2L cloud bands are being comple=
ted
under the current grant (Rodriguez 2003). Figure 3 shows an example analysi=
s of
L2L bands originating over <st1:place w:st=3D"on">Lake Superior</st1:place>=
 for
two of the five years examined. Results indicate that L2L bands can extend =
from
any of the northern or western <st1:place w:st=3D"on">Great Lakes</st1:plac=
e> to
the southern and eastern lakes. Bands between Lakes Ontario and <st1:City
w:st=3D"on"><st1:place w:st=3D"on">Erie</st1:place></st1:City> are rare. We=
 propose
to extend this research by examining surface, radar, and satellite data set=
s to
develop an understanding of variations in snow band position and movement,
changes in estimated snowfall rates across intervening land surfaces, and L=
2L
band diurnal evolution.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The associated modeling studies will also employ a two-pronged
approach. Simulations of L2L bands observed during Lake-ICE will be conduct=
ed
to examine the sensitivity of the L2L bands to environmental conditions. Th=
is
effort will use highly-successful approaches previously employed by our gro=
up
for examination of several lake-effect events. Understanding gained by
conducting case study simulations will be enhanced by performing more
generalized studies with single-sounding initializations over the lakes. Th=
is second
approach, similar to that used for single Lake Michigan bands by Hjelmfelt
(1990, 1992), will be utilized to examine a wide array of environmental
sensitivities across the range of conditions observed during L2L events over
the <st1:place w:st=3D"on">Great Lakes</st1:place>. The initial focus of th=
ese
simplified simulations will be directed toward determining the environmental
conditions allowing L2L bands to extend long distances over intervening land
areas, and to examine the over-land evolution of the residual boundary laye=
rs.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.3=
.3 Lake-effect
systems over small lakes</span></b><span style=3D'font-size:11.0pt'><o:p></=
o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The proposed study of lake-effect systems over small lakes will foc=
us
on snow events that occurred in the New York State (NYS) <st1:place w:st=3D=
"on">Finger
 Lakes</st1:place> region (Fig. 1) within the last decade. Lake-effect even=
ts
will be identified using criteria applied to the KBGM radar reflectivity fi=
eld,
supplemented by regional meteorological analyses. Events will be separated =
into
two classifications: 1) <i>Lake Effect</i>: precipitation structures which
develop over and downwind of a lake that are not associated with a larger-s=
cale
feature (i.e., synoptic frontal boundaries), or 2) <st1:place w:st=3D"on"><=
st1:PlaceType
 w:st=3D"on"><i>Lake</i></st1:PlaceType><i> <st1:PlaceName w:st=3D"on">Enha=
nced</st1:PlaceName></i></st1:place>:
precipitation associated with a larger-scale feature which is noticeably
enhanced by the development of local-scale radar reflectivity structures ov=
er
and downwind of a lake. During the classification of lake-effect and
lake-enhanced events, care will be taken in examining complex local
reflectivity patterns to identify and remove events that may have developed=
 due
to factors unrelated to the lakes. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><!--[if gte vml 1]><v=
:shape
 id=3D"_x0000_s1089" type=3D"#_x0000_t202" style=3D'position:absolute;left:=
0;
 text-align:left;margin-left:0;margin-top:33pt;width:5in;height:180pt;
 text-indent:0;z-index:-4;mso-position-horizontal:left' wrapcoords=3D"-56 0=
 -56 21480 21600 21480 21600 0 -56 0"
 stroked=3D"f">
 <v:textbox style=3D'mso-next-textbox:#_x0000_s1089'>
  <![if !mso]>
  <table cellpadding=3D0 cellspacing=3D0 width=3D"100%">
   <tr>
    <td><![endif]>
    <div>
    <p class=3DMsoNormal><span style=3D'font-size:10.0pt'><v:shape id=3D"_x=
0000_i1028"
     type=3D"#_x0000_t75" style=3D'width:344.25pt;height:147pt'>
     <v:imagedata src=3D"proposal_description_041202_files/image007.wmz" o:=
title=3D""/>
    </v:shape></span></p>
    <p class=3DMsoNormal><span style=3D'font-size:11.0pt'>Fig. 4. WSR-88D r=
adar
    reflectivity of lake-effect precipitation bands linked to Seneca and <s=
t1:place
    w:st=3D"on"><st1:PlaceName w:st=3D"on">Cayuga</st1:PlaceName> <st1:Plac=
eType
     w:st=3D"on">Lakes</st1:PlaceType></st1:place> in the New York State Fi=
nger
    Lakes region.<o:p></o:p></span></p>
    </div>
    <![if !mso]></td>
   </tr>
  </table>
  <![endif]></v:textbox>
 <w:wrap type=3D"square"/>
</v:shape><![endif]--><![if !vml]><img width=3D484 height=3D244
