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<!--l. 120--><p class="noindent">
</p><!--l. 125--><p class="noindent"><span 
class="cmbx-12">Enhanced Gaseous Absorption, Earth&#x2019;s Energy Budget, and Climate</span><br />
PI: Charles S. Zender<br />
University of California at Irvine<br />
</p>
</div>
<!--l. 131--><p class="noindent">Department of Earth System Science                                                      <span class="obeylines-h"><a 
href="zender@uci.edu" class="url" ><span 
class="cmtt-12">zender@uci.edu</span></a></span>
<br class="newline" />University of California                                                                                 Voice:
(949) 824-2987
<br class="newline" />Irvine, CA&#x00A0;&#x00A0;92697-3100                                                                                   Fax:
(949) 824-3256
</p><!--l. 135--><p class="noindent"><span 
class="cmbx-12">Project Summary</span>
<br class="newline" />This proposal outlines a program of scientific research and educational development focused
on radiative forcing and climate. The scientific program consists of determining the
role of three gaseous species in closing Earth&#x2019;s energy budget and in radiatively forcing
present and future climate. The gases are water vapor, collision complexes of oxygen
(<!--l. 143--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>), and
nitrogen dioxide. Absorption by these gases has heretofore been oversimplified or neglected in large
scale atmospheric models, so their radiative forcing and climate impact remain uncertain. By
representing these missing absorption processes, this project will directly improve predictions of
atmospheric heating, estimates of Earth&#x2019;s energy budget, and, likely, the accuracy of climate
predictions.
</p><!--l. 153--><p class="indent">   Oversimplifications in current representations of
<!--l. 153--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 153--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
<!--l. 154--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;in
large scale models are known and will be reduced or eliminated. First, water vapor absorption of
solar and terrestrial radiation in cloudy atmospheres is systematically underestimated and
biased by neglecting the sub-gridscale partitioning of vapor between the saturated cloud
and the sub-saturated clear sky. Second, collision complexes of oxygen absorb about
1&#x00A0;W m<!--l. 160--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;globally
annually averaged, but the climate response to this forcing is unknown. Third, neglected
<!--l. 163--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption
will be examined using a combination of satellite and model data to constrain
its distribution. These mechanisms are, in sum, expected to reduce the
current discrepancy in the global annual mean atmospheric energy budget by
2&#x2013;8&#x00A0;W m<!--l. 167--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;(10&#x2013;30% of the total
                                                                                         
                                                                                         
discrepancy). Moreover, <!--l. 168--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;and
<!--l. 168--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;forcings
are likely to change with climate.
</p><!--l. 170--><p class="indent">   The educational component of the proposal is to found a project to coordinate the
development, solicitation, standardization, and dissemination of Freely Available Community Texts
(FACTs) suitable for education and teaching in the Earth system sciences. Each FACT will be a
living monograph available via the World Wide Web to students and scientists anywhere to study,
modify, and improve. The license ensures authors retain recognition, copyright, and
review priveleges over modifications to their original material. The project will begin
with two existing, pilot FACTs designed to educate students about radiative forcing
and aerosols. We envision contributions of new material and FACTs from students and
faculty within our department, but, more significantly, from the international geosciences
community.
                                                                                         
                                                                                         
</p>
   <h3 class="likesectionHead"><a 
 id="x1-1000"></a>Contents</h3>
   <div class="tableofcontents">
   <span class="sectionToc">1 <a 
href="#x1-20001" id="QQ2-1-2">Results from Prior NSF Support</a></span>
<br />   <span class="sectionToc">2 <a 
href="#x1-30002" id="QQ2-1-3">Introduction</a></span>
<br />   <span class="sectionToc">3 <a 
href="#x1-40003" id="QQ2-1-4">Freely Available Community Texts</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.1 <a 
href="#x1-50003.1" id="QQ2-1-5">Vision Statement</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.2 <a 
href="#x1-60003.2" id="QQ2-1-6">Mission</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.3 <a 
href="#x1-70003.3" id="QQ2-1-7">Prototypes and Curricular Integration</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.4 <a 
href="#x1-80003.4" id="QQ2-1-8">Scientific Quality</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.5 <a 
href="#x1-90003.5" id="QQ2-1-9">Existing Free Community Geosciences Educational Material</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.6 <a 
href="#x1-100003.6" id="QQ2-1-10">Entraining Students and Educators</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.7 <a 
href="#x1-110003.7" id="QQ2-1-11">FACTs Project Organization and Communication</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.8 <a 
href="#x1-120003.8" id="QQ2-1-12">Project Work Plan</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.9 <a 
href="#x1-130003.9" id="QQ2-1-13">Project Evaluation</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.10 <a 
href="#x1-140003.10" id="QQ2-1-14">Significance to Professional Goals and Responsibilities</a></span>
<br />   &#x00A0;<span class="subsectionToc">3.11 <a 
href="#x1-150003.11" id="QQ2-1-15">Prior Education, Outreach, and Service Accomplishments</a></span>
<br />   <span class="sectionToc">4 <a 
href="#x1-160004" id="QQ2-1-16">Enhanced Gaseous Absorption and Climate</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.1 <a 
href="#x1-170004.1" id="QQ2-1-17">Overview</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.2 <a 
href="#x1-180004.2" id="QQ2-1-18">Shortwave Gaseous Absorption</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.3 <a 
href="#x1-190004.3" id="QQ2-1-20">Absorption by Water Vapor</a></span>
<br />   &#x00A0;&#x00A0;<span class="subsubsectionToc">4.3.1 <a 
href="#x1-200004.3.1" id="QQ2-1-21">Water Vapor Continuum Absorption</a></span>
<br />   &#x00A0;&#x00A0;<span class="subsubsectionToc">4.3.2 <a 
href="#x1-210004.3.2" id="QQ2-1-22">Water Vapor Dimer Absorption</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.4 <a 
href="#x1-220004.4" id="QQ2-1-23">Absorption by Collision Complexes of Oxygen</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.5 <a 
href="#x1-230004.5" id="QQ2-1-25">Absorption by Nitrogen Dioxide</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.6 <a 
href="#x1-240004.6" id="QQ2-1-26">Climate Sensitivity to Enhanced Absorption</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.7 <a 
href="#x1-250004.7" id="QQ2-1-27">Objectives and Hypotheses</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.8 <a 
href="#x1-260004.8" id="QQ2-1-28">Research Plans</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.9 <a 
href="#x1-270004.9" id="QQ2-1-29">Methods and Procedures</a></span>
<br />   &#x00A0;&#x00A0;<span class="subsubsectionToc">4.9.1 <a 
href="#x1-280004.9.1" id="QQ2-1-30">Model Evaluation</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.10 <a 
href="#x1-290004.10" id="QQ2-1-31">Expected Significance of Results</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.11 <a 
href="#x1-300004.11" id="QQ2-1-32">Synergies with Existing Research Efforts</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.12 <a 
href="#x1-310004.12" id="QQ2-1-33">Benefits to Community</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.13 <a 
href="#x1-320004.13" id="QQ2-1-34">Significance to Professional Goals and Responsibilities</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.14 <a 
href="#x1-330004.14" id="QQ2-1-35">Work Plan for Research</a></span>
<br />   &#x00A0;<span class="subsectionToc">4.15 <a 
href="#x1-340004.15" id="QQ2-1-36">Prior Research Accomplishments</a></span>
<br />   <span class="sectionToc">5 <a 
href="#x1-350005" id="QQ2-1-37">References</a></span>
<br />   <span class="sectionToc">6 <a 
href="#x1-370006" id="QQ2-1-39">Curriculum Vitae</a></span>
   </div>
                                                                                         
                                                                                         
   <h3 class="sectionHead"><span class="titlemark">1   </span> <a 
 id="x1-20001"></a>Results from Prior NSF Support</h3>
<!--l. 197--><p class="noindent">Dr. Zender has not previously had NSF support.
</p><!--l. 199--><p class="noindent">
</p>
   <h3 class="sectionHead"><span class="titlemark">2   </span> <a 
 id="x1-30002"></a>Introduction</h3>
<!--l. 201--><p class="noindent">This proposal outlines a five year program of research and educational development in Earth
System Sciences. The first portion of this proposal describes a project to coordinate development
and dissemination of a series of freely available educational geoscience monographs over the
World Wide Web. Each monograph will be written, reviewed and maintained by talented
students and educators with research interests in that field. We argue that this project will
become a high-quality resource for geoscience education because, being free, it will enlist
talents and contributions from the worldwide community of interested students and
educators.
</p><!--l. 213--><p class="indent">   The second portion of this proposal outlines a scientific research program to improve our
understanding of gaseous radiative forcing of climate, and of the climate response to this forcing. The
research project employs a hierarchy of models to simulate radiative forcing by three important gaseous
species, <!--l. 217--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 217--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
<!--l. 218--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>.
This project is organized into sub-projects for each gas, and concludes with integrative
studies involving all three gases. The studies contribute separately and in tandem to the
overall goals of closing Earth&#x2019;s radiative energy budget, understanding the response
of the climate system to trace gas forcing, and improving predictions of atmospheric
heating.
</p><!--l. 226--><p class="noindent">
</p>
   <h3 class="sectionHead"><span class="titlemark">3   </span> <a 
 id="x1-40003"></a>Freely Available Community Texts</h3>
<!--l. 228--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.1   </span> <a 
 id="x1-50003.1"></a>Vision Statement</h4>
<!--l. 229--><p class="noindent">The amount of information a geoscientist must master continuously increases as journals and data
archives proliferate and grow. Educators in the geosciences must ingest even more information in
order to remain current in their teaching and research careers. Comprehensive textbooks become
out of date soon after printing, and narrow, specialists texts are exorbitantly priced. Buying
more textbooks to keep up with this information glut is a short term solution that
only relatively priveleged students and researchers can afford. A better solution is to
                                                                                         
                                                                                         
harness the networking power of the World Wide Web to coordinate the distributed
development, maintainance, and distribution of &#x201C;living texts&#x201D; in the geosciences. The
educational component of this proposal is to found a project to organize the creation of Freely
Available Community Texts (FACTs) suitable for education and teaching in Earth System
Sciences.
</p><!--l. 245--><p class="indent">   The FACT project is not an idealistic pipe dream, as shown by the rapid growth of freely
distributed and community maintained software known as Free Software or Open Source software
[<a 
href="#XRay99"><span 
class="cmti-12">Raymond</span></a>,&#x00A0;<a 
href="#XRay99">1999</a>]. Adopting the successful principles underlying the Free Software movement,
FACT authors will retain copyright to their monographs, but will give the academic community
the license to modify, extend, and update (possibly portions of) their texts in perpetuity. It is
anticipated that graduate students, postdocs, and researchers will contribute significantly to
FACTs from their theses, collections of homework problems, and self-developed course
teaching materials. Moreover, all interested geoscientists with access to the Internet,
regardless of nationality or income, can benefit from and contribute to the high-quality
FACTs.
</p><!--l. 259--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.2   </span> <a 
 id="x1-60003.2"></a>Mission</h4>
<!--l. 260--><p class="noindent">The FACT project is intended to standardize and disseminate our fundamental knowledge of Earth
System Sciences in a flexible, adaptive, distributed framework which can evolve to fit the changing
needs and technology of the geosciences community. FACTs will be created, reviewed,
and continuously maintained and updated by members of the international academic
community communicating with eachother through a well-organized project website.
Each FACT will describe a specific subject area of the Earth system in detail, using a
consistent nomenclature and style common to the series. For example, the FACTs I
write (see <span 
class="cmsy-10x-x-120">&#x00A7;</span>&#x00A0;<a 
href="#x1-70003.3">3.3<!--tex4ht:ref: sxn:prt --></a>) are integrated with my research and teaching interests in climate and
radiative forcing (and thus with my Department&#x2019;s research mission). The primary author
or maintainer of the FACT is responsible for reviewing and approving changes and
updates.
</p><!--l. 277--><p class="indent">   FACTs are intended to cover fundamental and well-established principles of a given discipline,
not to replace or be an alternative for tradiational, peer-reviewed scientific journals. Thus FACTs
will not include speculative or unpublished theories. FACTs should start with the first priniciples
of a given field. The continual improvement of FACTs over time will result in texts that are more
current and up-to-date with recent advances in the field every year. The long term (5&#x2013;10 year) goal
is to build high quality state of the art monographs which are indispensable to researchers as well
as students.
</p><!--l. 289--><p class="indent">   To preserve the freedom of the community to modify the FACTs, and the rights of the authors
to control their intellectual property, FACTs will be distributed under a license called the GNU
Free Documentation License (FDL) (<span class="obeylines-h"><a 
href="http://www.gnu.ai.mit.edu/copyleft/fdl.html" class="url" ><span 
class="cmtt-12">http://www.gnu.ai.mit.edu/copyleft/fdl.html</span></a></span>). The
FDL ensures authors retain recognition, copyright, and review priveleges over modifications to
their original material. Once an author applies the FDL license, the FACT and all derived works of
it are forever freely available to all under the same terms. This perpetuity ensures that FACTs are
                                                                                         
