Biot-Savart law
Biot-Savart law, in physics, a fundamental quantitative relationship between an electric current I and the magnetic field B it produces, based on the experiments in 1820 of the French scientists Jean-Baptiste Biot and Félix Savart.
A current in a loop produces magnetic field lines B that form loops around the current. The Biot-Savart law expresses the partial contribution dB from a small segment of conductor to the total B field of a current in the conductor. For a segment of conductor of length and orientation dl that carries a current i,dB = μ0/4π Idl × r̂/r2.In this equation, μ0 is the permeability of free space and has the value of 4π × 10−7 newton per square ampere.
This equation is illustrated for a small segment of a wire that carries a current so that, at the origin of the coordinate system, the small segment of length dl of the wire lies along the x axis. Comparing dB at points 1 and 2 shows the inverse square dependence of the magnitude of the field with distance. The vectors at points 1, 3, and 4, which are all at the same distance from dl, show the direction of dB in a circle around the wire. In position 1, the contribution to the field, dB1, is perpendicular both to the current direction and to the vector r1. Finally, the vectors at 1, 5, 6, and 7 illustrate the angular dependence of the magnitude of dB at a point. The magnitude of dB varies as the sine of the angle between dl and r̂, where r̂ is in the direction from dl to the point. It is strongest at 90° to dl and decreases to zero for locations directly in line with dl. The magnetic field of a current in a loop or coil is obtained by summing the individual partial contributions of all the segments of the circuits, taking into account the vector nature of the field. While simple mathematical expressions for the magnetic field can be derived for a few current configurations, most practical applications require the use of high-speed computers.
The expression for the magnetic field B a distance r from a long straight wire with current I isB = μ0I/2πr θwhere θ is a unit vector pointing in a circle around the wire. That is, the value of the magnetic field B at a point nearby is directly proportional to the value of the current I and inversely proportional to the perpendicular distance r from the wire to the given point. (Compare Ampère’s law.)