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## Revista Brasileira de Ensino de Física

##
*Print version* ISSN 1806-1117

### Rev. Bras. Ensino Fís. vol.34 no.1 São Paulo Jan./Mar. 2012

#### http://dx.doi.org/10.1590/S1806-11172012000100009

**ARTIGOS GERAIS**

**On equivalent expressions for the Faraday's law of induction**

**Formulações equivalentes da lei de Faraday**

**Fabio G. Rodrigues ^{1}**

Instituto de Matemática, Estatística e Ciência da Computaçao, Universidade Estadual de Campinas, Campinas, SP, Brasil

**ABSTRACT**

In this paper we give a rigorous proof of the equivalence of some different forms of Faraday's law of induction clarifying some misconceptions on the subject and emphasizing that many derivations of this law appearing in textbooks and papers are only valid under very special circunstances, thus are not satisfactory under a mathematical point of view. We show also that Faraday's law of induction is a relativistic invariant law in a very precise mathematical sense.

**Keywords:** Faraday's law, principle of equivalence, relativistic invariance.

**RESUMO**

Neste trabalho e dada uma prova de equivalência entre diferentes formas de se escrever a lei de induzo de Faraday, elucidando alguns equívocos sobre o tópico e enfatizando que muitas derivações desta lei apresentadas na maioria dos livros e artigos são validas somente sob circunstâncias muito particulares e, portanto, não satisfatórias sob o ponto de vista matemático. Tambem mostramos que a lei de indução de Faraday e relativisticamente invariante em um sentido matematicamente bem preciso.

**Palavras-chave:** lei de Faraday, princípio de equivalência, invariancia relativistica.

**1. Introduction**

Let a smooth closed curve in with parametrization **x**(*t,l*) which is here supposed to represent a filamentary closed circuit which is moving in an a convex and simply-connected (open) region where at time *t* as measured in an inertial frame,^{2} there are an electric and a magnetic fields , (t, **x**) **E**(t, **x**) є and** **, (t, **x**) **B**(t, **x**) є . We suppose that when in motion the closed circuit may be eventually *deforming.* Let be a smooth closed curve in with parametrization **x**(l) representing the filamentary circuit at *t* = 0. Then, the smooth curve is given by where σ_{t} (see details below) is the *flow* of a velocity vector field , which describes the motion (and deformation) of the closed circuit. It is an empirical fact known as Faraday's law of induction that on the closed loop acts an induced *electromotive force,* *ε*, such that

where *S _{t}* is a smooth surface on such that is its boundary and

**n**is the normal vector field on

*S*We write with . Now, on each element of the force acting on a unit charge which is moving with velocity

_{t}.**v**(t,

**x**(t, s)) is given by the Lorentz force law. Thus

^{3}the

*E*is by definition

where and Faraday's law reads [3-7]

Note that **(E** + **v** *x* **B)** is the Lorentz force acting on a unity charged carrier in the circuit according to the laboratory observers and it is sometimes called the *effective electric field* [3]. In the appendix we show how the first term of Eq. (3) is related with measurements done by observers at rest in an inertial reference frame commoving at a given instant *t* with velocity **v** relative to the laboratory frame.

We want to prove that Eq. (3) is equivalent to

from where it trivially follows the differential form of Faraday's law, *i.e*.,

**2. Some identities involving the integration of differentiable vector fields **

Let be a convex and simply-connected (open) region, , (t, x) **X**(t, **x**) be a generic differentiable vector field and let be a differentiable *velocity vector field of a fluid flow*. An *integral line*^{4} of v passing through a given x ∈ R3 is a smooth curve which at t = 0 is at x (i.e., σ_{x}(0) = **x** ) and such that its tangent vector at σ(t, **x**) is

Let moreover . We call σ_{t} Faraday's law, *i.e., at* the *fluid flow map.* Let *J* = (0,1) Є and let be a closed loop parametrized by and denote by the loop *transported* by the flow (see Fig. 1). Then

is clearly a parametrization of . We have the proposition:

**Proposition**

where

is the so-called material derivative^{5} and

is the tangent line element^{6} of at σ(t, x(l)).

**Proof.** We can write

Now, taking into account that for each x(l), we have

hence, the first term in the right side of Eq. (11) can be written as

Also writing we see that the last term in Eq. (11) can be written as

We now recall that for arbitrary differentiable vector fields it holds

Setting **a** = *d***l** and **b= v** and noting that it implies that

We need also to recall the well known identity

which implies setting **a= X, b** = *d***l** and **c** = (∇ *x* **v**), that

and also the *not* so well known identity^{7}

to write that

Finally, using Eq. (13) and Eq. (20) completes the proof of Eq. (8a) and Eq. (8b). Also, from Eq. (8b) it follows if we recall Eq. (15) that

from where the proof of Eq. (8c) follows immediately.