                                                                                         
always and forever available via the World Wide Web to students and scientists anywhere to study,
modify, and improve.
</p><!--l. 302--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.3   </span> <a 
 id="x1-70003.3"></a>Prototypes and Curricular Integration</h4>
<!--l. 303--><p class="noindent">Two prototype FACTs, &#x201C;Radiative Transfer in the Earth System&#x201D; and &#x201C;Particle Size Distributions:
Theory and Application to Aerosols, Clouds, and Soils&#x201D; have been developed to supplement the
textbook in my new graduate course, ESS 111/211: &#x201C;Radiative Processes and Remote Sensing&#x201D;.
These prototypes are available from my website at <span class="obeylines-h"><a 
href="http://www.ess.uci.edu/~zender/rt" class="url" ><span 
class="cmtt-12">http://www.ess.uci.edu/~zender/rt</span></a></span> and
<span class="obeylines-h"><a 
href="http://www.ess.uci.edu/~zender/psd" class="url" ><span 
class="cmtt-12">http://www.ess.uci.edu/~zender/psd</span></a></span>, respectively. Examination of the Radiative Transfer
FACT illustrates some of the promise and pitfalls of FACTs.
      </p><ol  class="enumerate1" >
      <li class="enumerate" value="1" 
><a 
 id="x1-7002x1"></a>HTML format is for online browsing and the other formats are for printing (Postscript,
      PDF, DVI) or modification
      </li>
      <li class="enumerate" value="2" 
><a 
 id="x1-7004x2"></a>FACTs can look and be as professional as any textbook
      </li>
      <li class="enumerate" value="3" 
><a 
 id="x1-7006x3"></a>The Table of Contents, Reference section, and Index make FACTs easy to search
      </li>
      <li class="enumerate" value="4" 
><a 
 id="x1-7008x4"></a>Hyperlinks and cross-references within and among FACTs is possible but has not yet
      been implemented</li></ol>
<!--l. 323--><p class="indent">   Examples of welcome contributions which interested students and researchers in the radiative
transfer community could make to the radiative transfer FACT include (this task list should be
maintained within the FACT itself)
      </p><ol  class="enumerate1" >
      <li class="enumerate" value="1" 
><a 
 id="x1-7010x1"></a>Figures which illustrate the material in the text
      </li>
      <li class="enumerate" value="2" 
><a 
 id="x1-7012x2"></a>More homework exercises (see the example on Page&#x00A0;18)
      </li>
      <li class="enumerate" value="3" 
><a 
 id="x1-7014x3"></a>Standalone special interest boxes (e.g., &#x201C;Geometric Devivation of Optical Depth&#x201D; on
      pages 8&#x2013;9)
      </li>
      <li class="enumerate" value="4" 
><a 
 id="x1-7016x4"></a>Text for unfinished sections such as the optical properties on pages 30&#x2013;31.</li></ol>
<!--l. 335--><p class="noindent">Each graduate student enrolled in my ESS 211 course will be asked to contribute an item from this to
the Radiative Transfer FACT. The students will gain appreciation of the community value of
distributed collaborative work, and will be credited for the authorship of their contribution in the
FACT itself.
                                                                                         
                                                                                         
</p><!--l. 341--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.4   </span> <a 
 id="x1-80003.4"></a>Scientific Quality</h4>
<!--l. 342--><p class="noindent">Two forms of &#x201C;peer review&#x201D; will help ensure FACTs remain high quality materials. First, a
manuscript&#x2019;s primary author may decline any revisions which do not meet his standards. Of
course there is strong social pressure against submitting inferior contributions with one&#x2019;s
name attached. On the other hand, FACTs which are particularly well-written and
widely used may eventually garner their authors (and their institutions) international
recognition for their expertise and pedagogical skills. Second, FACTs are open texts
so they are subject to continuous suggestions and refinements by new readers. The
exposure will help authors identify any mistakes, omissions, or inadvertent plagiarism in the
texts.
</p><!--l. 357--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.5   </span> <a 
 id="x1-90003.5"></a>Existing Free Community Geosciences Educational Material</h4>
<!--l. 358--><p class="noindent">To our knowledge there are no other projects which create and make freely available geoscience
texts that are open to community modification. The design of FACTs appears to be truly
innovative, which makes foreseeing potential problems or learning from previous mistakes very
difficult. We believe that texts which can be modified to fit changing needs of users will be of
lasting intellectual value to the geoscience community, and that the community will recognize this
and help to make FACTs a success.
</p><!--l. 394--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.6   </span> <a 
 id="x1-100003.6"></a>Entraining Students and Educators</h4>
<!--l. 395--><p class="noindent">One of my priorities is to ensure that others contribute new FACTs which broaden the intellectual
appeal of the project beyond my own research interests. I will actively solicit colleagues to consider
contributing a FACT in their own niche. An informal poll of colleagues in my department and
elsewhere showed all were interested on contributing material to this project. Many expressed
hope that FACTs might become an integrative exercise for the department, allowing us
to share our expertise and painstakingly developed lecture notes with eachother more
easily.
</p><!--l. 406--><p class="indent">   One promising source of contributors are graduate students. While taking classes and preparing
for comprehensive and thesis examinations, graduate students often have more time and
motivation to read texts than more accomplished professionals in the field. Graduate students who
find problems or gaps with these monographs are likelier to send contributions than others. As
discussed in <span 
class="cmsy-10x-x-120">&#x00A7;</span>&#x00A0;<a 
href="#x1-70003.3">3.3<!--tex4ht:ref: sxn:prt --></a> graduate students in my courses will be asked to make a contribution to
FACTs.
                                                                                         
                                                                                         
</p><!--l. 415--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.7   </span> <a 
 id="x1-110003.7"></a>FACTs Project Organization and Communication</h4>
<!--l. 416--><p class="noindent">All project bookkeeping and coordination will be performed in the open via mail lists and discussion
forums. The FACTs website will initially be based at SourceForge (<span class="obeylines-h"><a 
href="http://sourceforge.net" class="url" ><span 
class="cmtt-12">http://sourceforge.net</span></a></span>), a
widely used, pro-bono website for Open Source projects. SourceForge hosts my successful netCDF
Operator (NCO) project (<span class="obeylines-h"><a 
href="http://sourceforge.net/projects/nco" class="url" ><span 
class="cmtt-12">http://sourceforge.net/projects/nco</span></a></span>) (and many much larger
projects) and provides the essential tools for administering a large, distributed project like FACTs.
The website will provide the following for each FACT: electronic forums for user/author discussion,
announcement lists to notify users of new contributions, staging areas for contributions under
review, download area.
</p><!--l. 430--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.8   </span> <a 
 id="x1-120003.8"></a>Project Work Plan</h4>
<!--l. 431--><p class="noindent">During Year&#x00A0;1 the programmer/analyst will concentrate on generating document templates for
authoring FACTs, and developing a working community website. PI Zender will integrate the
prototype FACTs into his graduate-level course on Radiative Processes and will solicit colleagues
to contribute new FACTs.
</p><!--l. 438--><p class="indent">   In Years 2 and&#x00A0;3 PI Zender will contribute new FACTs on particle wet and dry deposition
processes. The programmer analyst will assist authors contributing FACTs in other areas of Earth
Systemm Science, and will investigate the potential of new free document formats such as
DocBook and MathML.
</p><!--l. 444--><p class="indent">   By Years 4 and&#x00A0;5 the FACT project should be firmly established. The programmer will work to
increase hyperlinks and cross-references between existing FACTs. PI Zender will maintain and
improve his four FACTs and will solicit new FACTs in areas where there are still large gaps in the
Earth System Science curriculum.
</p><!--l. 451--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.9   </span> <a 
 id="x1-130003.9"></a>Project Evaluation</h4>
<!--l. 452--><p class="noindent">The success or failure of FACTs should be measured by the number of quality contributions
received and the number of people who read them. Assessing the first is relatively straightforward.
The number of newly contributed manuscripts and pages of improvements to existing manuscripts
can be tabulated annually. As with many websites, we will keep track of the number of visitors and
manuscript downloads. We will not be aware of second-generation users, e.g., a student who
receives a copy of the documentation (either paper or electronic) from a friend rather than directly
from the FACTs website.
</p><!--l. 463--><p class="noindent">
                                                                                         
                                                                                         
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.10   </span> <a 
 id="x1-140003.10"></a>Significance to Professional Goals and Responsibilities</h4>
<!--l. 464--><p class="noindent">Because of its international scope and availability to students of all income levels, the FACT
project may allow me and other geoscience educators to impact more students, and to a greater
depth, than we could possibly hope to before the advent of the Internet. The integration of FACTs
with my research interests and teaching responsibilities in the ESS department enhances its
likelihood of success.
</p><!--l. 472--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">3.11   </span> <a 
 id="x1-150003.11"></a>Prior Education, Outreach, and Service Accomplishments</h4>
<!--l. 474--><p class="noindent">
      </p><ol  class="enumerate1" >
      <li class="enumerate" value="1" 
><a 
 id="x1-15002x1"></a><span 
class="cmti-12">Development of Widely Distributed Geophysical Software</span>:  I  write  and  manage  the
      netCDF Operators (NCO) toolset (NCO works with HDF4, too). NCO is an Open
      Source  software  project  (<span class="obeylines-h"><a 
href="http://nco.sourceforge.net" class="url" ><span 
class="cmtt-12">http://nco.sourceforge.net</span></a></span>)  developing  free  tools  to
      manipulate  geophysical  datasets.  NCO  is  one  of  two  components  of  the  CCSM
      Component Model Processing Suite and is used daily by hundreds of geoscientists.
      </li>
      <li class="enumerate" value="2" 
><a 
 id="x1-15004x2"></a><span 
class="cmti-12">Undergraduate  Teaching</span>:  I  teach  ESS&#x00A0;20E:  &#x201C;The  Atmosphere&#x201D;,  an  undergraduate
      survey course with approximately 150 students. All course material is placed on the
      web (<span class="obeylines-h"><a 
href="http://eee.uci.edu/00s/42020" class="url" ><span 
class="cmtt-12">http://eee.uci.edu/00s/42020</span></a></span>), and the course includes web-based learning
      exercises. Students gave an overall grade of &#x201C;B&#x201D; to this course.
      </li>
      <li class="enumerate" value="3" 
><a 
 id="x1-15006x3"></a><span 
class="cmti-12">Mentoring of Undergraduates</span>: At the University of Colorado I founded and directed
      the Astrophysical, Planetary, Atmospheric Sciences Departmental Help Center, a free
      tutoring center which assisted dozens of undergraduates in the physical sciences every
      semester. My role included securing funding, tutoring, and managing a group of about
      10  paid  graduate  student  tutors.  This  activity  occurred  under  my  direction  from
      1992&#x2013;1995, and continued after my departure. Throughout this period I contributed
      to secondary school teaching by answering calls for to the Math and Science Teachers
      Hotline (1-800-866-MAST) organized by the University of Northern Colorado.</li></ol>
<!--l. 505--><p class="noindent">
</p>
   <h3 class="sectionHead"><span class="titlemark">4   </span> <a 
 id="x1-160004"></a>Enhanced Gaseous Absorption and Climate</h3>
<!--l. 507--><p class="noindent">
</p>
                                                                                         
