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{{Infobox scientist
The surface temperature of a planet can be calculated by equating the power received by the planet with the power emitted by a blackbody of temperature <var>T</var>.
| name = David Kipping
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| fields = [[Astronomy]]
| workplaces = [[Columbia University]]
| alma_mater = [[University College London]] (Ph.D. 2011) <br> [[University of Cambridge]] (M.Sc 2007, M.A. 2006)
| doctoral_advisor = [[Giovanna Tinetti]]
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| known_for = [[Exomoons]] <br> [[Exoplanets]]
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| awards = [[Keith Runcorn Prize]] (2012)
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'''David Kipping''' is an assistant professor of astronomy at [[Columbia University]]. His primary research interests include [[Exoplanets]], [[Exomoons]], and [[Astrostatistics]].
Take the case of a planet at a distance <var>D</var> from a star of [[luminosity]] <var>L</var>.


== Research ==
Here the area of the planet that absorbs the power from the star is <var>A<sub>abs</sub></var> which is some fraction of the total surface area <math>A_{\rm total} = 4 \pi r^2</math> where <var>r</var> is the radius of the planet. This area intercepts some of the power which is spread over the surface of a sphere of radius <var>D</var>. We also allow the planet to reflect some of the incoming radiation by incorporating a parameter <var>a</var> called the [[albedo]]. An albedo of 1 means that all the radiation is reflected, an albedo of 0 means all of it is absorbed. The expression for absorbed power is then:


<math>P_{\rm abs} = \frac {L A_{\rm abs} (1-a)}{4 \pi D^2}</math>


== References ==
The next assumption we can make is that the entire planet is at the same temperature <var>T</var> and the power is radiated over an area <var>A<sub>rad</sub></var> which is again some fraction of the total area of the planet <math>A_{\rm total} = 4 \pi r^2</math> where <var>r</var> is the radius of the planet. There is also a factor <var>ε</var>, which is the [[Emissivity]] and represents atmospheric effects. ε ranges from 1 to 0 with 1 meaning the planet is a perfect blackbody and emits all the incident power. The [[Stefan–Boltzmann law]] gives an expression for the power radiated by the planet:
{{reflist}}


== External links ==
<math>P_{\rm rad} = A_{\rm rad} \varepsilon \sigma T^4</math>


* [http://www.davidkipping.co.uk/ David Kipping Homepage]
Equating these two expressions and rearranging gives an expression for the surface temperature:
* {{Google Scholar id|UXY08zEAAAAJ}}
* [http://coolworlds.astro.columbia.edu/ Cool Worlds Lab]


{{DEFAULTSORT:Kipping, David}}
<math>T = \left (\frac{A_{\rm abs}}{A_{\rm rad}} \frac{L (1-a)}{4 \pi \sigma \varepsilon D^2} \right )^{\tfrac{1}{4}}</math>
[[Category:Living people]]

[[Category:Year of birth missing (living people)]]
Note the ratio of the two areas. Common assumptions for this ratio are 1/4 for a rapidly rotating body and 1/2 for a slowly rotating body. This ratio would be 1 for the [[subsolar point]], the point on the planet directly below the sun and gives the maximum temperature of the planet.<ref>Swihart, Thomas. "Quantitative Astronomy". Prentice Hall, 1992, Chapter 5, Section 1.</ref>

Lets look at the Earth. The Earth has an albedo of 0.367<ref>http://nssdc.gsfc.nasa.gov/planetary/factsheet/earthfact.html</ref>. The emissivity is more variable and there are many [[climate models]] for it but a good average for Earth is 0.5. The Earth is a fairly fast rotator so the area ratio can be estimated as 1/4. The other variables are constant. This calculation gives us an effective tempurature of the Earth of 298K. Considering how complicated the system is, this is a good estimate.

Also note here that this equation does not take into account any effects from internal heating of the planet.

{{Reflist}}

Revision as of 20:26, 21 November 2019

David Kipping
Alma materUniversity College London (Ph.D. 2011)
University of Cambridge (M.Sc 2007, M.A. 2006)
Known forExomoons
Exoplanets
AwardsKeith Runcorn Prize (2012)
Scientific career
FieldsAstronomy
InstitutionsColumbia University
Doctoral advisorGiovanna Tinetti

David Kipping is an assistant professor of astronomy at Columbia University. His primary research interests include Exoplanets, Exomoons, and Astrostatistics.

Research

References