Ampère's force law

This article is about Ampère's force law. For the law relating the integrated magnetic field around a closed loop to the electric current through the loop, see Ampère's circuital law.

Electromagnetism

Electricity Magnetism
Electrostatics Electric charge Static electricity Electric field Conductor Insulator Triboelectricity Electrostatic discharge Induction Coulomb's law Gauss's law Electric flux / potential energy Electric dipole moment Polarization density
Magnetostatics Ampère's law Magnetic field Magnetization Magnetic flux Biot–Savart law Magnetic dipole moment Gauss's law for magnetism
Electrodynamics Lorentz force law Electromagnetic induction Faraday's law Lenz's law Displacement current Magnetic potential Maxwell's equations Electromagnetic field Electromagnetic radiation Maxwell tensor Poynting vector Liénard–Wiechert potential Jefimenko's equations Eddy current London equations Mathematical descriptions of the electromagnetic field
Electrical network Electric current Electric potential Voltage Resistance Ohm's law Series circuit Parallel circuit Direct current Alternating current Charged current Neutral current Electromotive force Capacitance Inductance Impedance Resonant cavities Waveguides
Covariant formulation Electromagnetic tensor (stress–energy tensor) Four-current Electromagnetic four-potential
Scientists Ampère Coulomb Faraday Gauss Heaviside Henry Hertz Lorentz Maxwell Tesla Volta Weber Ørsted

The top wire with current I₁ experiences a Lorentz force F₁₂ due to magnetic field B₂ created by the bottom wire. (Not shown is the simultaneous process where the bottom wire I₂ experiences a magnetic force F₂₁ due to magnetic field B₁ created by the top wire.)

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, as defined by the Biot–Savart law, and the other wire experiences a magnetic force as a consequence, as defined by the Lorentz force.

Equation

The best-known and simplest example of Ampère's force law, which underlies the definition of the ampere, the SI unit of current, states that the force per unit length between two straight parallel conductors is

{\frac {F_{m}}{L}}=2k_{A}{\frac {I_{1}I_{2}}{r}}

where k_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 I₁, I₂ are the direct currents carried by the wires.

This is a good approximation if one wire is sufficiently longer than the other 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_A depends upon the system of units chosen, and the value of k_A decides how large the unit of current will be. In the SI system,^[1] ^[2]

k_{A}\ {\overset {{\underset {{\mathrm {def}}}{}}}{=}}\ {\frac {\mu _{0}}{4\pi }}

with μ₀ the magnetic constant, defined in SI units as^[3]^[4]

\mu _{0}\ {\overset {{\underset {{\mathrm {def}}}{}}}{=}}\ 4\pi \times 10^{{-7}}

N / A².

Thus, in vacuum,

the force per meter of length between two parallel conductors – spaced apart by 1 m and each carrying a current of 1 A – is exactly

\displaystyle 2 \times 10^{-7}

N / m.

Demonstration of Ampère's force law. The force acts between two parallel conductors with constant currents passing through them. If they have the same direction, there is force of attraction, but if the directions are opposite, then the force is repellent. Performed by Prof. Oliver Zajkov at the Physics Institute at the Ss. Cyril and Methodius University of Skopje, Macedonia.

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. ^[5]

^[6]^[7]

\vec{F}_{12} = \frac {\mu_0} {4 \pi} \int_{L_1} \int_{L_2} \frac {I_1 d \vec{\ell}_1\ \mathbf{ \times} \ (I_2 d \vec{\ell}_2 \ \mathbf{ \times } \ \hat{\mathbf{r}}_{21} )} {|r|^2}

where

$\vec{F}_{12}$ is the total force felt by wire 1 due to wire 2 (usually measured in newtons),
I₁ and I₂ are the currents running through wires 1 and 2, respectively (usually measured in amperes),
The double line integration sums the force upon each element of wire 1 due to the magnetic field of each element of wire 2,
$d \vec{\ell}_1$ and $d \vec{\ell}_2$ are infinitesimal vectors associated with wire 1 and wire 2 respectively (usually measured in metres); see line integral for a detailed definition,
The vector $\hat{\mathbf{r}}_{21}$ is the unit vector pointing from the differential element on wire 2 towards the differential element on wire 1, and |r| is the distance separating these elements,
The multiplication × is a vector cross product,
The sign of I_n is relative to the orientation $d \vec{\ell}_n$ (for example, if $d \vec{\ell}_1$ points in the direction of conventional current, then I₁>0).