                                                                                         
   <h4 class="subsectionHead"><span class="titlemark">4.1   </span> <a 
 id="x1-170004.1"></a>Overview</h4>
<!--l. 508--><p class="noindent">Absorption of radiant energy is the fundamental mechanism which drives the climate system. Thus
fully understanding the distribution of radiative absorption is essential to understanding climate.
Satellite-borne instruments have measured the Earth&#x2019;s global mean planetary albedo to be
<!--l. 513--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mn>3</mn><mn>0</mn> <mo 
class="MathClass-bin">&#x00B1;</mo> <mn>1</mn></math>%
[<a 
href="#XLMA97"><span 
class="cmti-12">Li et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XLMA97">1997</a>;&#x00A0;<a 
href="#XKiT97"><span 
class="cmti-12">Kiehl and Trenberth</span></a>,&#x00A0;<a 
href="#XKiT97">1997</a>]. The partitioning of the
<!--l. 514--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mn>7</mn><mn>0</mn> <mo 
class="MathClass-bin">&#x00B1;</mo> <mn>1</mn></math>%
absorbed between the atmosphere and the surface is very poorly constrained because
the spatio-temporal coverage of high quality surface observations is inadequate [<a 
href="#XWOG952"><span 
class="cmti-12">Wild</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XWOG952">1995</a>;&#x00A0;<a 
href="#XODF98"><span 
class="cmti-12">Ohmura et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XODF98">1998</a>;&#x00A0;<a 
href="#XGiO99"><span 
class="cmti-12">Gilgen and Ohmura</span></a>,&#x00A0;<a 
href="#XGiO99">1999</a>]. Until 1995 the consensus estimate
of the partitioning, based on models, was that the surface absorbed about 50% of incoming solar
radiation while the atmosphere absorbed the remaining 20%. Within the last six years, many
independent observational studies have concluded that Earth&#x2019;s atmosphere may absorb as
much as 28% of incoming solar radiation [e.g.,&#x00A0;<a 
href="#XCZM95"><span 
class="cmti-12">Cess et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XCZM95">1995</a>;&#x00A0;<a 
href="#XWOG952"><span 
class="cmti-12">Wild et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XWOG952">1995</a>;&#x00A0;<a 
href="#XLWC95"><span 
class="cmti-12">Li</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XLWC95">1995</a>,&#x00A0;&#x00A0;<a 
href="#XLMA97">1997</a>].
</p><!--l. 525--><p class="indent">   For our purposes this discrepancy between models and measurements of the atmospheric
absorbed radiation component of Earth&#x2019;s energy budget is called <span 
class="cmti-12">enhanced atmospheric</span>
<span 
class="cmti-12">absorption</span>, i.e., absorption by processes not represented in large scale atmospheric
models used for global studies and for climate prediction. Enhanced absorption
accounts for up to 8% of global annual mean incoming solar radiation, or about
25&#x00A0;W m<!--l. 531--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;[<a 
href="#XLMA97"><span 
class="cmti-12">Li</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XLMA97">1997</a>;&#x00A0;<a 
href="#XYZC99"><span 
class="cmti-12">Yu et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XYZC99">1999</a>]. Model climates are very sensitive to globally enhanced
atmospheric absorption of this magnitude [<a 
href="#XKHZ95"><span 
class="cmti-12">Kiehl et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XKHZ95">1995</a>;&#x00A0;<a 
href="#XCol00"><span 
class="cmti-12">Collins</span></a>,&#x00A0;<a 
href="#XCol00">2000</a>] so reducing
this discrepancy is crucial to improving prediction of climate and climate change. This
proposal concerns improving representation of known gaseous absorption mechanisms,
reducing the enhanced absorption discrepancy, and assessing the associated climate
response.
</p><!--l. 540--><p class="indent">   Large scale atmospheric models are known to underestimate gaseous absorption by
<!--l. 541--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 541--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
<!--l. 541--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>. This
project will include studies of the following processes which are known to contribute to enhanced
absorption: First, the sub-gridscale distribution of water vapor in clouds causes solar and terrestrial
radiation absorption biases [<a 
href="#XCri971"><span 
class="cmti-12">Crisp</span></a>,&#x00A0;<a 
href="#XCri971">1997</a>;&#x00A0;<a 
href="#XFuR99"><span 
class="cmti-12">Fung and Ramaswamy</span></a>,&#x00A0;<a 
href="#XFuR99">1999</a>]. Second, neglected
<!--l. 546--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;solar absorption
contributes about 1&#x00A0;W m<!--l. 546--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;to
the enhanced absorption [<a 
href="#XPEP97"><span 
class="cmti-12">Pfeilsticker et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XPEP97">1997</a>;&#x00A0;<a 
href="#XSPS98"><span 
class="cmti-12">Solomon et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XSPS98">1998</a>;&#x00A0;<a 
href="#XZen99"><span 
class="cmti-12">Zender</span></a>,&#x00A0;<a 
href="#XZen99">1999a</a>]. Third, neglected
<!--l. 548--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;solar
absorption causes an unknown, but potentially significant amount of enhanced absorption both in
the stratosphere and troposphere [<a 
href="#XZBP97"><span 
class="cmti-12">Zender et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XZBP97">1997</a>;&#x00A0;<a 
href="#XSPS99"><span 
class="cmti-12">Solomon et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XSPS99">1999</a>].
</p><!--l. 553--><p class="indent">   The proposal is organized as follows: Section&#x00A0;<a 
href="#x1-180004.2">4.2<!--tex4ht:ref: sxn:sw --></a> illustrates the spectral characteristics
of all significant gaseous shortwave absorbers. Sections <a 
href="#x1-190004.3">4.3<!--tex4ht:ref: sxn:h2o --></a>&#x2013;<a 
href="#x1-230004.5">4.5<!--tex4ht:ref: sxn:no2 --></a> describe the relevant
shortcomings of current representations of absorption in large scale atmospheric models due to
<!--l. 558--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 558--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
                                                                                         
                                                                                         
<!--l. 558--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>,
respectively. Section&#x00A0;<a 
href="#x1-240004.6">4.6<!--tex4ht:ref: sxn:sns --></a> summarizes how climate might respond to enhanced absorption. Sections
<a 
href="#x1-250004.7">4.7<!--tex4ht:ref: sxn:obj --></a>&#x2013;<a 
href="#x1-290004.10">4.10<!--tex4ht:ref: sxn:sgn --></a> describe our objectives and hypotheses, research plans, methods and procedures, and the
expected significance of the results, respectively.
</p><!--l. 565--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.2   </span> <a 
 id="x1-180004.2"></a>Shortwave Gaseous Absorption</h4>
<!--l. 566--><p class="noindent">Since the three absorption processes listed above involve solar absorption it is helpful to see the relative
spectral structure of all gaseous solar absorbers. Figure&#x00A0;<a 
href="#x1-180011">1<!--tex4ht:ref: fgr:odac --></a> shows the modeled absorption optical depth
<!--l. 570--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03C4;</mi><mstyle mathvariant="normal"><mi 
>a</mi><mi 
>b</mi><mi 
>s</mi></mstyle><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>&#x03BB;</mi></mrow><mo 
class="MathClass-close">)</mo></mrow></math> of all significant gaseous
solar absorbers for <!--l. 570--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mn>2</mn><mn>0</mn><mn>0</mn> <mo 
class="MathClass-rel">&#x003C;</mo> <mi 
>&#x03BB;</mi> <mo 
class="MathClass-rel">&#x003C;</mo> <mn>1</mn><mn>4</mn><mn>0</mn><mn>0</mn></math>&#x00A0;nm
at noontime on a pristine clear sky day in Oklahoma.
                                                                                         
                                                                                         
</p><!--l. 573--><p class="indent">   <a 
 id="x1-180011"></a></p><hr class="float" /><div class="float" 
><table class="float"><tr class="float"><td class="float" 
>
                                                                                         
                                                                                         
<div class="center" 
>
<!--l. 573--><p class="noindent">
</p><!--l. 575--><p class="noindent"><img 
src="prp_crr0x.png" alt="PIC" class="graphics" width="375.80542pt" height="354.08984pt"  /><!--tex4ht:graphics  
name="prp_crr0x.png" src="/data/zender/ps/odxc.eps"  
-->
</p>
</div>
<br />    <table class="caption" 
><tr style="vertical-align:baseline;" class="caption"><td class="id"><span 
class="cmbx-12">Figure</span><span 
class="cmbx-12">&#x00A0;1</span>:      </td><td  
class="content">Decomposition      of      simulated      absorption      optical      depth
<!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03C4;</mi><mstyle mathvariant="normal"><mi 
>a</mi><mi 
>b</mi><mi 
>s</mi></mstyle><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>&#x03BB;</mi></mrow><mo 
class="MathClass-close">)</mo></mrow></math>
at    the    ARM    CART    site    in    Oklahoma    at    local    solar    noontime    on
October    15,    1995    from    <a 
href="#XZen99"><span 
class="cmti-12">Zender</span></a>&#x00A0;[<a 
href="#XZen99">1999a</a>].    Gaseous    absorbers    included    are
<!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>O</mi><mn>2</mn></math>&#x00A0;(red),
<!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>N</mi><mn>2</mn></math>&#x00A0;(green),
<!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;(yellow),
<!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>3</mn></math>&#x00A0;(blue),
<!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn></math>&#x00A0;(light
blue), <!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;(light
green), and <!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>C</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;(black).
The line spectra of <!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>C</mi><mi 
>O</mi><mn>2</mn></math>,
and <!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn></math>&#x00A0;are
averaged over 10&#x00A0;<!--l. 585--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><!--mstyle 
class="mbox"--><mtext  >&#x00A0;cm</mtext><!--/mstyle--><mo 
class="MathClass-bin">&#x2212;</mo><mn>1</mn></math>.
                                                                                         
                                                                                         
</td></tr></table><!--tex4ht:label?: x1-180011 -->
                                                                                         
                                                                                         
   </td></tr></table></div><hr class="endfloat" />
<!--l. 587--><p class="indent">   <a 
href="#XZBP97"><span 
class="cmti-12">Zender et</span><span 
class="cmti-12">&#x00A0;al.</span></a>&#x00A0;[<a 
href="#XZBP97">1997</a>] describe the multistream narrow band
(10&#x00A0;<!--l. 587--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><!--mstyle 
class="mbox"--><mtext  >&#x00A0;cm</mtext><!--/mstyle--><mo 
class="MathClass-bin">&#x2212;</mo><mn>1</mn></math>)
radiative transfer model, the experimental uncertainties, and all the input data in more detail.
Structured or continuum absorption is present at nearly all wavelengths except in the neighborhood of
0.86&#x00A0;<!--l. 591--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03BC;</mi><!--mstyle 
class="mbox"--><mtext  >&#x00A0;m</mtext><!--/mstyle--></math>.
<!--l. 593--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;shares
with <!--l. 593--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;the
distinction of overlapping with all the significant solar absorbers. However, the strongest bands of
<!--l. 595--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 595--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
<!--l. 595--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;are
largely independent of one another. Currently all large scale atmospheric models account for most
<!--l. 597--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;(yellow) absorption, but none
include absorption by <!--l. 598--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;(red
and dark green) or <!--l. 599--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;(light
green centered near 0.4&#x00A0;<!--l. 599--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03BC;</mi><!--mstyle 
class="mbox"--><mtext  >&#x00A0;m</mtext><!--/mstyle--></math>).
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.3   </span> <a 
 id="x1-190004.3"></a>Absorption by Water Vapor</h4>
<!--l. 602--><p class="noindent">Correct representation of water vapor absorption at all wavelengths is critical to climate studies because
<!--l. 603--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;is both the
dominant solar absorber and greenhouse gas in Earth&#x2019;s atmosphere. Models predict that, globally averaged,
gaseous <!--l. 605--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;absorbs
about 72% and 55% of incident solar radiation in clear and cloudy atmospheres, respectively [<a 
href="#XKiT97"><span 
class="cmti-12">Kiehl</span>
<span 
class="cmti-12">and Trenberth</span></a>,&#x00A0;<a 
href="#XKiT97">1997</a>]. This absorption is maximized in humid regions above bright surfaces.
Regions of persistent marine stratus such as offshore of California, Peru, and Namibia produce the
greatest solar absorption by water vapor.
</p><!--l. 613--><p class="indent">   Water vapor accounts for about 55-60% of the total reduction in emission
of terrestrial radiation to space (the &#x201C;greenhouse effect&#x201D;) in both clear and
cloudy skies [<a 
href="#XKiT97"><span 
class="cmti-12">Kiehl and Trenberth</span></a>,&#x00A0;<a 
href="#XKiT97">1997</a>]. The strongest longwave forcing by
<!--l. 616--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;occurs
in the upper troposphere [<a 
href="#XRaR892"><span 
class="cmti-12">Raval and Ramanathan</span></a>,&#x00A0;<a 
href="#XRaR892">1989</a>;&#x00A0;<a 
href="#XKiB92"><span 
class="cmti-12">Kiehl and Briegleb</span></a>,&#x00A0;<a 
href="#XKiB92">1992</a>;&#x00A0;<a 
href="#XLub94"><span 
class="cmti-12">Lubin</span></a>,&#x00A0;<a 
href="#XLub94">1994</a>]
where it plays a role in maintaining deep convection [<a 
href="#XSoF95"><span 
class="cmti-12">Soden and Fu</span></a>,&#x00A0;<a 
href="#XSoF95">1995</a>]. Upper tropospheric
absolute humidity may increase in warmer climates due to the water-vapor feedback, although
there are exceptions to this reasoning [<a 
href="#XLin902"><span 
class="cmti-12">Lindzen</span></a>,&#x00A0;<a 
href="#XLin902">1990</a>].
</p><!--l. 623--><p class="indent">   Line-by-line radiative transfer models obtain excellent agreement with the measured
structure of water vapor monomer absorption [e.g.,&#x00A0;<a 
href="#XMCB98"><span 
class="cmti-12">Mlawer et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XMCB98">1998</a>;&#x00A0;<a 
href="#XDSS99"><span 
class="cmti-12">Daniel</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XDSS99">1999</a>] so there is little systematic error in the tabulated line strengths of the
<!--l. 626--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;monomer
[<a 
href="#XRRG98"><span 
class="cmti-12">Rothman et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XRRG98">1998</a>]. Unfortunately large scale atmospheric models (henceforth general
circulation models, GCMs, for concreteness) must make approximations to reduce the
computational burden of predicting radiative fluxes. One such approximation made by all radiative
                                                                                         
