Ampère's circuital law
Electromagnetism 


In classical electromagnetism, Ampère's circuital law (not to be confused with Ampère's force law that AndréMarie Ampère discovered in 1823^{[1]}) relates the integrated magnetic field around a closed loop to the electric current passing through the loop. James Clerk Maxwell (not Ampère) derived it using hydrodynamics in his 1861 paper "On Physical Lines of Force"^{[2]} and it is now one of the Maxwell equations, which form the basis of classical electromagnetism.
Maxwell's original circuital law
The original form of Maxwell's circuital law, which he derived in his 1855 paper "On Faraday's Lines of Force"^{[3]} based on an analogy to hydrodynamics, relates magnetic fields to electric currents that produce them. It determines the magnetic field associated with a given current, or the current associated with a given magnetic field.
The original circuital law is only a correct law of physics in a magnetostatic situation, where the system is static except possibly for continuous steady currents within closed loops. For systems with electric fields that change over time, the original law (as given in this section) must be modified to include a term known as Maxwell's correction (see below).
Equivalent forms
The original circuital law can be written in several different forms, which are all ultimately equivalent:
 An "integral form" and a "differential form". The forms are exactly equivalent, and related by the Kelvin–Stokes theorem.(see the "proof" section below)
 Forms using SI units, and those using cgs units. Other units are possible, but rare. This section will use SI units, with cgs units discussed later.
 Forms using either B or H magnetic fields. These two forms use the total current density and free current density, respectively. The B and H fields are related by the constitutive equation: B = μ_{0}H where μ_{0} is the magnetic constant.
Explanation
The integral form of the original circuital law is a line integral of the magnetic field around some closed curve C (arbitrary but must be closed). The curve C in turn bounds both a surface S which the electric current passes through (again arbitrary but not closed—since no threedimensional volume is enclosed by S), and encloses the current. The mathematical statement of the law is a relation between the total amount of magnetic field around some path (line integral) due to the current which passes through that enclosed path (surface integral).^{[4]}^{[5]}
In terms of total current, (which is the sum of both free current and bound current) the line integral of the magnetic Bfield (in teslas, T) around closed curve C is proportional to the total current I_{enc} passing through a surface S (enclosed by C). In terms of free current, the line integral of the magnetic Hfield (in amperes per metre, A·m^{−1}) around closed curve C equals the free current I_{f,enc} through a surface S.
Forms of the original circuital law written in SI units Integral form Differential form Using Bfield and total current Using Hfield and free current
 J is the total current density (in amperes per square metre, A·m^{−2}),
 J_{f} is the free current density only,
 ∮_{C} is the closed line integral around the closed curve C,
 ∬_{S} denotes a 2D surface integral over S enclosed by C,
 · is the vector dot product,
 dl is an infinitesimal element (a differential) of the curve C (i.e. a vector with magnitude equal to the length of the infinitesimal line element, and direction given by the tangent to the curve C)
 dS is the vector area of an infinitesimal element of surface S (that is, a vector with magnitude equal to the area of the infinitesimal surface element, and direction normal to surface S. The direction of the normal must correspond with the orientation of C by the right hand rule), see below for further explanation of the curve C and surface S.
 ∇ × is the curl operator.
Ambiguities and sign conventions
There are a number of ambiguities in the above definitions that require clarification and a choice of convention.
 First, three of these terms are associated with sign ambiguities: the line integral ∮_{C} could go around the loop in either direction (clockwise or counterclockwise); the vector area dS could point in either of the two directions normal to the surface; and I_{enc} is the net current passing through the surface S, meaning the current passing through in one direction, minus the current in the other direction—but either direction could be chosen as positive. These ambiguities are resolved by the righthand rule: With the palm of the righthand toward the area of integration, and the indexfinger pointing along the direction of lineintegration, the outstretched thumb points in the direction that must be chosen for the vector area dS. Also the current passing in the same direction as dS must be counted as positive. The right hand grip rule can also be used to determine the signs.
 Second, there are infinitely many possible surfaces S that have the curve C as their border. (Imagine a soap film on a wire loop, which can be deformed by moving the wire). Which of those surfaces is to be chosen? If the loop does not lie in a single plane, for example, there is no one obvious choice. The answer is that it does not matter; it can be proven that any surface with boundary C can be chosen.
Free current versus bound current
The electric current that arises in the simplest textbook situations would be classified as "free current"—for example, the current that passes through a wire or battery. In contrast, "bound current" arises in the context of bulk materials that can be magnetized and/or polarized. (All materials can to some extent.)
When a material is magnetized (for example, by placing it in an external magnetic field), the electrons remain bound to their respective atoms, but behave as if they were orbiting the nucleus in a particular direction, creating a microscopic current. When the currents from all these atoms are put together, they create the same effect as a macroscopic current, circulating perpetually around the magnetized object. This magnetization current J_{M} is one contribution to "bound current".