src=3D"proposal_description_041202_files/image008.gif" align=3Dleft hspace=
=3D12
alt=3D"Text Box:  &#13;&#10;Fig. 4. WSR-88D radar reflectivity of lake-effe=
ct precipitation bands linked to Seneca and Cayuga Lakes in the New York St=
ate Finger Lakes region.&#13;&#10;"
v:shapes=3D"_x0000_s1089"><![endif]><span style=3D'font-size:11.0pt'>The pr=
oposed
investigation of NYS Finger Lakes snow events will use archived radar,
meteorological, and lake data for the months of October &#8211; March for t=
he
years of 1995 &#8211; 2004. The timing of the events shown in Fig. 4 (i.e.,
Nov., Jan., and Feb.) suggests that snow bands originating from these small
lakes can occur throughout the winter season. The majority of Seneca and <s=
t1:PlaceName
w:st=3D"on">Cayuga</st1:PlaceName> <st1:PlaceType w:st=3D"on">Lakes</st1:Pl=
aceType>,
the largest of the 11 <st1:place w:st=3D"on">Finger Lakes</st1:place>, rema=
in
free of pack ice during the entire winter season due to their large volumes
(depths of 198 m and 132m, respectively). Several of the shallower lakes
typically have cooler winter temperatures and become ice covered during Jan=
uary
&#8211; March. These differences in environmental conditions, in addition to
fetch differences, will allow for a robust comparison of the lake-effect
systems that occur over each of the lakes during individual events. During =
the
events in Fig. 4 distinct mesoscale lake-effect snow bands originated from
Seneca and <st1:place w:st=3D"on"><st1:PlaceName w:st=3D"on">Cayuga</st1:Pl=
aceName>
 <st1:PlaceType w:st=3D"on">Lakes</st1:PlaceType></st1:place>, as well as s=
everal
of the smaller lakes, and extended downwind for nearly 30 km. <o:p></o:p></=
span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Our investigation will examine the frequency, spatial distribution,
intensity, and environmental conditions associated with mesoscale snow band=
s in
the NYS Finger Lakes region. Information on ice cover, lake water temperatu=
re,
and atmospheric parameters will be used to identify the favorable environme=
ntal
conditions which support small lake snow events. These data are collected b=
y a
number of sources in the <st1:place w:st=3D"on">Finger Lakes</st1:place> re=
gion
and are currently being assembled for inclusion into the clearinghouse data=
base
of the Finger Lakes Institute, located at Hobart &amp; William Smith Colleg=
es.
The results of our studies on lake-effect over small lakes will be compared
with findings from studies of larger lakes, such as the Great Lakes (e.g.,
Hjelmfelt 1990, Kristovich and Steve 1995, Laird et al. 2002, 2003) and the
Great Salt Lake (Steenburgh et al. 2000), and the few investigations of snow
bands associated with small lakes (Cosgrove et al. 1996, Watson et al. 1998,
Huggins et al. 2001, Cairns et al. 2001; Schultz et al. 2004). These will g=
ive
valuable information on the scalability of lake-effect circulations to small
lakes. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>In addition to the proposed climatological approach to examining NYS
Finger Lakes snow events, several case studies will be conducted. Events fr=
om
each of the two classifications (<i style=3D'mso-bidi-font-style:normal'>la=
ke-effect</i>
and <i style=3D'mso-bidi-font-style:normal'>lake-enhanced</i>) will be comp=
ared
to understand the changes in environmental conditions that lead to the
initiation of mesoscale snow band(s) and the temporal and spatial evolution=
 of
the events. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'><o:p>&nbsp;</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.3=
.4
Lake-effect and synoptic front interactions </span></b><span style=3D'font-=
size:
11.0pt'><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><!--[if gte vml 1]><v=
:shape
 id=3D"_x0000_s1090" type=3D"#_x0000_t202" style=3D'position:absolute;left:=
0;
 text-align:left;margin-left:0;margin-top:38.25pt;width:274.35pt;height:186=
.5pt;
 text-indent:0;z-index:-3;mso-position-horizontal:left' wrapcoords=3D"-71 0=
 -71 21483 21600 21483 21600 0 -71 0"
 stroked=3D"f">
 <v:textbox>
  <![if !mso]>
  <table cellpadding=3D0 cellspacing=3D0 width=3D"100%">
   <tr>
    <td><![endif]>
    <div>
    <p class=3DMsoNormal><span style=3D'font-size:10.0pt'><v:shape id=3D"_x=
0000_i1029"
     type=3D"#_x0000_t75" style=3D'width:285pt;height:141pt'>
     <v:imagedata src=3D"proposal_description_041202_files/image009.emz" o:=
title=3D""
      cropbottom=3D"12358f"/>
    </v:shape></span></p>
    <p class=3DMsoNormal><span style=3D'font-size:11.0pt'>Fig. 5. MM5 1000-=
hPa potential
    temperature (interval of 0.5 K) on 10 Jan 1998 showing (a) with-lake and