                                                                                         
parameterizations in GCMs (to our knowledge) is that the specific humidity within
clouds equals the gridbox mean specific humidity rather than the saturated specific
humidity. Thus GCMs neglect the sub-gridscale distribution of water vapor caused by
clouds.
</p><!--l. 638--><p class="indent">   The sub-gridscale <!--l. 638--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;distribution
caused by clouds is neglected for two reasons. First, the alternative requires multiple forward
radiative transfer calculations. The ideal method for computing radiative fluxes for a column
containing a single layer cloud would be to perform two radiative transfer calculations: one for the
saturated, cloudy fraction of the gridcell, and one for the sub-saturated clear portion of
the gridcell and weight the resulting fluxes by the respective areas of each. This time
consuming procedure for one cloudy layer is the simplest example of the independent pixel
approximation (IPA). However, this method becomes exorbitantly expensive for GCMs as
the number of cloudy layers increases because a separate radiative calculation must be
perform for each vertical overlap geometry matching the cloud overlap criteria (e.g.,
maximum overlap, random overlap) [e.g.,&#x00A0;<a 
href="#XCSH98"><span 
class="cmti-12">Chou et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XCSH98">1998</a>]. The second reason is that the
effects of cloud scattering and absorption are much larger than the error caused by the
approximation.
</p><!--l. 658--><p class="indent">   <a 
href="#XCri971"><span 
class="cmti-12">Crisp</span></a>&#x00A0;[<a 
href="#XCri971">1997</a>] estimates that 20% of in-cloud absorption in a typical mid-latitude summer
stratocumulus cloud is caused by vapor pressure difference between the cloud and its environment.
This is consistent with <a 
href="#XFuR99"><span 
class="cmti-12">Fung and Ramaswamy</span></a>&#x00A0;[<a 
href="#XFuR99">1999</a>] who studied the dependence of this enhanced
water vapor absorption on cloud liquid water path and droplet effective radius. Some of this
enhanced absorption is offset by reduced water vapor absorption in the now-drier environment
(which has supplied the vapor required to saturate the clouds). However this offset is very small
because much of the increased transmission through the sub-saturated environment is absorbed
lower in the atmosphere.
</p><!--l. 671--><p class="indent">   Based on these studies and our own calculations, we expect that neglect of the sub-gridscale
<!--l. 672--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;distribution
contributes 1&#x2013;2&#x00A0;W m<!--l. 673--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;to
the global and annual solar radiative budget discrepancy. Moreover, this enhanced absorption
mechanism causes models to systematically underpredict in-cloud absorption and so contributes to
cloudy sky solar absorption discrepancies observed at global scales [<a 
href="#XCZM95"><span 
class="cmti-12">Cess et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XCZM95">1995</a>;&#x00A0;<a 
href="#XWOG952"><span 
class="cmti-12">Wild</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XWOG952">1995</a>;&#x00A0;<a 
href="#XCol98"><span 
class="cmti-12">Collins</span></a>,&#x00A0;<a 
href="#XCol98">1998</a>]. Possible dynamical consequences of the bias are discussed in
<span 
class="cmsy-10x-x-120">&#x00A7;</span>&#x00A0;<a 
href="#x1-240004.6">4.6<!--tex4ht:ref: sxn:sns --></a>.
</p><!--l. 682--><p class="indent">   Longwave absorption and emission are also affected by the sub-gridscale
<!--l. 683--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;distribution in
cloudy atmospheres. Water vapor transmission (and thus absorption) vary approximately exponentially with
the pressure-weighted water vapor mass path. Thus the linear rearrangement required to segregate gridbox
mean <!--l. 686--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;into
saturated clouds and sub-saturated environments for radiative purposes will cause non-linear
responses in the transmission and absorption, and hence longwave radiative fluxes. Because GCM
clouds are not treated as saturated, they are less emissive at cloud top and cloud top
cooling is artificially reduced, as is heating of the layer immediately above cloud top. This
systematically reduces the outgoing longwave radiation in cloudy atmospheres. Our preliminary
calculations show this artificial enhancement of the greenhouse effect is typically order
1&#x00A0;W m<!--l. 696--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;for
                                                                                         
                                                                                         
medium to high clouds. Dynamical implications of this bias are discussed in <span 
class="cmsy-10x-x-120">&#x00A7;</span>&#x00A0;<a 
href="#x1-250004.7">4.7<!--tex4ht:ref: sxn:obj --></a>.
</p><!--l. 700--><p class="noindent">
</p>
   <h5 class="subsubsectionHead"><span class="titlemark">4.3.1   </span> <a 
 id="x1-200004.3.1"></a>Water Vapor Continuum Absorption</h5>
<!--l. 701--><p class="noindent">GCMs do not include contributions to solar absorption from the far wings
of water vapor lines. This continuum absorption may account for up to
1&#x00A0;W m<!--l. 703--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;[<a 
href="#XCri971"><span 
class="cmti-12">Crisp</span></a>,&#x00A0;<a 
href="#XCri971">1997</a>],
and is adequately constrained by observational studies [<a 
href="#XVRC981"><span 
class="cmti-12">Vogelmann et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XVRC981">1998</a>]. We will extend
water vapor vapor continuum effect into the near infrared using the most the most recently
updated continuum of <a 
href="#XCKD89"><span 
class="cmti-12">Clough et</span><span 
class="cmti-12">&#x00A0;al.</span></a>&#x00A0;[<a 
href="#XCKD89">1989</a>].
</p><!--l. 710--><p class="noindent">
</p>
   <h5 class="subsubsectionHead"><span class="titlemark">4.3.2   </span> <a 
 id="x1-210004.3.2"></a>Water Vapor Dimer Absorption</h5>
<!--l. 711--><p class="noindent">The water vapor dimer <!--l. 711--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>&#x00A0;may
cause significant structured absorption at visible wavelengths [<a 
href="#XChG97"><span 
class="cmti-12">Ch</span><span 
class="cmti-12">&#x00FD;</span><span 
class="cmti-12">lek and Geldart</span></a>,&#x00A0;<a 
href="#XChG97">1997</a>]. The absorption
cross section of <!--l. 713--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>,
<!--l. 713--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03B1;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>, is
very difficult to measure so researchers have instead resorted to <span 
class="cmti-12">ab initio </span>models for determining
<!--l. 715--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03B1;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math> [<a 
href="#XTGC98"><span 
class="cmti-12">Tso et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XTGC98">1998</a>].
The predicted <!--l. 716--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03B1;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>
are very uncertain in exact absorption band location, but less so in integrated absorption strength.
Based on these values, <a 
href="#XZeC98"><span 
class="cmti-12">Zender and Ch</span><span 
class="cmti-12">&#x00FD;</span><span 
class="cmti-12">lek</span></a>&#x00A0;[<a 
href="#XZeC98">1998</a>] showed the global annual mean absorption from
<!--l. 719--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>&#x00A0;was about
1&#x00A0;W m<!--l. 719--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>.
However, high precision field measurements [<a 
href="#XDSS99"><span 
class="cmti-12">Daniel et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XDSS99">1999</a>, S.&#x00A0;Clough,
personal communication, 1998] cast doubt on the validity the <a 
href="#XTGC98"><span 
class="cmti-12">Tso et</span><span 
class="cmti-12">&#x00A0;al.</span></a>&#x00A0;[<a 
href="#XTGC98">1998</a>]
<!--l. 722--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03B1;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>. It would be premature
to include <!--l. 723--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>&#x00A0;absorption
in production climate prediction models until uncertainty in
<!--l. 724--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03B1;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math> is reduced
and the <!--l. 725--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03B1;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>
employed can be observationally validated. We remain open to quantifying
<!--l. 727--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>&#x00A0;absorption
should these advances occur.
</p><!--l. 730--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.4   </span> <a 
 id="x1-220004.4"></a>Absorption by Collision Complexes of Oxygen</h4>
                                                                                         
                                                                                         
<!--l. 731--><p class="noindent">Three recent high quality laboratory experiments directly measured the binary cross-sections for
<!--l. 732--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;absorption,
<!--l. 732--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03C3;</mi><mi 
>b</mi>
<mstyle mathvariant="normal"><mi 
>O</mi></mstyle><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mstyle mathvariant="normal"><mi 
>X</mi></mstyle></math>
[<a 
href="#XGOB90"><span 
class="cmti-12">Greenblatt et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XGOB90">1990</a>;&#x00A0;<a 
href="#XNeB98"><span 
class="cmti-12">Newnham and Ballard</span></a>,&#x00A0;<a 
href="#XNeB98">1998</a>;&#x00A0;<a 
href="#XSmN00"><span 
class="cmti-12">Smith and Newnham</span></a>,&#x00A0;<a 
href="#XSmN00">2000</a>]. In addition,
measured <!--l. 734--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03C3;</mi><mi 
>b</mi>
<mstyle mathvariant="normal"><mi 
>O</mi></mstyle><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mstyle mathvariant="normal"><mi 
>X</mi></mstyle></math>
has been inferred and evaluated in two high-precision field studies [<a 
href="#XSPS98"><span 
class="cmti-12">Solomon et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XSPS98">1998</a>;&#x00A0;<a 
href="#XMCB98"><span 
class="cmti-12">Mlawer</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XMCB98">1998</a>].
</p><!--l. 737--><p class="indent">   <a 
href="#XZen99"><span 
class="cmti-12">Zender</span></a>&#x00A0;[<a 
href="#XZen99">1999a</a>] used the available measurements to study the regional, vertical, seasonal, and annual patterns
of <!--l. 738--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;abundance
and radiative forcing in a general circulation model (GCM). He showed that
<!--l. 740--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;absorbs about
1&#x00A0;W m<!--l. 740--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;globally
annually averaged, with no significant difference between clear and cloudy skies.
<!--l. 743--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;absorption has
strong vertical and regional gradients. These are due to the quadratic dependence of the heating on concentrations
of <!--l. 745--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn></math>&#x00A0;and
<!--l. 745--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mn>2</mn></math>&#x00A0;(i.e.,
air density), and to the regional distributions of reflective surfaces (e.g., stratus clouds, snow/ice,
and bright desert).
</p><!--l. 749--><p class="indent">   The results already obtained for <!--l. 749--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;forcing
of climate illustrate some of the vertical, seasonal, and geographic characteristics we will examine for
<!--l. 751--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;and
<!--l. 751--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;heating
biases. Figure&#x00A0;<a 
href="#x1-220012">2<!--tex4ht:ref: fgr:O2O2_O2N2_csn_avg --></a>a shows the simulated JJA average radiative forcing of
<!--l. 753--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>.
</p><hr class="figure" /><div class="figure" 
><table class="figure"><tr class="figure"><td class="figure" 
>
                                                                                         
                                                                                         
<a 
 id="x1-220012"></a>
                                                                                         
                                                                                         
<div class="center" 
>
<!--l. 755--><p class="noindent">
</p><!--l. 756--><p class="noindent"><img 
src="prp_crr1x.png" alt="PIC" class="graphics" width="234.87749pt" height="155.07936pt"  /><!--tex4ht:graphics  
name="prp_crr1x.png" src="/data/zender/fgr/dmr/dmr04_8589_0608_FSATFRC_ARM98.eps"  
--><img 
src="prp_crr2x.png" alt="PIC" class="graphics" width="234.87749pt" height="160.09811pt"  /><!--tex4ht:graphics  
name="prp_crr2x.png" src="/data/zender/fgr/dmr/dmr04_8589_0608_x_QRSFRC_ARM98.eps"  
--></p></div>
<br /> <table class="caption" 
><tr style="vertical-align:baseline;" class="caption"><td class="id"><span 
class="cmbx-12">Figure</span><span 
class="cmbx-12">&#x00A0;2</span>:  </td><td  
class="content">Seasonal  mean  instantaneous  radiative  forcing  in  Northern  Summer  (JJA
average) due to <!--l. 764--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>O</mi><mn>2</mn> <mo 
class="MathClass-bin">+</mo> <mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>N</mi><mn>2</mn></math>
from <a 
href="#XZen99"><span 
class="cmti-12">Zender</span></a>&#x00A0;[<a 
href="#XZen99">1999a</a>]. (a) Atmospheric absorption (W m<!--l. 764--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>).
(b) Heating rate (<!--l. 764--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" > <mo 
class="MathClass-bin">&#x00D7;</mo> <mn>1</mn><msup><mrow 
><mn>0</mn></mrow><mrow 
><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></mrow></msup 
></math>&#x00A0;K day<!--l. 764--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>1</mn></math>)
</td></tr></table><!--tex4ht:label?: x1-220012 -->
                                                                                         
