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		<title>Effective mode volume</title>
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		<summary type="html">&lt;p&gt;81.97.28.57: &lt;/p&gt;
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&lt;div&gt; {{See also|Mode volume}}&lt;br /&gt;
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For an [[optical fiber]], the &#039;&#039;&#039;effective mode volume&#039;&#039;&#039; is the square of the product of the diameter of the [[Near and far field|near-field]] pattern and the sine of the [[radiation angle]] of the [[Near and far field|far-field]] pattern. The diameter of the near-field [[radiation pattern]] is defined here as the [[full width at half maximum]] and the radiation angle at half maximum [[radiant intensity]]. Effective [[Transverse mode|mode]] volume is [[Proportionality (mathematics)|proportional]] to the breadth of the relative distribution of [[Power (physics)|power]] amongst the modes in a multimode fiber. It is not truly a spatial volume but rather an &#039;&#039;&amp;quot;optical volume&amp;quot;&#039;&#039; equal to the product of area and solid angle. The power divided by the effective mode volume is proportional to the [[radiance]] of the light emitted by the fiber.&lt;br /&gt;
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==References==&lt;br /&gt;
*{{FS1037C}}&lt;br /&gt;
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[[Category:Fiber optics]]&lt;/div&gt;</summary>
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