    (b) no-lake results (from Dreher et al. 2004).<o:p></o:p></span></p>
    </div>
    <![if !mso]></td>
   </tr>
  </table>
  <![endif]></v:textbox>
 <w:wrap type=3D"square"/>
</v:shape><![endif]--><![if !vml]><img width=3D370 height=3D253
src=3D"proposal_description_041202_files/image010.gif" align=3Dleft hspace=
=3D12
alt=3D"Text Box:  &#13;&#10;Fig. 5. MM5 1000-hPa potential temperature (int=
erval of 0.5 K) on 10 Jan 1998 showing (a) with-lake and (b) no-lake result=
s (from Dreher et al. 2004).&#13;&#10;"
v:shapes=3D"_x0000_s1090"><![endif]><span style=3D'font-size:11.0pt'>The in=
itial
focus of this investigation will be to develop a 5-10-year climatologic
database of wintertime synoptic frontal passages over individual <st1:place
w:st=3D"on">Great Lakes</st1:place> using surface, radar, satellite, and
upper-air datasets. The climatologic database of synoptic fronts will be us=
ed
to examine the frequency of passage, frontal orientation relative to the la=
ke
axes, and associated environmental and lake-surface conditions. Radar,
satellite, and surface observations will be examined to ascertain lake effe=
cts
on frontal speed, radar echo structure, or precipitation.&nbsp;Events will =
be
examined as a function of frontal type and specific <st1:place w:st=3D"on">=
Lake</st1:place>.&nbsp;&nbsp;
Lakes <st1:State w:st=3D"on">Michigan</st1:State>, <st1:City w:st=3D"on">Er=
ie</st1:City>,
and <st1:State w:st=3D"on"><st1:place w:st=3D"on">Ontario</st1:place></st1:=
State>
will be emphasized because of the considerable radar and surface observatio=
ns
in their vicinity. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Several cases will be chosen for more in-depth study including model
simulations, as in Dreher (2004) and Dreher et al (2004a,b), to further exa=
mine
the physical processes that result in a modification of the frontal
characteristics. Dreher (2004) found both observations and simulations
indicated that the cold front moved more slowly over the lake than over
adjacent land areas south of the lake (Fig 5).&nbsp; Observed radar
reflectivities were higher and more widespread downwind of the lake, as were
the corresponding simulated precipitation fields. Numerical sensitivity stu=
dies
suggested that, enhanced mixing due to the warm lake dominated over effects=
 of
the smoother lake surface to retard frontal progress over the lake.&nbsp;
Sensitivity simulations for the cases chosen for study will examine the
relative importance of lake-land temperature difference (turbulent mixing),
surface roughness and cloud processes (latent heating) within the frontal
bands.&nbsp; Differences in individual <st1:place w:st=3D"on"><st1:PlaceType
 w:st=3D"on">lake</st1:PlaceType> <st1:PlaceName w:st=3D"on">influencess</s=
t1:PlaceName></st1:place>,
pack ice cover, and the effects of the multiple lakes will also be
considered.&nbsp; Results will be generalized by relating the detailed stud=
ies
to the climatological analyses.<o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>3.3=
.5
Lake-Effect Cloud, Precipitation, and Radiative processes </span></b><span
style=3D'font-size:11.0pt'><o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Microphysical and radiation data collected by aircraft during the
Lake-ICE project will be used to<span style=3D'mso-spacerun:yes'>&nbsp;
</span>(1) understand the spatial and temporal changes in processes within =
the
lake-effect system and (2) create a dataset important for comparison with m=
odel
simulations of lake-effect systems. Lake-ICE flight plans were designed to
examine in-cloud and near-cloud conditions. To examine microphysical proces=
ses
in lake-effect clouds, the primary approach will be to compare changes in
microphysical characteristics across <st1:place w:st=3D"on">Lake Michigan</=
st1:place>
during classic lake-effect events and non-classic events where natural cloud
seeding from higher-level clouds occurred. For the chosen cases, cross-lake
spectral changes in cloud and precipitation particles will be investigated,=
 as
well as bulk parameters that are relevant to describing the cloud microphys=
ics
(e.g., water contents, volume mean diameter, etc.). Additionally, relations=
hips
of particle spectra and bulk parameter variations with small-scale convecti=
ve
eddies will be determined using techniques developed by Braham and Kristovi=
ch
(1996). Classic lake-effect cases (10 and 13 January 1998), non-classic see=
ding
cases (6, 20 December 1997, and 18 January 1998), and a nocturnal case (19
January 1998) have been identified. Completed studies by Schroeder et al.