                                                                                         
   </td></tr></table></div><hr class="endfigure" />
<!--l. 766--><p class="indent">   Surface albedo and cloud vertical location play a stronger role than anticipated in modulating enhanced
absorption by <!--l. 767--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>.
These factors will also be very important for enhanced
<!--l. 768--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;and
<!--l. 768--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption. The climate
response to <!--l. 770--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;forcing
remains unknown, although from the forcing pattern it appears likely that the strongest response
will occur in summertime polar regions.
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.5   </span> <a 
 id="x1-230004.5"></a>Absorption by Nitrogen Dioxide</h4>
<!--l. 775--><p class="noindent">Accurate,  high  spectral  resolution
<!--l. 775--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;cross-sections
<!--l. 775--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03C3;</mi><mstyle mathvariant="normal"><mi 
>N</mi><mi 
>O</mi></mstyle><mn>2</mn></math> [<a 
href="#XHBJ97"><span 
class="cmti-12">Harder et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XHBJ97">1997</a>]
allow <!--l. 776--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption
to be computed when its distribution is known. Long term measurements of stratospheric
<!--l. 778--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;concentration
are available from the SAGE measurements. However, there are no credible estimates of global forcing by
<!--l. 780--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;yet because
its tropospheric distribution is highly variable and uncertain [<a 
href="#XEmm97"><span 
class="cmti-12">Emmons</span></a>,&#x00A0;<a 
href="#XEmm97">1997</a>]. Significant sources
of <!--l. 783--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mi 
>x</mi></math>&#x00A0;to
the troposphere include pollution events, soils, and lightning [<a 
href="#XSeP97"><span 
class="cmti-12">Seinfeld and Pandis</span></a>,&#x00A0;<a 
href="#XSeP97">1997</a>;&#x00A0;<a 
href="#XPPP971"><span 
class="cmti-12">Price</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XPPP971">1997</a>], all of which are sensitive to anthropogenic influences [<a 
href="#XSPS99"><span 
class="cmti-12">Solomon et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XSPS99">1999</a>].
</p><!--l. 787--><p class="indent">   <a 
href="#XSPS99"><span 
class="cmti-12">Solomon et</span><span 
class="cmti-12">&#x00A0;al.</span></a>&#x00A0;[<a 
href="#XSPS99">1999</a>]  demonstrated  that
<!--l. 787--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mi 
>x</mi></math>&#x00A0;produced by
lightning and pollution can significantly increase the atmospheric absorptance in cloudy as well as clear skies.
In the presence of <!--l. 790--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>3</mn></math>,
<!--l. 790--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mi 
>x</mi></math>&#x00A0;quickly establishes a photochemical
equilibrium between <!--l. 791--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi></math>&#x00A0;and
<!--l. 791--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>. Absorption
by <!--l. 792--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;from
lightning and pollution caused peak instantaneous noontime radiative forcings of
5&#x2013;30&#x00A0;W m<!--l. 793--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;in
Boulder, Colorado [<a 
href="#XSPS99"><span 
class="cmti-12">Solomon et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XSPS99">1999</a>]. The forcing of
<!--l. 795--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;from
lightning is strongly sensitive to the vertical distribution of the
<!--l. 796--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;relative to
cloud top.
</p><!--l. 809--><p class="noindent">
</p>
                                                                                         
                                                                                         
   <h4 class="subsectionHead"><span class="titlemark">4.6   </span> <a 
 id="x1-240004.6"></a>Climate Sensitivity to Enhanced Absorption</h4>
<!--l. 810--><p class="noindent">The climate sensitivity to enhanced absorption will remain unknown until and unless causal
mechanisms are identified. Some qualitative effects are known from physical reasoning and climate
sensitivity experiments. Enhanced absorption introduces an artificial bias where models allow solar
energy to be absorbed by the surface instead of in the atmosphere. This artificially
heats the surface, destabilizes the boundary layer, and enhances sensible and latent heat
transfer. Climate sensitivity studies to prescribed enhanced absorption in clouds show
significant responses in the latent heat and wind fields, especially in the tropics [<a 
href="#XKHZ95"><span 
class="cmti-12">Kiehl</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XKHZ95">1995</a>]. Fully coupled simulations show enhanced absorption in clouds improves tropical
sea surface temperature and latent heat predictions relative to tropical observations
[<a 
href="#XCol00"><span 
class="cmti-12">Collins</span></a>,&#x00A0;<a 
href="#XCol00">2000</a>]. In our experiments of climate sensitivity to enhanced gaseous absorption by
<!--l. 825--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 825--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
<!--l. 825--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>, we
will look for similarities and differences with these previous studies.
</p><!--l. 828--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.7   </span> <a 
 id="x1-250004.7"></a>Objectives and Hypotheses</h4>
<!--l. 831--><p class="noindent">
      </p><ol  class="enumerate1" >
      <li class="enumerate" value="1" 
><a 
 id="x1-25002x1"></a><a 
 id="x1-25003r1"></a> <span 
class="cmbx-12">Objective</span>: Integrate all significant gaseous absorption from <!--l. 833--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
      <!--l. 833--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>,
      and <!--l. 833--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;into
      our understanding and representation of the solar energy budget.
      <br class="newline" /><span 
class="cmbx-12">Hypothesis</span>: Enhanced solar absorption by <!--l. 835--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
      <!--l. 835--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>,
      and <!--l. 836--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;is
      3&#x2013;8&#x00A0;W m<!--l. 836--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;
      <br class="newline" />Forcing by <!--l. 837--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;is
      about 0.75&#x2013;1.2&#x00A0;W m<!--l. 837--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;[<a 
href="#XZBP97"><span 
class="cmti-12">Zender</span>
      <span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XZBP97">1997</a>] so the large uncertainty in the total range is due to the unpredictable
      magnitudes of absorption due to <!--l. 839--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;and
      <!--l. 839--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>.
      Accounting for saturated <!--l. 840--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;in
      clouds increases total solar absorption predictably for a given column [<a 
href="#XCri971"><span 
class="cmti-12">Crisp</span></a>,&#x00A0;<a 
href="#XCri971">1997</a>;&#x00A0;<a 
href="#XFuR99"><span 
class="cmti-12">Fung</span>
      <span 
class="cmti-12">and Ramaswamy</span></a>,&#x00A0;<a 
href="#XFuR99">1999</a>]. However, this effect must be integrated over the global vertical
      distribution of clouds and other radiative boundary conditions. The extent to which
      total water vapor absorption is vertically redistributed, rather than increased, is unpredictable.
      </li>
      <li class="enumerate" value="2" 
><a 
 id="x1-25005x2"></a><a 
 id="x1-25006r2"></a> <span 
class="cmbx-12">Objective</span>: Quantify the role of clouds in increasing or diminishing enhanced absorption
      by <!--l. 849--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
      <!--l. 849--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>,
                                                                                         
                                                                                         
      <!--l. 849--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>
      <br class="newline" /><span 
class="cmbx-12">Hypothesis</span>: Saturated in-cloud <!--l. 850--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;and
      <!--l. 850--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;will
      preferentially increase cloudy sky absorption relative to clear sky absorption
      <br class="newline" /><a 
href="#XZen99"><span 
class="cmti-12">Zender</span></a>&#x00A0;[<a 
href="#XZen99">1999a</a>] showed that, globally averaged, <!--l. 853--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;enhances
      absorption equally in clear and in cloudy skies. Two key mechanisms in the proposed
      study, however, concern absorption by trace gases in (and near) clouds. Saturated water
      vapor in clouds, in conjunction with <!--l. 857--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;from
      thunderstorms, are both likely to enhance cloudy sky absorption relative to clear sky
      absorption.
      </li>
      <li class="enumerate" value="3" 
><a 
 id="x1-25008x3"></a><a 
 id="x1-25009r3"></a> <span 
class="cmbx-12">Objective</span>: Compare and contrast the regional, seasonal, and vertical characteristics of
      enhanced absorption by <!--l. 863--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
      <!--l. 863--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>,
      and <!--l. 864--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>
      <br class="newline" /><span 
class="cmbx-12">Hypothesis</span>: Enhanced solar heating by <!--l. 865--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;will
      peak in the tropics near 600&#x00A0;mb
      <br class="newline" />Like <!--l. 867--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;(Figure&#x00A0;<a 
href="#x1-220012">2<!--tex4ht:ref: fgr:O2O2_O2N2_csn_avg --></a>b),
      <!--l. 867--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;concentration
      decreases monotonically from the surface, but <!--l. 868--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;is
      concentrated in the tropics. Cloud screening ensures that virtually all of the enhanced
      <!--l. 870--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;absorption
      will occur at cloud top, so the peak <!--l. 871--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;absorption
      bias should be above the peak <!--l. 872--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;bias.
      The geographic distribution of tropospheric <!--l. 873--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;forcing
      will be quite distinct from <!--l. 874--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;and
      <!--l. 874--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>.
      Tropospherice <!--l. 875--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;forcing
      should show large land-sea, urban-rural, and tropical-extratropical contrasts due to the
      distributions of lightning, soils, and pollution.
      </li>
      <li class="enumerate" value="4" 
><a 
 id="x1-25011x4"></a><a 
 id="x1-25012r4"></a> <span 
class="cmbx-12">Objective</span>: Investigate the dynamical response to absorption by the (currently neglected)
      saturated water vapor and <!--l. 881--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;within
      clouds
      <br class="newline" /><span 
class="cmbx-12">Hypothesis #1</span>: The longwave effects of in-cloud saturation suppress the vertical
      development of deep convection
      <br class="newline" />The enhanced concentration of water vapor within clouds increases their emissivity,
      causing cloud tops to cool to space more efficiently. Moreover, the reduced <!--l. 888--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;concentration
      in the surrounding sub-saturated environment is more transmissive to thermal radiation
      from  below.  In  conjunction  these  effects  enhance  cooling  at  cloud  top  and  reduce
      heating immediately above cloud top and so act to stabilize the vertical region near
      the cloud top, i.e., to suppress convection.
      <br class="newline" /><span 
class="cmbx-12">Hypothesis #2</span>: The solar effects of in-cloud saturation enhance the vertical development
      of convection
      <br class="newline" />Allowing the saturated in-cloud water vapor to absorb shortwave radiation will enhance
                                                                                         
