In magnetostatics, the force of attraction or repulsion between two current-carrying wires (see first figure below) is often called Ampère's force law. The physical origin of this force is that each wire generates a magnetic field, following the Biot–Savart law, and the other wire experiences a magnetic force as a consequence, following the Lorentz force law.

Equation

Special case: Two straight parallel wires

The best-known and simplest example of Ampère's force law, which underlaid (before 20 May 2019 ) the definition of the ampere, the SI unit of electric current, states that the magnetic force per unit length between two straight parallel conductors is where k_{\rm A} is the magnetic force constant from the Biot–Savart law, F_m / L is the total force on either wire per unit length of the shorter (the longer is approximated as infinitely long relative to the shorter), r is the distance between the two wires, and I_1, I_2 are the direct currents carried by the wires. This is a good approximation if one wire is sufficiently longer than the other, so that it can be approximated as infinitely long, and if the distance between the wires is small compared to their lengths (so that the one infinite-wire approximation holds), but large compared to their diameters (so that they may also be approximated as infinitely thin lines). The value of k_{\rm A} depends upon the system of units chosen, and the value of k_{\rm A} decides how large the unit of current will be. In the SI system, with \mu_0 the magnetic constant, in SI units μ0 = 1.257 H/m

General case

The general formulation of the magnetic force for arbitrary geometries is based on iterated line integrals and combines the Biot–Savart law and Lorentz force in one equation as shown below. where To determine the force between wires in a material medium, the magnetic constant is replaced by the actual permeability of the medium. For the case of two separate closed wires, the law can be rewritten in the following equivalent way by expanding the vector triple product and applying Stokes' theorem: In this form, it is immediately obvious that the force on wire 1 due to wire 2 is equal and opposite the force on wire 2 due to wire 1, in accordance with Newton's third law of motion.

Historical background

The form of Ampere's force law commonly given was derived by James Clerk Maxwell in 1873 and is one of several expressions consistent with the original experiments of André-Marie Ampère and Carl Friedrich Gauss. The x-component of the force between two linear currents I and I, as depicted in the adjacent diagram, was given by Ampère in 1825 and Gauss in 1833 as follows: Following Ampère, a number of scientists, including Wilhelm Weber, Rudolf Clausius, Maxwell, Bernhard Riemann, Hermann Grassmann, and Walther Ritz, developed this expression to find a fundamental expression of the force. Through differentiation, it can be shown that: and also the identity: With these expressions, Ampère's force law can be expressed as: Using the identities: and Ampère's results can be expressed in the form: As Maxwell noted, terms can be added to this expression, which are derivatives of a function Q(r) and, when integrated, cancel each other out. Thus, Maxwell gave "the most general form consistent with the experimental facts" for the force on ds arising from the action of ds ': Q is a function of r, according to Maxwell, which "cannot be determined, without assumptions of some kind, from experiments in which the active current forms a closed circuit." Taking the function Q(r) to be of the form: We obtain the general expression for the force exerted on ds by ds: Integrating around s ' eliminates k and the original expression given by Ampère and Gauss is obtained. Thus, as far as the original Ampère experiments are concerned, the value of k has no significance. Ampère took k=−1; Gauss took k=+1, as did Grassmann and Clausius, although Clausius omitted the S component. In the non-ethereal electron theories, Weber took k=−1 and Riemann took k=+1. Ritz left k undetermined in his theory. If we take k = −1, we obtain the Ampère expression: If we take k=+1, we obtain Using the vector identity for the triple cross product, we may express this result as When integrated around ds ' the second term is zero, and thus we find the form of Ampère's force law given by Maxwell:

Derivation of parallel straight wire case from general formula

Start from the general formula: Assume wire 2 is along the x-axis, and wire 1 is at y=D, z=0, parallel to the x-axis. Let x_1,x_2 be the x-coordinate of the differential element of wire 1 and wire 2, respectively. In other words, the differential element of wire 1 is at (x_1,D,0) and the differential element of wire 2 is at (x_2,0,0). By properties of line integrals, and. Also, and Therefore, the integral is Evaluating the cross-product: Next, we integrate x_2 from -\infty to +\infty: If wire 1 is also infinite, the integral diverges, because the total attractive force between two infinite parallel wires is infinity. In fact, what we really want to know is the attractive force per unit length of wire 1. Therefore, assume wire 1 has a large but finite length L_1. Then the force vector felt by wire 1 is: As expected, the force that the wire feels is proportional to its length. The force per unit length is: The direction of the force is along the y-axis, representing wire 1 getting pulled towards wire 2 if the currents are parallel, as expected. The magnitude of the force per unit length agrees with the expression for shown above.

Notable derivations

Chronologically ordered:

References and notes