<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://en.formulasearchengine.com/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=77.126.69.125</id>
	<title>formulasearchengine - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="https://en.formulasearchengine.com/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=77.126.69.125"/>
	<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/wiki/Special:Contributions/77.126.69.125"/>
	<updated>2026-05-02T03:51:56Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.43.0-wmf.28</generator>
	<entry>
		<id>https://en.formulasearchengine.com/index.php?title=Couette_flow&amp;diff=9869</id>
		<title>Couette flow</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/index.php?title=Couette_flow&amp;diff=9869"/>
		<updated>2013-11-30T16:38:47Z</updated>

		<summary type="html">&lt;p&gt;77.126.69.125: /* Mathematical description */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Redirect|Ellipticity|ellipticity in differential calculus|elliptic operator}}&lt;br /&gt;
{{About|geometry|psychopathology|flattening of affect}}&lt;br /&gt;
[[File:An ellipse with auxiliary circle.svg|thumb |right|200px |A circle of radius &#039;&#039;a&#039;&#039; compressed to an ellipse.]] &lt;br /&gt;
[[File:Ellipsoid revolution oblate aab auxiliary sphere.svg|thumb|right|200px |A sphere of radius &#039;&#039;a&#039;&#039; compressed to an oblate ellipsoid of revolution oblate.]] &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Flattening&#039;&#039;&#039; is a measure of the compression of a [[circle]] or [[sphere]] along a diameter to form an [[ellipse]] or an [[ellipsoid]] of revolution ([[spheroid]]) respectively. Other terms used are &#039;&#039;&#039;ellipticity&#039;&#039;&#039;, or &#039;&#039;&#039;oblateness&#039;&#039;&#039;. The usual notation for flattening is &#039;&#039;f&#039;&#039; and its definition in terms of the semi-axes of the resulting ellipse or ellipsoid is&lt;br /&gt;
::&amp;lt;math&amp;gt; \mathrm{flattening} = f =\frac {a - b}{a}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The compression factor is &#039;&#039;b/a&#039;&#039; in each case. For the ellipse, this factor is also the aspect ratio of the ellipse.&lt;br /&gt;
&lt;br /&gt;
There are two other variants of flattening (see below) and when it is necessary to avoid confusion the above flattening is called the &#039;&#039;&#039;first flattening&#039;&#039;&#039;. The following definitions may be found in standard texts &amp;lt;ref name=maling&amp;gt;{{cite book | last=Maling |first=Derek Hylton | title=Coordinate Systems and Map Projections |edition=2nd |year=1992 | publisher =Pergamon Press|location=Oxford; New York |isbn=0-08-037233-3}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=snyder&amp;gt;{{cite book |author=Snyder, John P. | title=Map Projections: A Working Manual |series=U.S. Geological Survey Professional Paper |volume=1395 | year=1987| publisher =United States Government Printing Office |location=Washington, D.C. |url=http://pubs.er.usgs.gov/pubs/pp/pp1395}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=torge&amp;gt;Torge, W. (2001). &#039;&#039;Geodesy&#039;&#039; (3rd edition). de Gruyter. ISBN 3-11-017072-8&amp;lt;/ref&amp;gt; and online web texts&amp;lt;ref name=osborne&amp;gt;Osborne, P. (2008). &#039;&#039;[http://mercator.myzen.co.uk/mercator.pdf The Mercator Projections]&#039;&#039; Chapter 5.&amp;lt;/ref&amp;gt;&amp;lt;ref name=rapp&amp;gt;Rapp, Richard H. (1991). &#039;&#039;Geometric Geodesy, Part I&#039;&#039;. Dept. of Geodetic Science and Surveying, Ohio State Univ., Columbus, Ohio. [http://hdl.handle.net/1811/24333]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Definitions of flattening ==&lt;br /&gt;
In the following, &#039;&#039;a&#039;&#039; is the larger dimension (e.g. semimajor axis), whereas &#039;&#039;b&#039;&#039; is the smaller (semiminor axis).  All flattenings are zero for a circle (&#039;&#039;a&#039;&#039;=&#039;&#039;b&#039;&#039;).&lt;br /&gt;
::{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;border: 1px solid darkgray;   width: 60%;&amp;quot;  cellpadding=&amp;quot;5&amp;quot;&lt;br /&gt;
|  style=&amp;quot;padding-left: 0.5em&amp;quot;| (first) flattening &lt;br /&gt;
| style=&amp;quot;padding-left: 0.5em&amp;quot;|&amp;lt;math&amp;gt;f\,\!&amp;lt;/math&amp;gt; &lt;br /&gt;
| style=&amp;quot;padding-left: 0.5em&amp;quot;|&amp;lt;math&amp;gt;\frac{a-b}{a}\,\!&amp;lt;/math&amp;gt;&lt;br /&gt;
| style=&amp;quot;width: 50%; padding-left: 0.5em &amp;quot;|Fundamental. The inverse 1/f is the normal choice for geodetic [[reference ellipsoid]]s.&lt;br /&gt;
|-&lt;br /&gt;
