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 <title>Biot-Savart law</title>
 <name>BiotSavartLaw</name>
 <created>2006-01-14 18:47:52</created>
 <modified>2006-01-14 18:48:31</modified>
 <type>Law</type>
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	<category scheme="msc" code="41.20.Gz"/>
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 <content>The Biot-Savart law is a physical law with applications in both electromagnetism and aerodynamics. As originally formulated, the law describes the magnetic field set up by a steady current density. More recently, by a simple analogy between magnetostatics and fluid dynamics, the same law has been used to calculate the velocity of air induced by vortex lines in aerodynamic systems.

The Biot-Savart law is fundamental to magnetostatics just as Coulomb's law is to electrostatics. The Biot-Savart law follows from and is fully consistent with Ampère's law, much as Coulomb's law follows from Gauss' law.

In particular, if we define a differential element of current

$$I d{\bf l} $$

then the corresponding differential element of magnetic field is

$$ d{\bf B} = \frac{\mu_0}{4 \pi}\frac{I {\bf dl} \times {\bf\hat{r}}}{r^2} $$

where

I is the current, measured in amperes

$\hat{r}$ is the unit displacement vector from the element to the field point and the integral is over the current distribution

This entry is a derivative of the  Biot-Savart law article \PMlinkexternal{from Wikipedia, the Free Encyclopedia}{http://en.wikipedia.org/wiki/Biot-Savart\%27s_Law}.  Authors of the orginial article include: Salsb, Tim Starling, Metacomet, JabberWok and Toby Bartels.  History page of the original is \PMlinkexternal{here}{http://en.wikipedia.org/w/index.php?title=Biot-Savart_law\&amp;action=history}

{\bf References }

[2] Jackson, D.  "Classical Electrodynamics", John Wiley and Sons, Inc., 1975.</content>
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