                                                                                         
      solar heating in the upper layers of clouds. This will compensate, to an extent, the
      longwave effects of in-cloud vapor absorption described above. The degree of compensation
      will depend on cloud type, zenith angle, and vertical location. <!--l. 902--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;from
      lightning is also expected to heat cloud tops and enhance the vertical development of
      convection.
      </li>
      <li class="enumerate" value="5" 
><a 
 id="x1-25014x5"></a><a 
 id="x1-25015r5"></a> <span 
class="cmbx-12">Objective</span>: Quantify the climate response to <!--l. 906--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;heating
      <br class="newline" /><span 
class="cmbx-12">Hypothesis</span>: <!--l. 907--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;increases
      the temperature at the polar tropopause by <!--l. 908--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" > <mo 
class="MathClass-rel">&#x223C;</mo> <mn>1</mn></math>&#x00A0;K
      <br class="newline" />Single-column simulations show the radiative relaxation timescale at the polar tropopause
      is <!--l. 910--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" > <mo 
class="MathClass-rel">&#x223C;</mo> <mn>5</mn><mn>0</mn></math>&#x00A0;days.
      <!--l. 911--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;heating
      of the summertime polar tropopause is <!--l. 911--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" > <mo 
class="MathClass-rel">&#x223C;</mo> <mn>0</mn><mo 
class="MathClass-punc">.</mo><mn>0</mn><mn>1</mn></math>&#x00A0;K d<!--l. 911--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>1</mn></math>&#x00A0;(Figure&#x00A0;<a 
href="#x1-220012">2<!--tex4ht:ref: fgr:O2O2_O2N2_csn_avg --></a>b),
      which should increase the radiative equilibrium temperature by <!--l. 913--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" > <mo 
class="MathClass-rel">&#x223C;</mo> <mn>1</mn></math>&#x00A0;K.
      </li>
      <li class="enumerate" value="6" 
><a 
 id="x1-25017x6"></a><a 
 id="x1-25018r6"></a> <span 
class="cmbx-12">Objective</span>: Assess the role of <!--l. 916--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption
      in warming the stratosphere
      <br class="newline" /><span 
class="cmbx-12">Hypothesis</span>: <!--l. 918--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption
      warms the polar stratosphere
      <br class="newline" />Many GCMs have strong (up to 10&#x2013;14&#x00A0;K) cold biases at and above the summertime
      polar tropopause [<a 
href="#XHKH98"><span 
class="cmti-12">Hack et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XHKH98">1998</a>]. <!--l. 921--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;heating
      will have a maximum in the summer polar stratosphere. Stratospheric air density is very
      low so even a modest forcing (0.5&#x00A0;W m<!--l. 923--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>)
      can change its equilibrium temperature.
      </li></ol>
<!--l. 952--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.8   </span> <a 
 id="x1-260004.8"></a>Research Plans</h4>
<!--l. 953--><p class="noindent">All of our objectives (<span 
class="cmsy-10x-x-120">&#x00A7;</span><a 
href="#x1-250004.7">4.7<!--tex4ht:ref: sxn:obj --></a>) depend on successfully importing new radiative processes and procedures
for <!--l. 954--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 954--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
<!--l. 955--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;into a
3-D atmospheric general circulation model (GCM). The first three of our objectives (<span 
class="cmsy-10x-x-120">&#x00A7;</span><a 
href="#x1-250004.7">4.7<!--tex4ht:ref: sxn:obj --></a>) will be
met by analyzing the results of diagnostic GCM forcing simulations of one or two years in length.
The GCM will be driven by climatological sea surface temperatures so that the diagnostic
forcing by enhanced gaseous absorption is climatologically representative. Objectives <a 
href="#x1-25012r4">4<!--tex4ht:ref: idx_obj_htg_h2o --></a>&#x2013;<a 
href="#x1-25018r6">6<!--tex4ht:ref: idx_obj_no2_htg --></a>
will require long term (about 15&#x00A0;year) feedback experiments with AMIP SSTs as well
as in a fully coupled Climate System Model. Long term integrations are essential to
isolating the climate response signal from the noise of natural variability, especially in polar
regions.
</p><!--l. 969--><p class="indent">   Finally we would like to assess the change in enhanced absorption of of
<!--l. 970--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;and
                                                                                         
                                                                                         
<!--l. 970--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;expected
between now and the Year&#x00A0;2100. The influence of a warmer climate on
<!--l. 971--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;and of anthropogenic and
natural changes in <!--l. 972--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mi 
>x</mi></math>&#x00A0;sources
may cause their absorption to change significantly.
</p><!--l. 975--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.9   </span> <a 
 id="x1-270004.9"></a>Methods and Procedures</h4>
<!--l. 976--><p class="noindent">We will use the NCAR Community Atmosphere and Climate System Models (CAM and CCSM) [<a 
href="#XKHB98"><span 
class="cmti-12">Kiehl</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XKHB98">1998</a>;&#x00A0;<a 
href="#XBoG98"><span 
class="cmti-12">Boville and Gent</span></a>,&#x00A0;<a 
href="#XBoG98">1998</a>] for climate forcing and sensitivity studies with enhance
<!--l. 978--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 978--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
<!--l. 978--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption.
To represent the radiative effects of the sub-gridscale distribution of
<!--l. 980--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;in
cloud atmospheres, a radiative transfer procedure must segregate the clear sky humidity field
<!--l. 981--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>q</mi><mstyle mathvariant="normal"><mi 
>c</mi></mstyle></math> from the in-cloud
humidity field <!--l. 982--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>q</mi><mi 
>s</mi></math> such that
total gridcell humidity <!--l. 983--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mover 
accent="true"><mrow 
><mi 
>q</mi></mrow><mo 
class="MathClass-op">&#x0304;</mo></mover></math>
is conserved. We will modify a new generalized framework for treating cloud overlap developed by
W.&#x00A0;Collins of NCAR which makes this segregation as economical as possible. For a gridbox with horizontal
cloud fraction <!--l. 987--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>A</mi><mi 
>H</mi></math>,
the subgridscale humidity fields will be related by
</p>
   <table 
class="equation"><tr><td>
<!--tex4ht:inline--><!--l. 989--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="block" >
                                 <mstyle 
   id="x1-27001r1"  class="label" ></mstyle><!--endlabel--><mrow ><mo 
class="MathClass-open">(</mo><mrow><mn>1</mn> <mo 
class="MathClass-bin">&#x2212;</mo> <mi 
>A</mi><mi 
>H</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mi 
>q</mi><mstyle mathvariant="normal"><mi 
>c</mi></mstyle> <mo 
class="MathClass-bin">+</mo> <mi 
>A</mi><mi 
>H</mi><mi 
>q</mi><mi 
>s</mi> <mo 
class="MathClass-rel">=</mo> <mover 
accent="true"><mrow 
><mi 
>q</mi></mrow><mo 
class="MathClass-op">&#x0304;</mo></mover>
</math>
<!--l. 992--><p class="nopar"></p></td><td class="eq-no">(1)</td></tr></table>
<!--l. 992--><p class="nopar">
Since clouds are very near saturation with respect to the cloud temperature
<!--l. 994--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>T</mi></math> theoretically
<!--l. 994--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>q</mi><mi 
>s</mi> <mo 
class="MathClass-rel">=</mo> <mi 
>q</mi><mi 
>s</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>T</mi></mrow><mo 
class="MathClass-close">)</mo></mrow></math>. In practice, however,
GCMs allow <!--l. 995--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>A</mi><mi 
>H</mi> <mo 
class="MathClass-rel">=</mo> <mn>1</mn></math> when
gridcell relative humidity <!--l. 996--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><!--mstyle 
class="mbox"--><mtext  >&#x00A0;RH</mtext><!--/mstyle--> <mo 
class="MathClass-rel">&#x003C;</mo> <mn>1</mn><mn>0</mn><mn>0</mn><mi 
>%</mi></math>
                                                                                         
                                                                                         
[e.g.,&#x00A0;<a 
href="#XKHB98"><span 
class="cmti-12">Kiehl et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XKHB98">1998</a>]. In other words, a horizontally overcast gridbox is not necessarily
saturated through its entire volume. This small complication to (<a 
href="#x1-27001r1">1<!--tex4ht:ref: eqn:spchmdbdg --></a>) should be easily
surmountable.
</p><!--l. 1002--><p class="indent">   A sophisticated, high resolution (10&#x00A0;<!--l. 1002--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><!--mstyle 
class="mbox"--><mtext  >&#x00A0;cm</mtext><!--/mstyle--><mo 
class="MathClass-bin">&#x2212;</mo><mn>1</mn></math>)
offline radiative transfer model [<a 
href="#XZBP97"><span 
class="cmti-12">Zender et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XZBP97">1997</a>] will be used to parameterize
<!--l. 1003--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;and
<!--l. 1003--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption
cross-sections for use in the GCM. In order to quantify the radiative forcing due to
<!--l. 1005--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;one
needs to know its distribution in the troposphere. This appears to be the most difficult
portion of the entire project. As a first step we will use the global monthly daytime mean
<!--l. 1009--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;concentration
dataset predicted by the MOZART Chemical Transport Model (CTM)
[<a 
href="#XBHW98"><span 
class="cmti-12">Brasseur et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XBHW98">1998</a>]. MOZART simulations account for emissions of
<!--l. 1011--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mi 
>x</mi></math>&#x00A0;by lightning
and pollution. These simulations have been evaluated against the vertical and diurnal structure of
<!--l. 1014--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mi 
>x</mi></math>&#x00A0;in
many regions [<a 
href="#XEmm97"><span 
class="cmti-12">Emmons</span></a>,&#x00A0;<a 
href="#XEmm97">1997</a>;&#x00A0;<a 
href="#XBHW98"><span 
class="cmti-12">Brasseur et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XBHW98">1998</a>]. Although spatially
complete, these monthly data will not resolve the diurnal signal of
<!--l. 1016--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;established by its
photochemical balance with <!--l. 1017--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi></math>.
A simple diurnal cycle can easily be imposed on the monthly data based on the sun
angle.
</p><!--l. 1021--><p class="indent">   There are significant problems with using
<!--l. 1021--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;distributions
from a CTM climatology. Among them is that the vertical location of
<!--l. 1023--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mi 
>x</mi></math>&#x00A0;within
a cloud is crucial to determining the radiative forcing of
<!--l. 1024--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;[<a 
href="#XSPS99"><span 
class="cmti-12">Solomon</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XSPS99">1999</a>]. Unfortunately the vertical structure of
<!--l. 1025--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mi 
>x</mi></math>&#x00A0;from
lightning is not well understood [<a 
href="#XPPP971"><span 
class="cmti-12">Price et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XPPP971">1997</a>] so a CTM cannot be expected to
represent it correctly. A vast improvment to using pure CTM model data would be to
use a blend of available satellite, in situ, and model data. Groups are attempting to
assemble such climatologies [<a 
href="#XSol99"><span 
class="cmti-12">Solomon</span></a>,&#x00A0;<a 
href="#XSol99">1999</a>] and we will obtain these improved
datasets when available to refine our estimates of the global radiative impact of
<!--l. 1032--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;on
climate.
</p><!--l. 1034--><p class="noindent">
</p>
   <h5 class="subsubsectionHead"><span class="titlemark">4.9.1   </span> <a 
 id="x1-280004.9.1"></a>Model Evaluation</h5>
<!--l. 1035--><p class="noindent">Improvements to Earth&#x2019;s radiative budget will be evaluated against a combination of in situ
                                                                                         
                                                                                         
[<a 
href="#XGiO99"><span 
class="cmti-12">Gilgen and Ohmura</span></a>,&#x00A0;<a 
href="#XGiO99">1999</a>] and satellite observations. The Earth Radiation Budget Experiment
(ERBE) [<a 
href="#XRCH89"><span 
class="cmti-12">Ramanathan et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XRCH89">1989</a>] currently provides the gold standard in long term top of
atmosphere (TOA) solar and longwave radiative fluxes. We note that reduction of model biases
relative to observations may not occur without first re-tuning some free parameters of the GCM.
During the course of this research, data from the EOS CERES experiment [<a 
href="#XWBH96"><span 
class="cmti-12">Wielicki et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XWBH96">1996</a>]
will improve and extend the ERBE record, offering vertical information on heating as
well.
</p><!--l. 1050--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.10   </span> <a 
 id="x1-290004.10"></a>Expected Significance of Results</h4>
<!--l. 1051--><p class="noindent">Taken individually, these enhanced absorption processes by
<!--l. 1051--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
<!--l. 1051--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>, and
<!--l. 1052--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;may
appear to be minor. However, we expect the global annual mean absorption by these processes to total
3&#x2013;8&#x00A0;W m<!--l. 1054--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>.
Thus we expect to reduce the current discrepancy in the atmospheric energy budget of
20&#x2013;25&#x00A0;W m<!--l. 1056--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>&#x00A0;[<a 
href="#XYZC99"><span 
class="cmti-12">Yu</span>
<span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XYZC99">1999</a>] by about 15&#x2013;30%. If we are quick then our CCSM/CAM climate simulations will be
the first in the world to realistically account for this large a fraction of the enhanced absorption
discrepancy. We hope to maintain CAM&#x2019;s leading edge position by soon adding aerosol absorption
as well [<a 
href="#XCRE02"><span 
class="cmti-12">Collins et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XCRE02">2002</a>].
</p><!--l. 1063--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.11   </span> <a 
 id="x1-300004.11"></a>Synergies with Existing Research Efforts</h4>
<!--l. 1064--><p class="noindent">W.&#x00A0;Collins (NCAR) is working on improved parameterizations of cloud overlap effects and of
water vapor continuum absorption. The segregation of water vapor absorption into clear and
cloudy sky components is a natural extension of his generalized framework for treating cloud
overlap.
</p><!--l. 1070--><p class="indent">   S.&#x00A0;Solomon (NOAA) and colleagues are currently assembling a four-dimensional
<!--l. 1071--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;climatology
from satellite (SAGE, GOME) and in situ observations [<a 
href="#XSol99"><span 
class="cmti-12">Solomon</span></a>,&#x00A0;<a 
href="#XSol99">1999</a>]. Their
<!--l. 1073--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;climatology
will be more accurate than the MOZART CTM model predictions of
<!--l. 1074--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;we will start with. We will adopt
such an empirical <!--l. 1075--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;climatology
as soon as possible.
</p><!--l. 1077--><p class="noindent">
                                                                                         
