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		<id>https://en.formulasearchengine.com/w/index.php?title=Theta_solvent&amp;diff=259096</id>
		<title>Theta solvent</title>
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		<updated>2014-12-07T00:58:04Z</updated>

		<summary type="html">&lt;p&gt;165.124.128.186: &lt;/p&gt;
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&lt;div&gt;&lt;br /&gt;
&lt;br /&gt;
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		<author><name>165.124.128.186</name></author>
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	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Square-integrable_function&amp;diff=267244</id>
		<title>Square-integrable function</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Square-integrable_function&amp;diff=267244"/>
		<updated>2014-11-07T21:00:35Z</updated>

		<summary type="html">&lt;p&gt;165.124.129.186: /* Properties */ Clarified reference to earlier example&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;My greatest and possibly only downside with the Ruger Standard Model got here when stripping it down for cleaning. There is a metal lever within the rear of the pistol grip that unfolds like a pocket knife, permitting the barreled receiver to be separated from the frame. In this situation, the bolt could be faraway from the receiver and the gun cleaned totally. What I didn&#039;t discover on the time was that the tiny rebound spring popped out of place on the bolt when I reassembled the gun. The bolt locked solidly into place and I could not get the gun back apart.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;Building a door frame for set up underneath a basement staircase is similar to establishing framework for any inside door opening. As with all doorways, a variety of elements will decide the frame’s exact layout. Should you’re constructing a closet below stairs positioned in opposition to a wall, for example, you may be capable of place the door at the back aspect of the case, beneath the highest tread. Ceiling height, staircase dimension and desired format will decide whether you’re able to set up a regular-size door or if it&#039;s essential modify the door and its casing to fit below the stairs.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;Warthog knife [http://Wiki.Wandboard.org/index.php/Throwing_Knives_For_Beginners sharpener] is one sort of sharpeners that originated from South Africa but is now obtainable within the United States and different parts of the world. The title of the company was derived from the name of a wild animal with sharp tusks. The corporate manufactures all kinds of knives from kitchen knives , hunting knives , pocket knives and plenty of other blades. 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When you have determined to mount this water heater, relaxation assured it&#039;ll require a small ceiling area. Backed with positive buyer testimonials, Bosch 2700ES Aquaster can present hot water to multiple electrical appliances at one time. For instance, chances are you&#039;ll wish to use the bathe as well as run the dishwasher and washer. Now, operating all these appliances at the identical time means, a continuous provide of scorching water is a must. This can be easily achieved if you have Bosch 2700ES Aquastar installed in your house.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;In the knife group Chris Reeve is synonymous with high quality and innovation and no discussion of finest pocket knives is complete without mentioning the Sebenza. The Chris Reeve Sebenza has long been regarded by the industry as top-of-the-line folding knives cash can buy. It has a titanium body lock design that mixes simplicity with sturdiness [http://www.thebestpocketknifereviews.com/best-throwing-knives-top-recommendations/ throwing knives For sale ebay] and a blade made out of S35VN chrome steel that endlessly retains its edge. Once opened and locked the knife feels as solid as a set blade and holds comfortably within the hand. The quality is truly second to none and it’ll shave the hairs in your chin right out of the field!&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;The Opinel is sharp enough to shave fatwood. As you might already know, fatwood is the resin saturated wood often discovered within the stumps of fallen pine bushes. It&#039;s also referred to as lightwood or pitchwood, depending on where you grew up. The good news is that small pile of fatwood sticks or shavings is sufficient to get any correct fireplace began. It lights very easily then burns scorching and quick. However, a whittling away on a good chunk of previous fatwood can virtually be like trying to cut a bit of glass, for the reason that resin hardens with age.&lt;/div&gt;</summary>
		<author><name>165.124.129.186</name></author>
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	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Directional_statistics&amp;diff=8459</id>
		<title>Directional statistics</title>
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		<updated>2014-01-23T21:24:25Z</updated>