(2003) of the 5 December 1997 seeding case will be used for comparison. <o:=
p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>Variations in vertical radiative fluxes and implied heating/cooling
rates will be determined for cases targeted for microphysical analyses.
Lake-ICE aircraft carried sensors for detecting upward and downward directe=
d,
longwave and shortwave radiation. Examination of the vertical and horizontal
(i.e., cross lake) variations of radiative fluxes and derived heating rates
using pass-mean radiative properties combined with cloud and precipitation
analyses will allow for the development of a combined cloud, precipitation,=
 and
radiative conceptual model for lake-effect systems. Findings will be compar=
ed
with the only previous observational study to quantify radiative heating ra=
tes
in lake-effect boundary layers, Chang and Braham (1991), and will provide a
better understanding and dataset for comparison with mesoscale model simula=
tions
of lake-effect systems. <o:p></o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>4.
Timeline and Collaboration</span></b><span style=3D'font-size:11.0pt'><o:p>=
</o:p></span></p>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify;text-indent:.25in'><span style=3D'font-s=
ize:
11.0pt'>The three Principal Investigators each provide expertise that is
crucial to the proposed research project. Through well-established
collaboration, we are able to address the inter-related issues associated w=
ith
lake-effect and lake-enhanced systems. This table outlines the PIs&#8217;
efforts (UIUC: Kristovich, HWS: Laird, SDSMT: Hjelmfelt) toward the five
objectives of the proposed research. While we will collaborate as appropria=
te
(CAA) on all efforts, it is most efficient for each PI to lead<span
style=3D'mso-spacerun:yes'>&nbsp; </span>different aspects of the research.=
 Dr.
Kristovich (UIUC) will lead efforts on L2L observational studies, flux
observations from GLICAF, and cloud, precipitation, and radiation analyses
using Lake-ICE datasets. Dr. Laird will lead studies of lake-effect systems
over small lakes and GLICAF ice cover analyses. Dr. Hjelmfelt will lead
modeling efforts related to GLICAF, L2L bands, and fronts. Dr. Capehart, at
South Dakota School of Mines and Technology, will play a large role in
numerical modeling on non-uniform surface conditions observed during GLICAF.
This collaborative approach has been highly successful in previous efforts,
resulting in many multi-institution published papers.<o:p></o:p></span></p>

<p class=3DMsoBodyTextIndent style=3D'margin-top:3.0pt;margin-right:0in;mar=
gin-bottom:
3.0pt;margin-left:0in;text-indent:.25in'><span style=3D'mso-bidi-font-size:=
11.0pt'><o:p>&nbsp;</o:p></span></p>

<table class=3DMsoNormalTable border=3D1 cellspacing=3D0 cellpadding=3D0 wi=
dth=3D638
 style=3D'width:6.65in;border-collapse:collapse;border:none;mso-border-alt:=
solid windowtext .5pt;
 mso-padding-alt:0in 5.4pt 0in 5.4pt;mso-border-insideh:.5pt solid windowte=
xt;
 mso-border-insidev:.5pt solid windowtext'>
 <tr style=3D'mso-yfti-irow:0;mso-yfti-firstrow:yes'>
  <td width=3D121 valign=3Dtop style=3D'width:90.9pt;border:solid windowtex=
t 1.0pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>Topic<o:p></o:p><=
/span></p>
  </td>
  <td width=3D168 valign=3Dtop style=3D'width:1.75in;border:solid windowtex=
t 1.0pt;
  border-left:none;mso-border-left-alt:solid windowtext .5pt;mso-border-alt:
  solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>Year 1<o:p></o:p>=
</span></p>
  </td>
  <td width=3D180 valign=3Dtop style=3D'width:135.0pt;border:solid windowte=
xt 1.0pt;
  border-left:none;mso-border-left-alt:solid windowtext .5pt;mso-border-alt:
  solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>Year 2<o:p></o:p>=
</span></p>
  </td>
  <td width=3D169 valign=3Dtop style=3D'width:126.9pt;border:solid windowte=
xt 1.0pt;
  border-left:none;mso-border-left-alt:solid windowtext .5pt;mso-border-alt:
  solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>Year 3<o:p></o:p>=
</span></p>
  </td>
 </tr>
 <tr style=3D'mso-yfti-irow:1'>
  <td width=3D121 valign=3Dtop style=3D'width:90.9pt;border:solid windowtex=
t 1.0pt;