| style=&amp;quot;padding-left: 0.5em&amp;quot;|second flattening&lt;br /&gt;
| style=&amp;quot;padding-left: 0.5em&amp;quot;|&amp;lt;math&amp;gt;f&#039;\,\!&amp;lt;/math&amp;gt; &lt;br /&gt;
| style=&amp;quot;padding-left: 0.5em&amp;quot;|&amp;lt;math&amp;gt;\frac{a-b}{b}\,\!&amp;lt;/math&amp;gt; &amp;amp;nbsp;  &lt;br /&gt;
|  style=&amp;quot;padding-left: 0.5em&amp;quot;| Rarely used.&lt;br /&gt;
|-&lt;br /&gt;
| style=&amp;quot;padding-left: 0.5em&amp;quot;|  third  flattening &lt;br /&gt;
| style=&amp;quot;padding-left: 0.5em&amp;quot;|&amp;lt;math&amp;gt;n\quad(f&#039;&#039;)\,\!&amp;lt;/math&amp;gt; &amp;amp;nbsp;    &lt;br /&gt;
| style=&amp;quot;padding-left: 0.5em&amp;quot;|&amp;lt;math&amp;gt;\frac{a-b}{a+b}\,\!&amp;lt;/math&amp;gt; &lt;br /&gt;
|  style=&amp;quot;padding-left: 0.5em&amp;quot;| Used in geodetic calculations as a small expansion parameter.&amp;lt;ref name=bessel&amp;gt;F. W. Bessel, 1825, &#039;&#039;Uber die Berechnung der geographischen Langen und Breiten aus geodatischen Vermessungen&#039;&#039;, &#039;&#039;Astron.Nachr.&#039;&#039;, 4(86), 241-254, {{doi|10.1002/asna.201011352}}, translated into English by C. F. F. Karney and R. E. Deakin as &#039;&#039;The calculation of longitude and latitude from geodesic measurements&#039;&#039;, &#039;&#039;Astron. Nachr.&#039;&#039; 331(8), 852-861 (2010), E-print {{arxiv|0908.1824}},  {{bibcode|1825AN......4..241B}}&amp;lt;/ref&amp;gt;   &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==Identities involving flattening==&lt;br /&gt;
The flattenings are related to other parameters of the ellipse. For example:&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{align}&lt;br /&gt;
b&amp;amp;=a(1-f)=a\left(\frac{1-n}{1+n}\right),\\&lt;br /&gt;
 e^2&amp;amp;=2f-f^2 = \frac{4n}{(1+n)^2}.\\&lt;br /&gt;
\end{align}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Numerical values for planets==&lt;br /&gt;
For the [[Earth]] modelled by the [[WGS84]] ellipsoid the &#039;&#039;defining&#039;&#039; values  are&amp;lt;ref&amp;gt;[http://earth-info.nga.mil/GandG/publications/tr8350.2/tr8350_2.htmlNIMAThe WGS84 parameters are listed in the National Geospatial-Intelligence Agency publication TR8350.2] page 3-1.&amp;lt;/ref&amp;gt; &lt;br /&gt;
::&#039;&#039;a&#039;&#039; (equatorial radius): 6 378 137.0&amp;amp;nbsp;m&lt;br /&gt;
:: &#039;&#039;1/f&#039;&#039; (inverse flattening): 298.257 223 563&lt;br /&gt;
from which one derives&lt;br /&gt;
:: &#039;&#039;b&#039;&#039; (polar radius): 6 356 752.3142&amp;amp;nbsp;m,&lt;br /&gt;
so that the difference of the major and minor semi-axes is  {{convert|21.385|km|0|abbr=on}}. (This is only &amp;amp;nbsp;0.335% of the major axis so a representation of the Earth on a computer screen could be sized as 300px by 299px. Because this would be virtually indistinguishable from a sphere shown as 300px by 300px, illustrations typically greatly exaggerate the flattening in cases where the image needs to represent the oblateness of the Earth.) &lt;br /&gt;
&lt;br /&gt;
Other values in the Solar System are [[Jupiter]], &amp;amp;nbsp;&#039;&#039;f&#039;&#039;=1/16; [[Saturn]], &amp;amp;nbsp;&#039;&#039;f&#039;&#039;= 1/10, the [[Moon]] &amp;amp;nbsp;&#039;&#039;f&#039;&#039;= 1/900. The flattening of the [[Sun]] is less than 1/1000.&lt;br /&gt;
&lt;br /&gt;
==Origin of flattening==&lt;br /&gt;
In 1687 [[Isaac Newton]] published the &#039;&#039;[[Philosophiæ Naturalis Principia Mathematica|Principia]]&#039;&#039; in which he included a proof that a rotating self-gravitating fluid body in equilibrium takes the form of an oblate [[ellipsoid]] of revolution (a [[spheroid]]).&amp;lt;ref name=newton&amp;gt;Isaac Newton:&#039;&#039;Principia&#039;&#039; Book III Proposition XIX Problem III, p. 407 in [https://archive.org/stream/ost-physics-newtonspmathema00newtrich/newtonspmathema00newtrich#page/n411/mode/2up Andrew Motte translation]&amp;lt;/ref&amp;gt; The amount of flattening depends on the [[density]] and  the balance of [[gravitational force]] and [[centrifugal force (rotating reference frame)|centrifugal force]].&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Astronomy]]&lt;br /&gt;
* [[Earth ellipsoid]]&lt;br /&gt;
* [[Earth&#039;s rotation]]&lt;br /&gt;
* [[Eccentricity (mathematics)#Ellipses|Eccentricity (mathematics)]]&lt;br /&gt;
* [[Equatorial bulge]]&lt;br /&gt;
* [[Gravitational field]]&lt;br /&gt;
* [[Gravity formula]]&lt;br /&gt;
* [[Ovality]]&lt;br /&gt;
* [[Planetology]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Celestial mechanics]]&lt;br /&gt;
[[Category:Geodesy]]&lt;br /&gt;
[[Category:Trigonometry]]&lt;/div&gt;</summary>
		<author><name>77.126.69.125</name></author>
	</entry>
</feed>