		<summary type="html">&lt;p&gt;165.124.128.146: /* Software */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[mathematics]], especially [[functional analysis]], &#039;&#039;&#039;Bessel&#039;s inequality&#039;&#039;&#039; is a statement about the coefficients of an element &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;  in a [[Hilbert space]] with respect to an [[orthonormal]] [[sequence]].&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt; be a Hilbert space, and suppose that &amp;lt;math&amp;gt;e_1, e_2, ...&amp;lt;/math&amp;gt; is an orthonormal sequence in &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt;. Then, for any &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; in &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt; one has&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_{k=1}^{\infty}\left\vert\left\langle x,e_k\right\rangle \right\vert^2 \le \left\Vert x\right\Vert^2 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where 〈•,•〉 denotes the [[inner product space|inner product]] in the Hilbert space &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt;. If we define the infinite sum&lt;br /&gt;
:&amp;lt;math&amp;gt;x&#039; = \sum_{k=1}^{\infty}\left\langle x,e_k\right\rangle e_k, &amp;lt;/math&amp;gt;&lt;br /&gt;
consisting of &#039;infinite sum&#039; of [[vector resolute]] &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; in direction &amp;lt;math&amp;gt;e_k&amp;lt;/math&amp;gt;, Bessel&#039;s [[inequality (mathematics)|inequality]] tells us that this [[series (mathematics)|series]] [[Limit of a sequence|converges]]. One can think of it that there exists &amp;lt;math&amp;gt;x&#039; \in H&amp;lt;/math&amp;gt; which can be described in terms of potential basis &amp;lt;math&amp;gt;e_1, e_2, ...&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
For a complete orthonormal sequence (that is, for an orthonormal sequence which is a [[Orthonormal basis|basis]]), we have [[Parseval&#039;s identity]], which replaces the inequality with an equality (and consequently &amp;lt;math&amp;gt; x&#039;&amp;lt;/math&amp;gt; with &amp;lt;math&amp;gt; x&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Bessel&#039;s inequality follows from the identity:&lt;br /&gt;
:&amp;lt;math&amp;gt;0 \le \left\| x - \sum_{k=1}^n \langle x, e_k \rangle e_k\right\|^2 = \|x\|^2 - 2 \sum_{k=1}^n |\langle x, e_k \rangle |^2 + \sum_{k=1}^n | \langle x, e_k \rangle |^2 = \|x\|^2 - \sum_{k=1}^n | \langle x, e_k \rangle |^2,&amp;lt;/math&amp;gt;&lt;br /&gt;
which holds for any natural &#039;&#039;n&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Cauchy–Schwarz inequality]]&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* {{springer|title=Bessel inequality|id=p/b015850}}&lt;br /&gt;
* [http://mathworld.wolfram.com/BesselsInequality.html Bessel&#039;s Inequality] the article on Bessel&#039;s Inequality on MathWorld.&lt;br /&gt;
&lt;br /&gt;
{{PlanetMath attribution|title=Bessel inequality|id=3089}}&lt;br /&gt;
&lt;br /&gt;
{{Functional Analysis}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Hilbert space]]&lt;br /&gt;
[[Category:Inequalities]]&lt;/div&gt;</summary>
		<author><name>165.124.128.146</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Jacobi_form&amp;diff=24570</id>
		<title>Jacobi form</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Jacobi_form&amp;diff=24570"/>
		<updated>2013-08-11T17:30:36Z</updated>

		<summary type="html">&lt;p&gt;165.124.167.212: /* Definition */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;effective diffusion coefficient&#039;&#039;&#039; (also referred to as the apparent diffusion coefficient) of a diffusant in [[atomic diffusion]] of solid [[polycrystalline]] materials like [[metal alloy]]s is often represented as a [[weighted average]] of the [[grain boundary diffusion coefficient]] and the [[lattice diffusion coefficient]].&amp;lt;ref name=Heitjans&amp;gt;P. Heitjans, J. Karger, Ed, “Diffusion in condensed matter: Methods, Materials, Models,” 2nd edition, Birkhauser, 2005, pp. 1-965.&amp;lt;/ref&amp;gt;  Diffusion along both the grain boundary and in the lattice may be modeled with an [[Arrhenius equation]]. The ratio of the grain boundary diffusion activation energy over the lattice diffusion activation energy is usually 0.4 - 0.6, so as temperature is lowered, the grain boundary diffusion component increases.&amp;lt;ref name=Heitjans /&amp;gt;  Increasing temperature often allows for increased grain size, and the lattice diffusion component increases with increasing temperature, so often at 0.8T&amp;lt;sub&amp;gt;melt&amp;lt;/sub&amp;gt; (of an alloy), the grain boundary component can be neglected.  &lt;br /&gt;
&lt;br /&gt;
==Modeling==&lt;br /&gt;
The effective diffusion coefficient can be modeled using Hart&#039;s equation when only grain boundary and lattice diffusion are dominant:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; {D^{\mathrm{eff}}} = f&amp;lt;/math&amp;gt; D&amp;lt;sub&amp;gt;gb&amp;lt;/sub&amp;gt; &amp;lt;math&amp;gt; + (1-f) &amp;lt;/math&amp;gt;D&amp;lt;sub&amp;gt;l&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
:&amp;lt;math&amp;gt; {D^{\mathrm{eff}}} = &amp;lt;/math&amp;gt; effective diffusion coefficient.&lt;br /&gt;
:D&amp;lt;sub&amp;gt;gb&amp;lt;/sub&amp;gt; = grain boundary diffusion coefficient.&lt;br /&gt;
:D&amp;lt;sub&amp;gt;l&amp;lt;/sub&amp;gt; = lattice diffusion coefficient.&lt;br /&gt;
:&amp;lt;math&amp;gt; f = \tfrac{q}{d} &amp;lt;/math&amp;gt;.δ&lt;br /&gt;
:&amp;lt;math&amp;gt; q = &amp;lt;/math&amp;gt; value based on grain shape, 1 for parallel grains, 3 for square grains.&lt;br /&gt;
:&amp;lt;math&amp;gt; d = &amp;lt;/math&amp;gt; average grain size.&lt;br /&gt;
:δ &amp;lt;math&amp;gt; = &amp;lt;/math&amp;gt; grain boundary width,often assumed to be 0.5 nm.&lt;br /&gt;
&lt;br /&gt;
Grain boundary diffusion is significant in [[face centered cubic]] metals below about 0.8 T&amp;lt;sub&amp;gt;melt&amp;lt;/sub&amp;gt; (Absolute). Line dislocations and other [[Crystallographic defect|crystalline defects]] can become significant below ~0.4 T&amp;lt;sub&amp;gt;melt&amp;lt;/sub&amp;gt; in FCC metals.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
{{refbegin}}&lt;br /&gt;
{{refend}}&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Kirkendall effect]]&lt;br /&gt;
* [[Phase transformations in solids]]&lt;br /&gt;
* [[Mass diffusivity]]&lt;br /&gt;
&lt;br /&gt;
[[Category:Diffusion]]&lt;/div&gt;</summary>
		<author><name>165.124.167.212</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Wendel%27s_theorem&amp;diff=25681</id>
		<title>Wendel&#039;s theorem</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Wendel%27s_theorem&amp;diff=25681"/>
		<updated>2013-05-25T00:45:07Z</updated>

