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	<title>Wine and Cheese Spring 2023 - Revision history</title>
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	<updated>2026-06-04T21:17:18Z</updated>
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		<id>https://caswiki.johnshopkins.edu/index.php?title=Wine_and_Cheese_Spring_2023&amp;diff=1556&amp;oldid=prev</id>
		<title>Kdkuntz: Created page with &quot;{| align=&quot;right&quot;   | __TOC__   |}  This page records the schedule, titles and abstracts of the JHU/STScI CAS Astrophysics Wine &amp; Cheese Series in Spring 2023.  Wine and Cheese sessions with one speaker will have a 50 minute talk with 10 minutes for questions. Sessions with two speakers will have two 25 minute talks, each with 5 minutes for questions. Sessions in the Graduate Student Series will have three 15 minute talks, each with 5 minu...&quot;</title>
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		<updated>2023-01-27T16:00:44Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;{| align=&amp;quot;right&amp;quot;   | __TOC__   |}  This page records the schedule, titles and abstracts of the &lt;a href=&quot;/index.php?title=CAS_Wine_and_Cheese_Seminars&quot; title=&quot;CAS Wine and Cheese Seminars&quot;&gt;JHU/STScI CAS Astrophysics Wine &amp;amp; Cheese Series&lt;/a&gt; in Spring 2023.  Wine and Cheese sessions with one speaker will have a 50 minute talk with 10 minutes for questions. Sessions with two speakers will have two 25 minute talks, each with 5 minutes for questions. Sessions in the Graduate Student Series will have three 15 minute talks, each with 5 minu...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{| align=&amp;quot;right&amp;quot;&lt;br /&gt;
  | __TOC__&lt;br /&gt;
  |}&lt;br /&gt;
&lt;br /&gt;
This page records the schedule, titles and abstracts of the [[CAS_Wine_and_Cheese_Seminars|JHU/STScI CAS Astrophysics Wine &amp;amp; Cheese Series]] in Spring 2023.&lt;br /&gt;
&lt;br /&gt;
Wine and Cheese sessions with one speaker will have a 50 minute talk with 10 minutes for questions. Sessions with two speakers will have two 25 minute talks, each with 5 minutes for questions. Sessions in the Graduate Student Series will have three 15 minute talks, each with 5 minutes for questions.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;h2&amp;gt;[[CAS_Wine_and_Cheese_Seminars|Back to W&amp;amp;C Schedule]] &amp;lt;/h2&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=30 January=&lt;br /&gt;
== Matt Clement (JHU-APL) ==&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;The Early Secular Evolution of the Outer Solar System and the&lt;br /&gt;
Present State of the Nice Model&amp;#039;&amp;#039;&amp;#039;&amp;lt;br&amp;gt;&lt;br /&gt;
In the current consensus dynamical evolutionary hypothesis for the&lt;br /&gt;
solar system, after forming in a compact configuration of circular&lt;br /&gt;
orbits, the giant planets acquire their modern dynamical configuration&lt;br /&gt;
through an episode of orbital instability.  Over the past two decades,&lt;br /&gt;
numerical simulations of the so-called Nice Model have been&lt;br /&gt;
successfully leveraged to explain numerous peculiar solar system&lt;br /&gt;
qualities.  In particular, the orbital distributions of small bodies&lt;br /&gt;
(e.g.: asteroids, Kuiper belt objects, irregular satellites and outer&lt;br /&gt;
solar system trojans) provide strong observational constraints that no&lt;br /&gt;
other proposed model is capable of satisfying.  I will review the&lt;br /&gt;
current state of the Nice Model, and highlight a collection of&lt;br /&gt;
systematic issues identified in past studies that have motivated my&lt;br /&gt;
research activities as a postdoc.  While simulations in classic&lt;br /&gt;
investigations overestimated the inner asteroid belt’s high&lt;br /&gt;
inclination population by several orders of magnitude (i.e.: they&lt;br /&gt;
create stable orbits that are not observed today), I will show how&lt;br /&gt;
Jupiter and Saturn’s precise approach to their modern orbits induces a&lt;br /&gt;
corresponding cycling of resonances in the belt that removes these&lt;br /&gt;
objects.  An additional constraint on instability simulations comes&lt;br /&gt;
from Jupiter&amp;#039;s fifth eccentric eigenmode, which is an important driver&lt;br /&gt;
of the solar system’s global evolution. Starting from commonly-assumed&lt;br /&gt;
near-circular orbits, the present-day magnitude of this mode in&lt;br /&gt;
Jupiter’s eccentricity vector is significantly outside the range of&lt;br /&gt;
numerically generated outcomes.  I will present new results motivated&lt;br /&gt;
by modern hydrodynamical simulations of the giant planets&amp;#039; evolution&lt;br /&gt;
within the primordial gaseous disk that consider the possibility of&lt;br /&gt;
Jupiter and Saturn emerging from the nebular gas locked in 2:1&lt;br /&gt;
resonance with non-zero eccentricities. I will show that, in such a&lt;br /&gt;
scenario, the modern Jupiter-Saturn system represents a typical&lt;br /&gt;
simulation outcome.  Finally, I will highlight the survivability of&lt;br /&gt;
the giant planets’ regular satellites (namely those of Jupiter and&lt;br /&gt;
Uranus) as an outstanding problem, and discuss the potential&lt;br /&gt;
implications of this shortcoming.&lt;/div&gt;</summary>
		<author><name>Kdkuntz</name></author>
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