  border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:s=
olid windowtext .5pt;
  padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>Influence of ice =
cover<o:p></o:p></span></p>
  </td>
  <td width=3D168 valign=3Dtop style=3D'width:1.75in;border-top:none;border=
-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: sfc flux an=
aly.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: ice cover an=
aly.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: model=
 dev.<o:p></o:p></span></p>
  </td>
  <td width=3D180 valign=3Dtop style=3D'width:135.0pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: sfc flux an=
aly.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: ice cover an=
aly.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: sensi=
tivity
  tests<o:p></o:p></span></p>
  </td>
  <td width=3D169 valign=3Dtop style=3D'width:126.9pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: thesis comp=
letion<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: pub. obs. re=
sults.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span lang=3DDE style=3D'font-size:11.0pt;mso-ansi=
-language:
  DE'>SDSM&amp;T:pub. model res<o:p></o:p></span></p>
  </td>
 </tr>
 <tr style=3D'mso-yfti-irow:2'>
  <td width=3D121 valign=3Dtop style=3D'width:90.9pt;border:solid windowtex=
t 1.0pt;
  border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:s=
olid windowtext .5pt;
  padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><st1:place w:st=3D"on"><span style=3D'font-size:11=
.0pt'>Lake-to-lake</span></st1:place><span
  style=3D'font-size:11.0pt'> interactions<o:p></o:p></span></p>
  </td>
  <td width=3D168 valign=3Dtop style=3D'width:1.75in;border-top:none;border=
-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: L2L case st=
udy<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: sensi=
t.
  tests,<span style=3D'mso-spacerun:yes'>&nbsp; </span>case simulation<o:p>=
</o:p></span></p>
  </td>
  <td width=3D180 valign=3Dtop style=3D'width:135.0pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: begin clim.
  analy.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: publ.
  results case, sensit. tests<o:p></o:p></span></p>
  </td>
  <td width=3D169 valign=3Dtop style=3D'width:126.9pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: pub. obs. r=
esults<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: pub.
  sensit. results<o:p></o:p></span></p>
  </td>
 </tr>
 <tr style=3D'mso-yfti-irow:3'>
  <td width=3D121 valign=3Dtop style=3D'width:90.9pt;border:solid windowtex=
t 1.0pt;
  border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:s=
olid windowtext .5pt;
  padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>Lake-effect syste=
ms
  over small lakes<o:p></o:p></span></p>
  </td>
  <td width=3D168 valign=3Dtop style=3D'width:1.75in;border-top:none;border=
-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: CAA<o:p></o=
:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: radar clim. =
analy.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: CAA<o=
:p></o:p></span></p>
  </td>
  <td width=3D180 valign=3Dtop style=3D'width:135.0pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: CAA<o:p></o=
:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: radar clim. =
analy.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: - CAA=
<o:p></o:p></span></p>
  </td>
  <td width=3D169 valign=3Dtop style=3D'width:126.9pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: CAA<o:p></o=
:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: pub. results=
<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: CAA<o=
:p></o:p></span></p>
  </td>
 </tr>
 <tr style=3D'mso-yfti-irow:4'>
  <td width=3D121 valign=3Dtop style=3D'width:90.9pt;border:solid windowtex=
t 1.0pt;
  border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:s=
olid windowtext .5pt;
  padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>Lake-effect and s=
yn.
  front interactions<o:p></o:p></span></p>
  </td>
  <td width=3D168 valign=3Dtop style=3D'width:1.75in;border-top:none;border=
-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: clim. analy=
.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: clim.