The other source of bound current is bound charge. When an electric field is applied, the positive and negative bound charges can separate over atomic distances in polarizable materials, and when the bound charges move, the polarization changes, creating another contribution to the "bound current", the polarization current J_{P}.
The total current density J due to free and bound charges is then:
with J_{f} the "free" or "conduction" current density.
All current is fundamentally the same, microscopically. Nevertheless, there are often practical reasons for wanting to treat bound current differently from free current. For example, the bound current usually originates over atomic dimensions, and one may wish to take advantage of a simpler theory intended for larger dimensions. The result is that the more microscopic Ampère's circuital law, expressed in terms of B and the microscopic current (which includes free, magnetization and polarization currents), is sometimes put into the equivalent form below in terms of H and the free current only. For a detailed definition of free current and bound current, and the proof that the two formulations are equivalent, see the "proof" section below.
Shortcomings of the original formulation of the circuital law
There are two important issues regarding the circuital law that require closer scrutiny. First, there is an issue regarding the continuity equation for electrical charge. In vector calculus, the identity for the divergence of a curl states that a vector field's curl divergence must always be zero. Hence
and so the original Ampère's circuital law implies that
But in general, reality follows the continuity equation for electric charge:
which is nonzero for a timevarying charge density. An example occurs in a capacitor circuit where timevarying charge densities exist on the plates.^{[6]}^{[7]}^{[8]}^{[9]}^{[10]}
Second, there is an issue regarding the propagation of electromagnetic waves. For example, in free space, where
The circuital law implies that
but experimental tests actually show that
To treat these situations, the contribution of displacement current must be added to the current term in the circuital law.
James Clerk Maxwell conceived of displacement current as a polarization current in the dielectric vortex sea, which he used to model the magnetic field hydrodynamically and mechanically.^{[11]} He added this displacement current to Ampère's circuital law at equation 112 in his 1861 paper On Physical Lines of Force.^{[12]}
Displacement current
In free space, the displacement current is related to the time rate of change of electric field.
In a dielectric the above contribution to displacement current is present too, but a major contribution to the displacement current is related to the polarization of the individual molecules of the dielectric material. Even though charges cannot flow freely in a dielectric, the charges in molecules can move a little under the influence of an electric field. The positive and negative charges in molecules separate under the applied field, causing an increase in the state of polarization, expressed as the polarization density P. A changing state of polarization is equivalent to a current.
Both contributions to the displacement current are combined by defining the displacement current as:^{[6]}
where the electric displacement field is defined as:
where ε_{0} is the electric constant, ε_{r} the relative static permittivity, and P is the polarization density. Substituting this form for D in the expression for displacement current, it has two components:
The first term on the right hand side is present everywhere, even in a vacuum. It doesn't involve any actual movement of charge, but it nevertheless has an associated magnetic field, as if it were an actual current. Some authors apply the name displacement current to only this contribution.^{[13]}
The second term on the right hand side is the displacement current as originally conceived by Maxwell, associated with the polarization of the individual molecules of the dielectric material.
Maxwell's original explanation for displacement current focused upon the situation that occurs in dielectric media. In the modern postaether era, the concept has been extended to apply to situations with no material media present, for example, to the vacuum between the plates of a charging vacuum capacitor. The displacement current is justified today because it serves several requirements of an electromagnetic theory: correct prediction of magnetic fields in regions where no free current flows; prediction of wave propagation of electromagnetic fields; and conservation of electric charge in cases where charge density is timevarying. For greater discussion see Displacement current.
Extending the original law: the Maxwell–Ampère equation
Next, the circuital equation is extended by including the polarization current, thereby remedying the limited applicability of the original circuital law.
Treating free charges separately from bound charges, The equation including Maxwell's correction in terms of the Hfield is (the Hfield is used because it includes the magnetization currents, so J_{M} does not appear explicitly, see Hfield and also Note):^{[14]}
(integral form), where H is the magnetic H field (also called "auxiliary magnetic field", "magnetic field intensity", or just "magnetic field"), D is the electric displacement field, and J_{f} is the enclosed conduction current or free current density. In differential form,
On the other hand, treating all charges on the same footing (disregarding whether they are bound or free charges), the generalized Ampère's equation, also called the Maxwell–Ampère equation, is in integral form (see the "proof" section below):
In differential form,
In both forms J includes magnetization current density^{[15]} as well as conduction and polarization current densities. That is, the current density on the right side of the Ampère–Maxwell equation is:
where current density J_{D} is the displacement current, and J is the current density contribution actually due to movement of charges, both free and bound. Because ∇ ⋅ D = ρ, the charge continuity issue with Ampère's original formulation is no longer a problem.^{[16]} Because of the term in ε_{0}∂E/∂t, wave propagation in free space now is possible.
With the addition of the displacement current, Maxwell was able to hypothesize (correctly) that light was a form of electromagnetic wave. See electromagnetic wave equation for a discussion of this important discovery.