		<summary type="html">&lt;p&gt;165.124.40.223: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In mathematics, the &#039;&#039;&#039;uncertainty exponent&#039;&#039;&#039; is a method of measuring the [[fractal dimension]] of a [[basin boundary]].  In a [[chaotic scattering]] system, the &lt;br /&gt;
[[invariant (mathematics)#Invariant set|invariant set]] of the system is usually not directly accessible because it is non-attracting and typically of [[measure (mathematics)|measure]] zero.  Therefore, the only way to infer the presence of members&lt;br /&gt;
and to measure the properties of the invariant set  is through the [[basin of attraction|basins of attraction]].  Note that in a scattering system, basins of attraction are not limit cycles therefore do not constitute members of the invariant set.&lt;br /&gt;
&lt;br /&gt;
Suppose we start with a random trajectory and perturb it by a small amount,&lt;br /&gt;
&amp;lt;math&amp;gt;\epsilon&amp;lt;/math&amp;gt;, in a random direction.  If the new trajectory ends up&lt;br /&gt;
in a different basin from the old one, then it is called &#039;&#039;epsilon uncertain&#039;&#039;.&lt;br /&gt;
If we take a large number of such trajectories,&lt;br /&gt;
then the fraction of them that are epsilon uncertain is the &#039;&#039;uncertainty fraction&#039;&#039;,&lt;br /&gt;
&amp;lt;math&amp;gt;f(\epsilon)&amp;lt;/math&amp;gt;, and we expect it to scale exponentially&lt;br /&gt;
with &amp;lt;math&amp;gt;\varepsilon&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
f(\varepsilon) \sim \varepsilon^\gamma \,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus the uncertainty exponent, &amp;lt;math&amp;gt;\gamma&amp;lt;/math&amp;gt;, is defined as follows:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\gamma = \lim_{\varepsilon\to 0} \frac {\ln f(\varepsilon)} {\ln \varepsilon}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The uncertainty exponent can be shown to approximate the [[box-counting dimension]]&lt;br /&gt;
as follows:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
D_0 = N - \gamma \, &lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;N&#039;&#039; is the embedding dimension.  Please refer to the article on [[chaotic mixing]] for an example of numerical computation of the &#039;&#039;uncertainty dimension&#039;&#039;&lt;br /&gt;
compared with that of a box-counting dimension.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*C. Grebogi, S. W. McDonald, E. Ott and J. A. Yorke, &#039;&#039;Final state sensitivity: An obstruction to predictability&#039;&#039;, [[Phys. Letters]] 99A: 415-418 (1983).&lt;br /&gt;
&lt;br /&gt;
* {{Cite book&lt;br /&gt;
 | author = Edward Ott&lt;br /&gt;
 | title = Chaos in Dynamical Systems&lt;br /&gt;
 | publisher = Cambridge University Press&lt;br /&gt;
 | year = 1993&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Chaos theory]]&lt;br /&gt;
[[Category:Fractals]]&lt;/div&gt;</summary>
		<author><name>165.124.40.223</name></author>
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		<updated>2012-08-01T16:24:32Z</updated>

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