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	<title>Comments on: Q</title>
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	<description>characterizing planetary systems</description>
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		<title>By: Centauri Dreams &#187; Blog Archive &#187; Hyades Planet Challenges Formation Theories</title>
		<link>http://oklo.org/2006/04/15/q/comment-page-1/#comment-1250</link>
		<dc:creator>Centauri Dreams &#187; Blog Archive &#187; Hyades Planet Challenges Formation Theories</dc:creator>
		<pubDate>Wed, 21 Feb 2007 15:09:35 +0000</pubDate>
		<guid isPermaLink="false">http://oklo.org/?p=39#comment-1250</guid>
		<description>[...] Laughlin is saying that the likely dispersal of the protostellar disks in the Hyades stars (thanks to UV) makes core accretion less likely in the case of Epsilon Tauri b (there simply wasn&#8217;t time). Whereas if gravitational instability produces a planet for every few hundred stars formed, as Laughlin believes, then there is no reason not to expect such a world in an open cluster like the Hyades. That&#8217;s a win for gravitational instability, though Laughlin still sees core accretion as the dominant model, writing elsewhere that &#8220;&#8230;the weight of observational and theoretical evidence seems to be shifting against the gravitational instability hypothesis.&#8221; [...]</description>
		<content:encoded><![CDATA[<p>[...] Laughlin is saying that the likely dispersal of the protostellar disks in the Hyades stars (thanks to UV) makes core accretion less likely in the case of Epsilon Tauri b (there simply wasn&#8217;t time). Whereas if gravitational instability produces a planet for every few hundred stars formed, as Laughlin believes, then there is no reason not to expect such a world in an open cluster like the Hyades. That&#8217;s a win for gravitational instability, though Laughlin still sees core accretion as the dominant model, writing elsewhere that &#8220;&#8230;the weight of observational and theoretical evidence seems to be shifting against the gravitational instability hypothesis.&#8221; [...]</p>
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		<title>By: systemic - Lonely Planet Guide to the Hyades</title>
		<link>http://oklo.org/2006/04/15/q/comment-page-1/#comment-1107</link>
		<dc:creator>systemic - Lonely Planet Guide to the Hyades</dc:creator>
		<pubDate>Fri, 09 Feb 2007 07:49:58 +0000</pubDate>
		<guid isPermaLink="false">http://oklo.org/?p=39#comment-1107</guid>
		<description>[...] For more information, this series: 1, 2, 3, 4 and 5, 6, and 7. of oklo posts that compare and contrast the gravitational instability and core accretion theories for giant planet formation. [...]</description>
		<content:encoded><![CDATA[<p>[...] For more information, this series: 1, 2, 3, 4 and 5, 6, and 7. of oklo posts that compare and contrast the gravitational instability and core accretion theories for giant planet formation. [...]</p>
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	<item>
		<title>By: systemic - G.I. No</title>
		<link>http://oklo.org/2006/04/15/q/comment-page-1/#comment-100</link>
		<dc:creator>systemic - G.I. No</dc:creator>
		<pubDate>Tue, 02 May 2006 02:28:25 +0000</pubDate>
		<guid isPermaLink="false">http://oklo.org/?p=39#comment-100</guid>
		<description>[...] (1) In order to have gravitational instability work in the manner shown in the fragmentation simulations, you need to start with an axisymmetric disk that has a sufficiently low value for the Toomre Q parameter. That is, in order for the initial conditions in the successful Boss simulations to be valid, a growing protostellar disk needs to remain completely stable with respect to low-level non-axisymmetric disturbances until BOOM, it reaches a threshold Q value where it is prone to spiral instabilities that exponentiate on a near-orbital timescale. [...]</description>
		<content:encoded><![CDATA[<p>[...] (1) In order to have gravitational instability work in the manner shown in the fragmentation simulations, you need to start with an axisymmetric disk that has a sufficiently low value for the Toomre Q parameter. That is, in order for the initial conditions in the successful Boss simulations to be valid, a growing protostellar disk needs to remain completely stable with respect to low-level non-axisymmetric disturbances until BOOM, it reaches a threshold Q value where it is prone to spiral instabilities that exponentiate on a near-orbital timescale. [...]</p>
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