To determine the force between wires in a material medium, the magnetic constant is replaced by the actual permeability of the medium.

Historical background

Diagram of original Ampere experiment

The form of Ampere's force law commonly given was derived by Maxwell and is one of several expressions consistent with the original experiments of Ampère and 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:^[8]

dF_x = k I I' ds' \int ds \frac {\cos(xds) \cos(rds') - \cos(rx)\cos(dsds')} {r^2}.

Following Ampère, a number of scientists, including Wilhelm Weber, Rudolf Clausius, James Clerk Maxwell, Bernhard Riemann, and Walther Ritz, developed this expression to find a fundamental expression of the force. Through differentiation, it can be shown that:

\frac{\cos(xds) \cos(rds')} {r^2} = -\cos(rx) \frac{(\cos\epsilon - 3 \cos\phi \cos\phi')} {r^2}

and also the identity:

\frac{\cos(rx) \cos(dsds')} {r^2} = \frac{\cos(rx) \cos\epsilon} {r^2}

With these expressions, Ampère's force law can be expressed as:

dF_x = k I I' ds'\int ds' \cos(rx) \frac{2\cos\epsilon - 3\cos\phi \cos\phi'} {r^2}

Using the identities:

\frac{\partial r} {\partial s} = \cos\phi, \frac{\partial r} {\partial s'} = -\cos\phi'

and

\frac{\partial^2 r} {\partial s \partial s'} = \frac{-\cos\epsilon + \cos\phi \cos\phi'} {r}

Ampère's results can be expressed in the form:

d^2 F = \frac{k I I' ds ds'} {r^2} \left( \frac{\partial r}{\partial s} \frac{\partial r}{\partial s'} - 2r \frac{\partial^2 r}{\partial s \partial s'}\right)

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':^[9]

d^2 F_x = k I I' ds ds' \left[ \left( \frac{1} {r^2} \left( \frac{\partial r}{\partial s} \frac{\partial r}{\partial s'} - 2r \frac{\partial^2 r}{\partial s \partial s'}\right) + r \frac{\partial^2 Q}{\partial s \partial s'}\right) \cos(rx) + \frac{\partial Q} {\partial s'} \cos(xds) - \frac{\partial Q} {\partial s} \cos(xds') \right]

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:

Q = - \frac{(1+k)} {2r}

We obtain the general expression for the force exerted on ds by ds:

\mathbf{d^2F} = -\frac{k I I'} {2r^2} \left[ (3-k)\hat{\mathbf{r_1}} (\mathbf{dsds'}) - 3(1-k) \hat{\mathbf{r_1}} (\mathbf{\hat{r_1} ds}) (\mathbf{\hat{r_1} ds'}) - (1+k)\mathbf{ds} (\mathbf{\hat{r_1} ds'})-(1+k) \mathbf{d's} (\mathbf{\hat{r_1} ds}) \right]

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:

\mathbf{d^2F} = -\frac{k I I'} {r^3} \left[ 2 \mathbf{r} (\mathbf{dsds'}) - 3\mathbf{r} (\mathbf{r ds}) (\mathbf{r ds'}) \right]

If we take k=+1, we obtain

\mathbf{d^2F} = -\frac{k I I'} {r^3} \left[ \mathbf{r} (\mathbf{dsds'}) - \mathbf{ds (r ds')} -\mathbf{ds'(r ds)} \right]

Using the vector identity for the triple cross product, we may express this result as

\mathbf{d^2F} = \frac{k I I'} {r^3} \left[ \left(\mathbf{ds}\times\mathbf{ds'}\times\mathbf{r}\right)+ \mathbf{ds'(r ds)} \right]

When integrated around ds' the second term is zero, and thus we find the form of Ampère's force law given by Maxwell:

\mathbf{F} = k I I' \int \int \frac{\mathbf{ds}\times(\mathbf{ds'}\times\mathbf{r})} {|r|^3}

Derivation of parallel straight wire case from general formula

Start from the general formula:

\vec{F}_{12} = \frac {\mu_0} {4 \pi} \int_{L_1} \int_{L_2} \frac {I_1 d \vec{\ell}_1\ \mathbf{ \times} \ (I_2 d \vec{\ell}_2 \ \mathbf{ \times } \ \hat{\mathbf{r}}_{21} )} {|r|^2}