*a result that is known in fluid mechanics as Kelvin's circulation theorem (see, e.g., Refs. [8, 9]).*

Now,

where, if *S* is a smooth surface such that , then . Also n is the normal vector field to St.

Then using Eq. (8c) we can write

Also, denoting **Y:** = ∇x **X** we can write

Despite Eq. (24), for a general differentiable vector field such that we have

the so-called *Helmholtz identity* [10]. Note that the identity is also mentioned in [11]. A proof of Helmholtz identity can be obtained using arguments similar to the ones used in the proof of Eq. (8a). Some textbooks quoting Helmholtz identity are [12-16]. However, we emphasize that the proof of Faraday's law of induction presented in all the textbooks just quoted are always for very particular situations and definitively not satisfactory from a mathematical point of view.

We now want to use the above results to prove Eq. (3) and Eq. (4).

**3. Proofs of Eq. (3) and Eq. (4)**

We start remembering that in Maxwell theory we have that the **E** and **B** fields are derived from potentials, *i.e.* ,

where is the scalar potential and is the (magnetic) vector potential. If Eq. (26) is taken into account we can immediately derive Eq. (3). All we need is to use the results just derived in Section 2 taking **X= A.** Indeed, the first line of Eq. (23) then becomes

To obtain Eq. (4) we recall that from the second line of Eq. (23) we can write (using Stokes theorem)

Comparing the second member of Eq. (27) and Eq. (28) we get Eq. (4), *i.e.* ,

from where the differential form of Faraday's law follows.

**Remark 2** *We end this section by recalling that in the physical world the real circuits are not filamentary and worse, are not described by smooth closed curves. However, if the closed curve representing a 'filamentary circuit' is made of finite number of sections that are smooth, we can yet apply the above formulas with the integrals meaning Lebesgue integrals.*

**4. Conclusions**

Recently a paper [17] titled 'Faraday's law via the magnetic vector potential', has been commented in Ref. [18] and replied in Ref. [19]. Thus, the author of Ref. [17], claims to have presented an "alternative" derivation for Faraday's law for a filamentary circuit which is moving with an arbitrary velocity and which is changing its shape, using directly the vector potential **A** instead of the magnetic field **B** and the electric field **E** (which is the one presented in almost all textbooks).

Now, Ref. [18] correctly identified that the deriva tion in Ref. [17] is wrong, and that author agreed with that in Ref. [19]. Here we want to recall that a presen tation of Faraday's law in terms of the magnetic vector potential **A** already appeared in Maxwell treatise [20], using big formulas involving the components of the vec tor fields involved. We recall also that a formulation of Faraday's law in terms of **A** using modern vector calculus has been given by Gamo more than 30 years ago [21]. In Gamo's paper (not quoted in Refs. [17-19]) Eqs. (8c) appear for the special case in which **X= A** (the vector potential) and **B** = *V x* **A** (the magnetic field), *i.e.,*

Thus, Eq. (30) also appears in Ref. [17] (it is there Eq. (9)). However, in footnote 3 of [17] it is said that Eq. (30) is equivalent to where the term is missing. This is the error that has been observed by authors [18], which also presented a proof of Eq. (8b), which however is not very satisfactory from a mathematical point of view, that being one of the reasons why we decided to write this note presenting a correct derivation of Faraday's law in terms of **A** and its relation with Helmholtz formula. Another reason is that there are still people *(e.g.,* Ref. [22]) that do not understand that Eq. (3) and Eq. (4) are equiva lent and think that Eq. (3) implies the form of Maxwell equations as given by Hertz, something that we know since a long time that is wrong [23].

We also want to observe that Jackson's proof of Faraday's law using 'Galilean invariance' is valid only for a filamentary circuit moving without deformation with a constant velocity. The proof we presented is general and valid in Special Relativity, since it is based on trustful mathematical identities and in the Lorentz force law applied in the laboratory frame with the motion and deformation of the filamentary circuit mathematically well described.

**A Proof of the identity in Eq. (19)**

We know from Eq. (16) that

Let *{e ^{1}, e^{2}, e^{3}}* be an orthonormal base of . We can write, using

*Einstein convention,*

where with are Cartesian coordinates. It follows then

Using the known identity **a** *x* **b** *x* **c= (a** *•* **c)b- (a** *•* **b)c** in Eq. (33), we obtain

On the other hand, considering d**l** = *(dl1,dl2,dl3)* = *dl _{i}e^{i}*, we have

Hence, substituting Eq. (34) and Eq. (35) in Eq. (31), we can rewrite it as

From this last result, it is easy to see that

where

**B Phenomenological interpretation of the first member of Eq. (3)**

Let *S* be the inertial laboratory frame and *S'* the inertial frame that at time *t* has velocity **u= v** (t, σ(t, **x**(l))) (which is the velocity of an element of the circuit ) .