                                                                                         
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.12   </span> <a 
 id="x1-310004.12"></a>Benefits to Community</h4>
<!--l. 1078--><p class="noindent">The climate-sensitivity portion of this research will be performed
in, and contributed to the NCAR CCSM. My previous research on
<!--l. 1080--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;forcing
[<a 
href="#XZen99"><span 
class="cmti-12">Zender</span></a>,&#x00A0;<a 
href="#XZen99">1999a</a>] is now being incorporated into the Community Atmosphere Model (CAM).
Everyone who uses CCSM simulations will ultimately benefit from the improvements contributed
by this project.
</p><!--l. 1085--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.13   </span> <a 
 id="x1-320004.13"></a>Significance to Professional Goals and Responsibilities</h4>
<!--l. 1086--><p class="noindent">This research plan firmly advances my personal career goal to help close Earth&#x2019;s energy budget and
to reduce the associated uncertainty in climate predictions. This proposal on gaseous absorption
nicely balances my research on mineral dust aerosol radiative forcing, since aerosols and trace gases
are the only significant known absorption mechanisms not accounted for in climate
predictions.
</p><!--l. 1094--><p class="indent">   My goal as a faculty member in ESS is to create a research group that regularly contributes
expertise in radiative forcing issues of interest to national and international climate modeling and
assessment programs.
</p><!--l. 1099--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.14   </span> <a 
 id="x1-330004.14"></a>Work Plan for Research</h4>
<!--l. 1100--><p class="noindent">The research will take place in phases which are interleaved to synergize with other research
projects. The tentative goals for each year are </p>
      <ul class="itemize1">
      <li class="itemize">Assess climate response to <!--l. 1105--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;forcing.
      Study <!--l. 1106--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;forcing
      based on MOZART climatology.
      </li>
      <li class="itemize">Study climate response to <!--l. 1108--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;forcing.
      Assess forcing sensitivity to more realistic empirical <!--l. 1109--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;climatology.
      Study forcing due to in-cloud water vapor saturation.
      </li>
      <li class="itemize">Study climate response to in-cloud water vapor forcing. Examine solar forcing due
      <!--l. 1113--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>&#x00A0;continuum
      absorption in near-infrared. Add <!--l. 1114--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>&#x00A0;processes
      if <!--l. 1114--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03B1;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>
      are available.
                                                                                         
                                                                                         
      </li>
      <li class="itemize">Evaluate climate sensitivity to total enhanced <!--l. 1116--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
      <!--l. 1116--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>,
      and <!--l. 1116--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption.
      Evaluate other gaseous absorption processes for possible refinements.
      </li>
      <li class="itemize">Finish evaluations of climate sensitivity to total enhanced <!--l. 1120--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>H</mi><mn>2</mn><mi 
>O</mi></math>,
      <!--l. 1121--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>,
      and <!--l. 1121--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>N</mi><mi 
>O</mi><mn>2</mn></math>&#x00A0;absorption.
      Evaluate change in forcings due to Year&#x00A0;2100 conditions.</li></ul>
<!--l. 1125--><p class="noindent">
</p>
   <h4 class="subsectionHead"><span class="titlemark">4.15   </span> <a 
 id="x1-340004.15"></a>Prior Research Accomplishments</h4>
<!--l. 1127--><p class="noindent">
      </p><ol  class="enumerate1" >
      <li class="enumerate" value="1" 
><a 
 id="x1-34002x1"></a><span 
class="cmti-12">Radiative Effects of Tropical Cirrus Anvil on Climate</span>: We first documented the effect
      of ice crystal size and habit on anvil formation and radiative properties [<a 
href="#XZeK941"><span 
class="cmti-12">Zender and</span>
      <span 
class="cmti-12">Kiehl</span></a>,&#x00A0;<a 
href="#XZeK941">1994</a>]. An important conclusion from this study was that shortwave radiative
      properties of tropical cirrus anvils are very sensitive to the presence of small (<!--l. 1135--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mn>3</mn> <mo 
class="MathClass-rel">&#x003C;</mo> <mi 
>L</mi> <mo 
class="MathClass-rel">&#x003C;</mo> <mn>2</mn><mn>0</mn></math>&#x00A0;<!--l. 1135--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>&#x03BC;</mi><!--mstyle 
class="mbox"--><mtext  >&#x00A0;m</mtext><!--/mstyle--></math>)
      ice crystals which account for less than <!--l. 1136--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mn>2</mn><mi 
>%</mi></math>
      of cloud mass. On a global scale, these anvil physics contribute to teleconnections
      between tropical anvil heating and the extratropical circulation [<a 
href="#XZeK972"><span 
class="cmti-12">Zender and Kiehl</span></a>,&#x00A0;<a 
href="#XZeK972">1997</a>].
      </li>
      <li class="enumerate" value="2" 
><a 
 id="x1-34004x2"></a><span 
class="cmti-12">Observational Detection of Enhanced Shortwave Absorption in Clouds</span>: The discrepancy
      between models and observations of Earth&#x2019;s atmospheric shortwave energy budget is up
      to 25&#x00A0;W m<!--l. 1147--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>,
      globally annually averaged [<a 
href="#XCZM95"><span 
class="cmti-12">Cess et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XCZM95">1995</a>;&#x00A0;<a 
href="#XLMA97"><span 
class="cmti-12">Li et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XLMA97">1997</a>;&#x00A0;<a 
href="#XYZC99"><span 
class="cmti-12">Yu et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XYZC99">1999</a>]. The
      ARESE experiment measured the solar energy budget in clear and cloudy conditions
      using  stacked  aircraft  observations.  Detailed  spectral  analysis  of  the  results  shows
      significant evidence of enhanced shortwave absorption in cloudy atmospheres [<a 
href="#XZBP97"><span 
class="cmti-12">Zender</span>
      <span 
class="cmti-12">et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XZBP97">1997</a>].
      </li>
      <li class="enumerate" value="3" 
><a 
 id="x1-34006x3"></a><span 
class="cmti-12">Radiative Forcing by Oxygen Collision Complexes</span>:  Scrutiny  of  the  magnitude  and
      causes of enhanced shortwave absorption has led to many interesting discoveries, including
      the recognition that absorption by collision complexes of oxygen is significant globally
      (about 1&#x00A0;W m<!--l. 1163--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mo 
class="MathClass-bin">&#x2212;</mo><mn>2</mn></math>).
      <a 
href="#XZen99"><span 
class="cmti-12">Zender</span></a>&#x00A0;[<a 
href="#XZen99">1999a</a>] produced the first climatology of collision complexes and their absorption
      and illustrated many unique features of collision complex absorption. This study refuted
      the notion that <!--l. 1167--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>X</mi></math>&#x00A0;contributes
      to enhanced cloudy absorption (globally).
                                                                                         
                                                                                         
      </li>
      <li class="enumerate" value="4" 
><a 
 id="x1-34008x4"></a><span 
class="cmti-12">Mineral Dust Aerosol Transport and Radiative Forcing</span>: Globally mineral dust accounts
      for more aerosol mass and surface area. We have developed a mineral dust aerosol
      model [<a 
href="#XZen992"><span 
class="cmti-12">Zender</span></a>,&#x00A0;<a 
href="#XZen992">1999b</a>] and included it in a global aerosol assimilation model with an
      integrated aerosol suite (sulfate, dust, sea-salt, carbon) [<a 
href="#XCRE01"><span 
class="cmti-12">Collins et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XCRE01">2001</a>,&#x00A0;&#x00A0;<a 
href="#XCRE02">2002</a>].
      This assimilation scheme helped INDOEX flight operations forecast targets for aerosol
      missions. We are now applying this assimilation model to help constrain global aerosol
      radiative forcing.
      </li>
      <li class="enumerate" value="5" 
><a 
 id="x1-34010x5"></a><span 
class="cmti-12">Radiative Forcing and Absorption by Boundary Layer Aerosol in the US</span>: An important
      task in understanding Earth&#x2019;s atmospheric energy budget is to constrain models with
      long  term  observations  of  aerosol  radiative  forcing.  In  collaboration  with  a  group
      making long term station observations of boundary layer aerosol, we have produced
      the first estimate of the direct radiative forcing by tropospheric aerosols from in situ
      observations in the southeastern US on an annual timescale [<a 
href="#XYZS01"><span 
class="cmti-12">Yu et</span><span 
class="cmti-12">&#x00A0;al.</span></a>,&#x00A0;<a 
href="#XYZS01">2001</a>].
      </li></ol>
                                                                                         
                                                                                         
   <h3 class="sectionHead"><span class="titlemark">5   </span> <a 
 id="x1-350005"></a>References</h3>
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  radiation by water vapor, oxygen, and related collision pairs in the Earth&#x2019;s atmosphere,
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  absorption of radiation by water dimer, <span 
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  constraints on the non-lorentzian continuum effects in the near-infrared solar spectrum
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  Cooper, Clouds and the Earth&#x2019;s radiant energy system (CERES): An&#x00A0;Earth observing
  system experiment, <span 
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class="cmti-12">&#x00A0;Meteorol.</span><span 
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  </p>
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<a 
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  fluxes using surface observations, <span 
class="cmti-12">J.</span><span 
class="cmti-12">&#x00A0;Clim.</span>, <span 
class="cmti-12">8</span>(5), 1309&#x2013;1324, 1995.
  </p>
  <p class="bibitem"><span class="biblabel">
<a 
 id="XYZC99"></a><span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span>Yu,  R.,  M.&#x00A0;Zhang,  and  R.&#x00A0;D.  Cess,  Analysis  of  the  atmospheric  energy  budget:
  A&#x00A0;consistency study of available data sets, <span 
class="cmti-12">J.</span><span 
class="cmti-12">&#x00A0;Geophys.</span><span 
class="cmti-12">&#x00A0;Res.</span>, <span 
class="cmti-12">104</span>(D8), 9655&#x2013;9661, 1999.
  </p>
  <p class="bibitem"><span class="biblabel">
<a 
 id="XYZS01"></a><span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span>Yu,  S.,  C.&#x00A0;S.  Zender,  and  V.&#x00A0;K.  Saxena,  Direct  radiative  forcing  and  atmospheric
  absorption by boundary layer aerosol in the southeastern&#x00A0;US: model estimates on the
  basis of new observations, <span 
class="cmti-12">Atmos.</span><span 
class="cmti-12">&#x00A0;Environ.</span>, <span 
class="cmti-12">35</span>(23), 3967&#x2013;3977, 2001.
  </p>
  <p class="bibitem"><span class="biblabel">
<a 
 id="XZen99"></a><span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span>Zender, C.&#x00A0;S., Global climatology of abundance and solar absorption of oxygen collision
  complexes, <span 
class="cmti-12">J.</span><span 
class="cmti-12">&#x00A0;Geophys.</span><span 
class="cmti-12">&#x00A0;Res.</span>, <span 
class="cmti-12">104</span>(D20), 24,471&#x2013;24,484, 1999a.
  </p>
  <p class="bibitem"><span class="biblabel">
<a 
 id="XZen992"></a><span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span>Zender, C.&#x00A0;S., Radiative forcing by mineral dust, in <span 
class="cmti-12">Proceedings of the Workshop on</span>
  <span 
class="cmti-12">Mineral Dust</span>, June 9&#x2013;11, Boulder,&#x00A0;CO, 1999b.
  </p>
  <p class="bibitem"><span class="biblabel">
<a 
 id="XZeC98"></a><span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span>Zender,        C.&#x00A0;S.,        and        P.&#x00A0;Ch&#x00FD;lek,        A&#x00A0;global        climatology        of
  <!--l. 271--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>O</mi><mn>2</mn></math>,
  <!--l. 271--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mi 
>O</mi><mn>2</mn><mo 
class="MathClass-bin">&#x22C5;</mo><mi 
>N</mi><mn>2</mn></math>,
  and <!--l. 272--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>H</mi><mn>2</mn><mi 
>O</mi></mrow><mo 
class="MathClass-close">)</mo></mrow><mn>2</mn></math>
  abundance  and  absorption,  in  <span 
class="cmti-12">Proceedings  of  the  Eighth  Atmospheric  Radiation</span>
  <span 
class="cmti-12">Measurement (ARM) Science Team Meeting</span>, DOE/ER-0738, pp. 837&#x2013;841, Department
  of  Energy,  U.S.&#x00A0;Department  of  Energy,  Washington,&#x00A0;DC,  March  23&#x2013;27,  Tucson,&#x00A0;AZ,
  1998.
  </p>
  <p class="bibitem"><span class="biblabel">
<a 
 id="XZeK941"></a><span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span>Zender, C.&#x00A0;S., and J.&#x00A0;T. Kiehl, Radiative sensitivities of tropical anvils to small ice
  crystals, <span 
class="cmti-12">J.</span><span 
class="cmti-12">&#x00A0;Geophys.</span><span 
class="cmti-12">&#x00A0;Res.</span>, <span 
class="cmti-12">99</span>(D12), 25,869&#x2013;25,880, 1994.
  </p>
  <p class="bibitem"><span class="biblabel">
<a 
 id="XZeK972"></a><span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span>Zender, C.&#x00A0;S., and J.&#x00A0;T. Kiehl, Tropical climate sensitivity to representation of cirrus
  anvil lifecycle, in <span 
class="cmti-12">Proceedings of the Ninth AMS Conference on Atmospheric Radiation</span>,
  pp. 111&#x2013;114, American Meteorological Society, AMS Press, Boston,&#x00A0;MA, February 2&#x2013;5,
  Long Beach,&#x00A0;CA, 1997.
                                                                                         