  analy.<o:p></o:p></span></p>
  </td>
  <td width=3D180 valign=3Dtop style=3D'width:135.0pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: clim. analy=
.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: simul=
ations<o:p></o:p></span></p>
  </td>
  <td width=3D169 valign=3Dtop style=3D'width:126.9pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: CAA<o:p></o=
:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: pub. =
resul.<o:p></o:p></span></p>
  </td>
 </tr>
 <tr style=3D'mso-yfti-irow:5;mso-yfti-lastrow:yes'>
  <td width=3D121 valign=3Dtop style=3D'width:90.9pt;border:solid windowtex=
t 1.0pt;
  border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:s=
olid windowtext .5pt;
  padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>Cloud, precip. and
  radiative processes<o:p></o:p></span></p>
  </td>
  <td width=3D168 valign=3Dtop style=3D'width:1.75in;border-top:none;border=
-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: aircraft an=
aly.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: CAA<o=
:p></o:p></span></p>
  </td>
  <td width=3D180 valign=3Dtop style=3D'width:135.0pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: aircraft an=
aly.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: CAA<o=
:p></o:p></span></p>
  </td>
  <td width=3D169 valign=3Dtop style=3D'width:126.9pt;border-top:none;borde=
r-left:
  none;border-bottom:solid windowtext 1.0pt;border-right:solid windowtext 1=
.0pt;
  mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid window=
text .5pt;
  mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>UIUC: complete an=
aly.<o:p></o:p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>HWS: CAA<o:p></o:=
p></span></p>
  <p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bo=
ttom:
  3.0pt;margin-left:0in'><span style=3D'font-size:11.0pt'>SDSM&amp;T: CAA<o=
:p></o:p></span></p>
  </td>
 </tr>
</table>

<p class=3DMsoNormal style=3D'margin-top:3.0pt;margin-right:0in;margin-bott=
om:3.0pt;
margin-left:0in;text-align:justify'><b><span style=3D'font-size:11.0pt'>5.
Broader Impacts<o:p></o:p></span></b></p>

<p class=3DMsoBodyTextIndent style=3D'margin-top:3.0pt;margin-right:0in;mar=
gin-bottom:
3.0pt;margin-left:0in;text-indent:.25in'><span style=3D'mso-bidi-font-size:=
11.0pt'>Results
of the proposed studies will give valuable insight into interactions between
antecedent and new internal boundary layers, interactions between fronts an=
d boundary
layers, and characteristics of cloud-topped marine boundary layers. These
complex processes often complicate winter forecasting of mesoscale phenomena
common to the <st1:place w:st=3D"on">Great Lakes</st1:place> region. Our fi=
ndings
from GLICAF analyses should be helpful to high-latitude studies, particular=
ly
on regions where decreases in ice cover and thickness are predicted.</span>
Results will be communicated to the meteorological community through journal
and conference articles and to the operational community through regional
workshops and presentations at National Weather Service offices. Based on o=
ur
experiences with previous grants, such workshops and presentations are
beneficial to the forecasting community. In this way, the improved
understanding gained from the proposed research will benefit society as a
result of improved forecasts of lake-effect phenomena. <span style=3D'mso-b=
idi-font-size:
11.0pt'><span style=3D'mso-spacerun:yes'>&nbsp;</span>Results of the propos=
ed
studies will provide insights which can impact work on atmospheric response=
 to
heterogeneous surfaces, air-ice-sea interactions, and other areas beyond
lake-effect snow storms. In addition, the next generation of forecasters and
scientists will benefit through a wide range of graduate and undergraduate
educational and training activities. Results will be incorporated into
classroom lessons for both atmospheric science majors and non-majors.<o:p><=
/o:p></span></p>

<b><i><span style=3D'font-size:11.0pt;font-family:Arial;mso-fareast-font-fa=
mily:
"Times New Roman";mso-ansi-language:EN-US;mso-fareast-language:EN-US;
mso-bidi-language:AR-SA'><br clear=3Dall style=3D'mso-column-break-before:a=
lways'>
</span></i></b>

<div style=3D'mso-element:para-border-div;border:none;border-bottom:solid w=
indowtext 1.0pt;
mso-border-bottom-alt:solid windowtext .5pt;padding:0in 0in 1.0pt 0in'>

<p class=3DMsoTitle style=3D'margin-top:3.0pt;margin-right:0in;margin-botto=
m:3.0pt;
margin-left:0in'><span style=3D'mso-bidi-font-size:11.0pt;font-family:"Time=
s New Roman"'>REFERENCES<o:p></o:p></span></p>

</div>

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