Proof of equivalence
Proof that the formulations of the circuital law in terms of free current are equivalent to the formulations involving total current. In this proof, we will show that the equation is equivalent to the equation
Note that we are only dealing with the differential forms, not the integral forms, but that is sufficient since the differential and integral forms are equivalent in each case, by the Kelvin–Stokes theorem.
We introduce the polarization density P, which has the following relation to E and D:
Next, we introduce the magnetization density M, which has the following relation to B and H:
and the following relation to the bound current:
where
is called the magnetization current density, and
is the polarization current density. Taking the equation for B:
Consequently, referring to the definition of the bound current:
as was to be shown.
Ampère's circuital law in cgs units
In cgs units, the integral form of the equation, including Maxwell's correction, reads
where c is the speed of light.
The differential form of the equation (again, including Maxwell's correction) is
See also
Notes
 ↑ Ampère never utilized the field concept in any of his works; cf. Assis, André Koch Torres; Chaib, J. P. M. C; Ampère, AndréMarie (2015). Ampère's electrodynamics: analysis of the meaning and evolution of Ampère's force between current elements, together with a complete translation of his masterpiece: Theory of electrodynamic phenomena, uniquely deduced from experience (PDF). Montreal, QC: Apeiron. ch. 15 p. 221. ISBN 9781987980035. The "Ampère circuital law" is thus more properly termed the "AmpèreMaxwell law." It is named after Ampère because of his contributions to understanding electric current. Maxwell does not take Ampère's force law as a starting point in deriving any of his equations, although he mentions Ampère's force law in his A Treatise on Electricity and Magnetism vol. 2, part 4, ch. 2 (§§502527) & 23 (§§845866).
 ↑ Clerk Maxwell, James. "On Physical Lines of Force".
 ↑ Clerk Maxwell, James. "On Faraday's Lines of Force".
 ↑ Knoepfel, Heinz E. (2000). Magnetic Fields: A comprehensive theoretical treatise for practical use. Wiley. p. 4. ISBN 0471322059.
 ↑ Owen, George E. (2003). Electromagnetic Theory (Reprint of 1963 ed.). CourierDover Publications. p. 213. ISBN 0486428303.
 1 2 Jackson, John David (1999). Classical Electrodynamics (3rd ed.). Wiley. p. 238. ISBN 047130932X.
 ↑ Griffiths, David J. (1999). Introduction to Electrodynamics (3rd ed.). Pearson/AddisonWesley. pp. 322–323. ISBN 013805326X.
 ↑ Owen, George E. (2003). Electromagnetic Theory. Mineola, NY: Dover Publications. p. 285. ISBN 0486428303.
 ↑ Billingham, J.; King, A. C. (2006). Wave Motion. Cambridge University Press. p. 179. ISBN 0521634504.
 ↑ Slater, J. C.; Frank, N. H. (1969). Electromagnetism (Reprint of 1947 ed.). Courier Dover Publications. p. 83. ISBN 0486622630.
 ↑ Siegel, Daniel M. (2003). Innovation in Maxwell's Electromagnetic Theory: Molecular Vortices, Displacement Current, and Light. Cambridge University Press. pp. 96–98. ISBN 0521533295.
 ↑ Clerk Maxwell, James (1861). "On Physical Lines of Force" (PDF). Philosophical Magazine and Journal of Science.
 ↑ For example, see Griffiths, David J. (1999). Introduction to Electrodynamics. Upper Saddle River, NJ: Prentice Hall. p. 323. ISBN 013805326X. and Tai L. Chow (2006). Introduction to Electromagnetic Theory. Jones & Bartlett. p. 204. ISBN 0763738271.
 ↑ Rogalski, Mircea S.; Palmer, Stuart B. (2006). Advanced University Physics. CRC Press. p. 267. ISBN 1584885114.
 ↑ Rogalski, Mircea S.; Palmer, Stuart B. (2006). Advanced University Physics. CRC Press. p. 251. ISBN 1584885114.
 ↑ The magnetization current can be expressed as the curl of the magnetization, so its divergence is zero and it does not contribute to the continuity equation. See magnetization current.
Further reading
 Griffiths, David J. (1998). Introduction to Electrodynamics (3rd ed.). Prentice Hall. ISBN 013805326X.
 Tipler, Paul (2004). Physics for Scientists and Engineers: Electricity, Magnetism, Light, and Elementary Modern Physics (5th ed.). W. H. Freeman. ISBN 0716708108.
External links
 Simple Nature by Benjamin Crowell Ampere's law from an online textbook
 MISN0138 Ampere's Law (PDF file) by Kirby Morgan for Project PHYSNET.
 MISN0145 The Ampere–Maxwell Equation; Displacement Current (PDF file) by J.S. Kovacs for Project PHYSNET.
 The Ampère's Law Song (PDF file) by Walter Fox Smith; Main page, with recordings of the song.
 A Dynamical Theory of the Electromagnetic Field Maxwell's paper of 1864