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<article language="en">
	<journal>
		<journal_title>Atmospheric Chemistry and Physics Discussions</journal_title>
		<journal_url>www.atmos-chem-phys-discuss.net</journal_url>
		<issn>1680-7367</issn>
		<eissn>1680-7375</eissn>
		<volume_number>8</volume_number>
		<issue_number>2</issue_number>
		<publication_year>2008</publication_year>
	</journal>
	<doi>10.5194/acpd-8-4407-2008</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/8/4407/2008/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/8/4407/2008/acpd-8-4407-2008.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/8/4407/2008/acpd-8-4407-2008.pdf</fulltext_pdf>
	<start_page>4407</start_page>
	<end_page>4437</end_page>
	<publication_date>2008-03-04</publication_date>
	<article_title content_type="html">Growth-deviation model to understand the perceived variety of falling snow</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>J. Nelson</name>
			<email>jnelson@se.ritsumei.ac.jp</email>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">College of Science and Engineering, Ritsumeikan University, Nojihigashi 1-1-1, Kusatsu 525-8577, Japan</affiliation>
	</affiliations>
	<abstract content_type="html">What is the source of snow-crystal variety? This question is answered using
a model of snow-crystal growth in a cloud. In the model, crystals start
under various initial cloud-crystal conditions, and then encounter growth
perturbations from random air-temperature deviations along simple crystal
trajectories. To obtain distributions of these deviations, I analyzed recent
high-resolution measurements of cloud updrafts and temperatures. The
trajectories and distributions are used to estimate the number of possible
snow crystal shapes, to a given viewing resolution, from a range of initial
conditions. The logarithm of this number, defined here as the perceived
shape variety or &quot;diversity&quot;, is dominated not by the range of conditions,
but rather by the air-temperature deviations along a trajectory. This
qualitative result is independent of the viewing resolution. Thus,
temperature deviations are the main source of crystal diversity. When
plotted against the crystal&apos;s initial temperature (here &amp;ndash;11 to &amp;ndash;19&amp;deg;C),
the curve is mitten-shaped, with a main peak at &amp;ndash;15.4&amp;deg;C and a smaller,
sharper peak near &amp;ndash;14.4&amp;deg;C. The mitten shape arises from temperature
trends in the crystal&apos;s terminal fallspeed and prism-face growth rate.
Specifically, the two diversity peaks are due to maxima in growth-rate
sensitivity to temperature near &amp;ndash;15.4 and &amp;ndash;14.0&amp;deg;C. Applying the
results to all snow crystals ever formed, then, to 1-&amp;mu;m resolution, all
crystals that began near &amp;ndash;15&amp;deg;C would appear unique, but some that
began near &amp;ndash;11&amp;deg;C would not.</abstract>
	<references>
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</article>