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, $d\vec{\ell}_1=(dx_1,0,0)$ and $d\vec{\ell}_2=(dx_2,0,0)$ . Also,

\hat{\mathbf{r}}_{21} = \frac{1}{\sqrt{(x_1-x_2)^2+D^2}}(x_1-x_2,D,0)

and

|r| = \sqrt{(x_1-x_2)^2+D^2}

Therefore the integral is

\vec{F}_{12} = \frac {\mu_0 I_1 I_2} {4 \pi} \int_{L_1} \int_{L_2} \frac {(dx_1,0,0)\ \mathbf{ \times} \ \left[ (dx_2,0,0) \ \mathbf{ \times } \ (x_1-x_2,D,0) \right ] } {|(x_1-x_2)^2+D^2|^{3/2}}

Evaluating the cross-product:

\vec{F}_{12} = \frac {\mu_0 I_1 I_2} {4 \pi} \int_{L_1} \int_{L_2} dx_1 dx_2 \frac {(0,-D,0)} {|(x_1-x_2)^2+D^2|^{3/2}}

Next, we integrate $x_{2}$ from $-\infty$ to $+\infty$ :

\vec{F}_{12} = \frac {\mu_0 I_1 I_2} {4 \pi}\frac{2}{D}(0,-1,0) \int_{L_1} dx_1

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:

\vec{F}_{12} = \frac {\mu_0 I_1 I_2} {4 \pi}\frac{2}{D}(0,-1,0) L_1

As expected, the force that the wire feels is proportional to its length. The force per unit length is:

\frac{\vec{F}_{12}}{L_1} = \frac {\mu_0 I_1 I_2} {2 \pi D}(0,-1,0)

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 ${\frac {F_{m}}{L}}$ shown above.

Famous Derivations of Ampère's Force Law

Chronologically ordered:

Ampère's original 1823 derivation:
- Assis, André Koch Torres; Chaib, J. P. M. C; Ampère, André-Marie (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: Apeiron. ISBN 978-1-987980-03-5.
Maxwell's 1873 derivation:
- Treatise on Electricity and Magnetism vol. 2, part 4, ch. 2 (§§502-527)
Pierre Duhem's 1892 derivation:
- Leçons sur l'électricité et le magnétisme vol. 3, appendix to book 14, pp. 309-332 (French)
Alfred O'Rahilly's 1938 derivation:
- Electromagnetic Theory: A Critical Examination of Fundamentals vol. 1, pp. 102-104 (cf. the following pages, too)

References and notes

↑ Raymond A Serway & Jewett JW (2006). Serway's principles of physics: a calculus based text (Fourth ed.). Belmont, California: Thompson Brooks/Cole. p. 746. ISBN 0-534-49143-X.
↑ Paul M. S. Monk (2004). Physical chemistry: understanding our chemical world. New York: Chichester: Wiley. p. 16. ISBN 0-471-49181-0.
↑ BIPM definition
↑ "Magnetic constant". 2006 CODATA recommended values. NIST. Archived from the original on 20 August 2007. Retrieved 8 August 2007.
↑ The integrand of this expression appears in the official documentation regarding definition of the ampere BIPM SI Units brochure, 8th Edition, p. 105
↑ Tai L. Chow (2006). Introduction to electromagnetic theory: a modern perspective. Boston: Jones and Bartlett. p. 153. ISBN 0-7637-3827-1.
↑ Ampère's Force Law Scroll to section "Integral Equation" for formula.
↑ O'Rahilly, Alfred (1965). Electromagnetic Theory. Dover. p. 104. (cf. Duhem, P. (1886). "Sur la loi d'Ampère". J. Phys. Theor. Appl. 5 (1): 26–29. doi:10.1051/jphystap:01886005002601. Retrieved 2015-01-07. , which appears in Duhem, Pierre Maurice Marie (1891). Leçons sur l'électricité et le magnétisme. 3. Paris: Gauthier-Villars. )
↑ Maxwell, James Clerk (1904). Treatise on Electricity and Magnetism. Oxford. p. 173.

External links

Ampère's force law Includes animated graphic of the force vectors.

This article is issued from Wikipedia - version of the 11/14/2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.