                                                                                         
  </p>
  <p class="bibitem"><span class="biblabel">
<a 
 id="XZBP97"></a><span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span>Zender, C.&#x00A0;S., B.&#x00A0;Bush, S.&#x00A0;K. Pope, A.&#x00A0;Bucholtz, W.&#x00A0;D. Collins, J.&#x00A0;T. Kiehl, F.&#x00A0;P.&#x00A0;J.
  Valero,  and  J.&#x00A0;Vitko,  Jr.,  Atmospheric  absorption  during  the  Atmospheric  Radiation
  Measurement  (ARM)  Enhanced  Shortwave  Experiment  (ARESE),  <span 
class="cmti-12">J.</span><span 
class="cmti-12">&#x00A0;Geophys.</span><span 
class="cmti-12">&#x00A0;Res.</span>,
  <span 
class="cmti-12">102</span>(D25), 29,901&#x2013;29,915, 1997.
</p>
  </div>
                                                                                         
                                                                                         
<h3 class="sectionHead"><span class="titlemark">6   </span> <a 
 id="x1-370006"></a>Curriculum Vitae</h3>
<div class="center" 
>
<!--l. 1216--><p class="noindent">
</p><!--l. 1217--><p class="noindent"><span 
class="cmti-12">Curriculum Vitae</span><br />
CHARLES S. ZENDER<br />
</p>
</div>
<!--l. 1221--><p class="noindent">Department of Earth System Science                                                   zender@uci.edu
<br class="newline" />University of California                                                                                 Voice:
(949) 824-2987
<br class="newline" />Irvine, CA&#x00A0;&#x00A0;92697-3100                                                                                   Fax:
(949) 824-3256
<br class="newline" />
</p><!--l. 1225--><p class="noindent"><span 
class="cmbx-12">EDUCATION</span>
      </p><ol  class="enumerate1" >
      <li class="enumerate" value="0" 
><a 
 id="x1-37001x6"></a>(1996)  Atmospheric  Sciences,  University  of  Colorado,  Boulder.  &#x201C;Representation  of
      tropical cirrus anvil in climate models&#x201D;, Advisors: Jeffrey Kiehl and Gary Thomas
      </li>
      <li class="enumerate" value="0" 
><a 
 id="x1-37002x6"></a>(1993) Atmospheric Sciences, University of Colorado, Boulder.
      </li>
      <li class="enumerate" value="0" 
><a 
 id="x1-37003x6"></a>(1990) Physics, Harvard University</li></ol>
<!--l. 1235--><p class="noindent"><span 
class="cmbx-12">SPECIALTIES AND INTERESTS</span>
</p><!--l. 1237--><p class="noindent">Atmospheric Physics, Cloud and Aerosol Microphysics and Chemistry, Terrigenic Aerosol, Particle
Composition and Optical Properties, Radiative Transfer and Radiative Forcing, Global Climate
and Climate Change
</p><!--l. 1243--><p class="noindent"><span 
class="cmbx-12">PROFESSIONAL APPOINTMENTS</span>
      </p><ol  class="enumerate1" >
      <li class="enumerate" value="0" 
><a 
 id="x1-37004x6"></a>University of California at Irvine &#x2013; Assistant Professor of Earth System Science
      </li>
      <li class="enumerate" value="0" 
><a 
 id="x1-37005x6"></a>National Center for Atmospheric Research (NCAR), Boulder, CO &#x2013; Affiliate Scientist
      of the Climate and Global Dynamics (CGD) Division
      </li>
      <li class="enumerate" value="0" 
><a 
 id="x1-37006x6"></a>NCAR &#x2013; Visiting Scientist in Atmospheric Chemistry and CGD Divisions
      </li>
      <li class="enumerate" value="0" 
><a 
 id="x1-37007x6"></a>NCAR &#x2013; Postdoctoral fellow in Advanced Study Program
      </li>
      <li class="enumerate" value="0" 
><a 
 id="x1-37008x6"></a>University of Colorado at Boulder and NCAR CGD &#x2013; Graduate research assistant
                                                                                         
                                                                                         
      </li>
      <li class="enumerate" value="0" 
><a 
 id="x1-37009x6"></a>College of the Atlantic, Bar Harbor, ME &#x2013; Visiting Faculty in Physical Sciences
      </li>
      <li class="enumerate" value="0" 
><a 
 id="x1-37010x6"></a>Smithsonian Astrophysical Observatory, Cambridge, MA &#x2013; Programmer, Technician</li></ol>
<!--l. 1260--><p class="noindent"><span 
class="cmbx-12">REFEREED PUBLICATIONS</span>
</p><!--l. 1264--><p class="indent">Zender, C.&#x00A0;S. and J.&#x00A0;T.&#x00A0;Kiehl, Radiative sensitivities of tropical anvils to small ice crystals, <span 
class="cmti-12">J.</span>
<span 
class="cmti-12">Geophys. Res.</span>, <span 
class="cmti-12">99</span>, 25869&#x2013;25880, 1994.
</p><!--l. 1269--><p class="indent">Zender, C.&#x00A0;S., B. Bush, S.&#x00A0;K. Pope, A. Bucholtz, W.&#x00A0;D. Collins, J.&#x00A0;T. Kiehl, F.&#x00A0;P.&#x00A0;J. Valero, and J.
Vitko&#x00A0;Jr., Atmospheric absorption during the Atmospheric Radiation Measurement
(ARM) Enhanced Shortwave Experiment (ARESE), <span 
class="cmti-12">J. Geophys. Res.</span>, <span 
class="cmti-12">102</span>, 29901&#x2013;29915,
1997.
</p><!--l. 1275--><p class="indent">Zender, C.&#x00A0;S. and J.&#x00A0;T.&#x00A0;Kiehl, Sensitivity of climate simulations to radiative effects of tropical anvil
structure, <span 
class="cmti-12">J. Geophys. Res.</span>, <span 
class="cmti-12">102</span>, 23793&#x2013;23803, 1997.
</p><!--l. 1280--><p class="indent">Cess, R.&#x00A0;D., M.&#x00A0;Zhang, F.&#x00A0;P.&#x00A0;J. Valero, S.&#x00A0;K. Pope, A.&#x00A0;Bucholtz, B.&#x00A0;Bush, C.&#x00A0;S. Zender, and
J.&#x00A0;Vitko&#x00A0;Jr., Absorption of solar radiation by the cloudy atmosphere: Further interpretations of
collocated aircraft measurements, <span 
class="cmti-12">J. Geophys. Res.</span>, <span 
class="cmti-12">104</span>, 2059&#x2013;2066, 1999.
</p><!--l. 1286--><p class="indent">Zender, C.&#x00A0;S., Global climatology of abundance and solar absorption of oxygen collision complexes,
<span 
class="cmti-12">J. Geophys. Res.</span>, <span 
class="cmti-12">104</span>, 24471&#x2013;24484, 1999.
</p><!--l. 1291--><p class="indent">Collins, W.&#x00A0;D., P.&#x00A0;J. Rasch, B.&#x00A0;E. Eaton, B.&#x00A0;Khattatov, J.-F. Lamarque, and C.&#x00A0;S. Zender,
Forecasting aerosols using a chemical transport model with assimilation of satellite aerosol
retrievals: Methodology for INDOEX, <span 
class="cmti-12">In Press in J. Geophys. Res.</span>, 2000.
</p><!--l. 1298--><p class="indent">Yu,&#x00A0;S., C.&#x00A0;S. Zender, and V.&#x00A0;K. Saxena, Direct radiative forcing and atmospheric absorption by
boundary layer aerosol in the southeastern US: new observational estimates and model results,
<span 
class="cmti-12">Submitted to Atmos. Environ.</span>, 2000.
</p><!--l. 1305--><p class="noindent"><span 
class="cmbx-12">FUNDING</span> </p>
      <ul class="itemize1">
      <li class="itemize">Co-I on NASA grant &#x201C;Effects of land-use on climate and water resources: application of
      a land surface model for land-use management&#x201D;, PI: G.&#x00A0;B.&#x00A0;Bonan, 1/1/2000&#x2013;1/1/2003</li></ul>
<!--l. 1313--><p class="noindent"><span 
class="cmbx-12">SERVICE</span> </p>
      <ul class="itemize1">
      <li class="itemize">Peer-review for Geophys. Res. Lett., J. Geophys. Res., J. Atmos. Sci., Mon. Weather
      Rev., <span 
class="cmti-12">Nature</span>, Q. J. R. Meteorol. Soc., <span 
class="cmti-12">Tellus</span>, NSF, NASA, USGCRP
      </li>
      <li class="itemize">Maintainer        of        NCAR        CCM        Column        Radiation        Model
      (<span class="obeylines-h"><a 
href="http://www.cgd.ucar.edu/cms/crm" class="url" ><span 
class="cmtt-12">http://www.cgd.ucar.edu/cms/crm</span></a></span>). 1996&#x2013;present.
      </li>
      <li class="itemize">Author                                        and                                        administrator
      of NCO netCDF Operators (<span class="obeylines-h"><a 
href="http://www.cgd.ucar.edu/cms/nco" class="url" ><span 
class="cmtt-12">http://www.cgd.ucar.edu/cms/nco</span></a></span>), a freely available
      geophysical data manipulation toolkit. 1995&#x2013;present.
      </li>
      <li class="itemize">Author      and      maintainer      of      Enhanced      Absorption      Bibliography
      (<span class="obeylines-h"><a 
href="ftp://ftp.cgd.ucar.edu/pub/zender/arese/bib_aca.ps.gz" class="url" ><span 
class="cmtt-12">ftp://ftp.cgd.ucar.edu/pub/zender/arese/bib_aca.ps.gz</span></a></span>). 1997&#x2013;present.
                                                                                         
                                                                                         
      </li>
      <li class="itemize">Contributor to the University of Northern Colorado Mathematics and Science Teachers
      Hotline (MAST) (800 866-MAST). 1995&#x2013;present.
      </li>
      <li class="itemize">University of Colorado, Boulder, CO &#x2013; Founder and director of the APAS Help Center,
      a free tutoring center which assisted dozens of diverse undergraduates in the physical
      sciences every year. My role included securing funding, tutoring, and managing a group
      of about 10 paid graduate student tutors. 1992&#x2013;1995.</li></ul>
<!--l. 1334--><p class="noindent"><span 
class="cmbx-12">HONORS</span> </p>
      <ul class="itemize1">
      <li class="itemize">Outstanding Student Presentation in Atmospheric Sciences Section, Fall AGU Meeting,
      San Francisco CA, 1995</li></ul>
<!--l. 1340--><p class="noindent"><span 
class="cmbx-12">COURSES TAUGHT</span> </p>
      <ul class="itemize1">
      <li class="itemize">Earth System Science 20E: The Atmosphere
      </li>
      <li class="itemize">Earth System Science 111/211: Radiative Processes and Remote Sensing</li></ul>
<!--l. 1346--><p class="noindent"><span 
class="cmbx-12">COLLABORATORS</span> </p>
      <ul class="itemize1">
      <li class="itemize">C.&#x00A0;A. Ammann (U.&#x00A0;Massachusetts Amherst), G.&#x00A0;B. Bonan (NCAR), G.&#x00A0;P. Brasseur
      (MPI Hamburg), R.&#x00A0;D. Cess (SUNY Stonybrook), P.&#x00A0;Ch&#x00FD;lek (Dalhousie), W.&#x00A0;D.
      Collins  (NCAR),  J.&#x00A0;T.  Kiehl  (NCAR),  N.&#x00A0;M.  Mahowald  (UC  Santa  Barbara),
      G.&#x00A0;McFarquhar  (NCAR)  K.&#x00A0;Oleson  (NCAR),  P.&#x00A0;J.  Rasch  (NCAR),  X.&#x00A0;X.  Tie
      (NCAR), F.&#x00A0;P.&#x00A0;J. Valero (Scripps), S.&#x00A0;Yu (Duke)</li></ul>
                                                                                         
                                                                                         
 
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