## The Biot-Savart Law

What I’m going to present is slightly different from what usually gets called the Biot-Savart law, but I think it’s the most natural parallel to the Coulomb law. As far as I can tell, it doesn’t get stressed all that much in modern coverage; in the first course I took on electromagnetism way back in the summer of 1994 I didn’t even see the name written down and parsed what I heard as “bee-ohs of r”. So at least you know how it’s supposed to be pronounced.

If we have two charged particles that are both moving, then they also feel a different force than the electric one. We call the excess the magnetic force. In magnitude it’s proportional to both the magnitudes of the charges and their speeds, and inversely proportional to the square of the distance between them, and then it gets complicated. It’s probably going to be easier to write this down as a formula first.

So many cross products! Like last time, this is the force exerted on the first particle by the second; is the vector pointing from the second particle to the first, and is the unit vector pointing in the same direction. From this formula, we see that the force is perpendicular to the direction the first particle is moving — the magnetic force can only turn a particle, not speed it up or slow it down — and in the plane spanned by the direction the second particle is moving and the displacement vector between them.

Again, we’ve written the constant of proportionality in a weird way. The “magnetic constant” now appears in the numerator, so its units are almost like the inverse of those on the electric constant. But we’ve also got two velocities to contend with; these lead to a factor of time squared over area, resulting in mass times distance over charge squared. In the SI system we have another convenience unit called the “henry”, with symbol , defined by

which lets us write in units of henries per meter. Specifically, the SI units give it a value of . Yes, I know that this makes the proportionality constant look that much weirder, since it just works out to , but still.

I read all your posts. Thanks for starting posts on electro-magnetic applications. I am looking forward to seeing how generalized Stokes’ theorem is applied to them.

Comment by Soma Murthy | January 4, 2012 |

[...] of the reason that the Biot-Savart law isn’t usually stated in the way I did is that it’s really about currents, which are [...]

Pingback by Currents « The Unapologetic Mathematician | January 7, 2012 |

[...] so the Biot-Savart law says that the differential contribution to the magnetic field at a point from the current density [...]

Pingback by Gauss’ Law for Magnetism « The Unapologetic Mathematician | January 12, 2012 |

[...] Biot-Savart law says that electric currents give rise to a magnetic field. Given the current distribution we have [...]

Pingback by Maxwell’s Equations « The Unapologetic Mathematician | February 1, 2012 |

[...] get the Biot-Savart law, we can use Ampère’s law to calculate the magnetic field around an infinitely long straight [...]

Pingback by Deriving Physics from Maxwell’s Equations « The Unapologetic Mathematician | February 3, 2012 |

[...] Armstrong: Too many to list! A very small sample chosen mostly at random: Coulomb’s Law, The Biot-Savart Law, Currents, Gauss’ Law for Magnetism, Faraday’s Law, Conservation of Charge, Deriving [...]

Pingback by Fourteenth Linkfest | February 6, 2012 |

we can not find in this the other name of biot savart law.

Comment by vipul wani | August 5, 2012 |