The electric and magnetic fields observed in *S'* are [3, 4]

where is the *Lorentz factor* and the symbols || and denotes the components parallel and orthogonal to **u.** Then, taking into account that and and by letting it follows that

where is the flux of **B**.

Using the right-side identity in Eq. (38), we can write

since is the element of proper time for an observer at rest in the commoving frame *S'* (with standard coordinates (x'º= t',x'^{i}). The integral is interpreted as the difference of potential measured by a voltmeter carried by an observer in *S'* (this is obviously clear when the field **v** is constant and the loop *Tt* is not deforming). So, we see that differs by terms of second order in **v ^{2}** from the differential potential measured by an observer in

*S'*.

Finally, we show an important result.^{8} Let a 2-form field, be the so called *electromagnetic field* [1,24,25], where (xº = *t,x ^{i})* are standard coordinates in a inertial reference frame in a Minkowski coordinates in a inertial reference frame in a Minkowski spacetime.

^{9}Then the antisymmetric matrix with entries F

*is*

_{µv}We now show that Φ is an invariant relativistic quantity.

Indeed, it can be written as

To show that, recall that if is the *electromagnetic potential* ( being the the *scalar potential* and **A** = (A1;A2,A2) the *vector potential*), then F = *d*A. Then by Stokes theorem we can write (taking into account that St is, for any t, a 2-dimensional open spacelike surface in Minkowski spacetime and that is the boundary of St)

This shows that Eq. (3) (and its equivalent Eq. (34)) is a relativistic invariant law.

**References**

[1] W.A. Rodrigues Jr. and E. Capelas de Oliveira, in: *Lecture Notes in Physics* 722 (Springer, Heidelberg, 2007). [ Links ]

[2] R.K. Sachs and H. Wu, *General Relativity for Mathematicians* (Springer-Verlag, New York, 1977). [ Links ]

[3] N. Rosen and D. Schieber, Am. J. Phys. **50,** 974 (1982). [ Links ]

[4] L.D. Landau and E.M. Lifshitz, *Electrodynamics of Continuous Media* (Pergamon, New York, 1960), p. 206. [ Links ]

[5] D.T. Paris and F.K. Hurd, *Basic Electromagnetic Theory* (McGraw-Hill, New York, 1969), p. 544. [ Links ]

[6] M. Schwartz, *Principles of Electrodynamics* (McGraw-Hill, New York, 1972), p. 187. [ Links ]

[7] A. Shadowitz, The Electromagnetic Field (Dover Publications, Inc., New York, 1988). [ Links ]

[8] A.J. Chorin and J.E. Mardsen, A Mathematical Introduction to Fluid Mechanics (Springer-Verlag, New York, 1993). [ Links ]

[9] P.G. Saffman, *Vortex Dynamics - Cambridge Monographs on Mechanics and Applied Mathematics* (Cambridge Univ. Press, Cambridge, 1992). [ Links ]

[10] H. Helmholtz, *Gesammelt Scriften* (Olms-Weidmann, Hildeshein, 2003), v. I (3), p. 597-603 (a reprint of *Wissenschaftliche Abhandlungen* v. 3 (Johann Ambrosius Barth, Leipzig, 1895). [ Links ]

[11] H.R. Hertz, *Electric Waves* (MacMillan, London, 1893), p. 243-247 (also, Dover, New York, 1962). [ Links ]

[12] M. Abraham and R. Becker, *The Classical Theory of Electricity and Magnetism* (Blackie, London, 1932). [ Links ]

[13] J.D. Jackson, *Classical Electrodynamics* (J. Wiley & Sons, Inc., New York, 1999). [ Links ]

[14] W.K.H. Panofski and M. Phillips, *Classical Electricity and Magnetism* (Addison-Wesley Publ. Co., Reading, 1962), p. 160-162. [ Links ]

[15] A. Sommerfeld, *Electrodynamics* (Academic Press, New York, 1952), p. 285-287. [ Links ]

[16] C.R. Paul, K.W. Whites and A.A. Nasar, *Introduction to Electromagnetic Fields* (McGraw-Hill, Boston, 1998), p. 653-658. [ Links ]

[17] D.V. Redzic, Eur. J. Phys. **28,** N7 (2007). [ Links ]

[18] A.K. Kholmetskii, O. Missevitch and T. Yarman, Eur. J. Phys. **29,** L1 (2008). [ Links ]

[19] D.V. Redzic, Eur. J. Phys. **29,** L5 (2008) [ Links ]

[20] J.C. Maxwell, *A Treatise of Electricity and Magnetism* (Dover, New York, 1954), p. 238-243. [ Links ]

[21] S.A. Gamo, Proc. IEEE **67,** 676 (1979). [ Links ]

[22] T.E. Phipps Jr., *Old Physics for New - A Worldview Alternative to Einstein s Relativity Theory* (Apeiron, Montreal, 2006). [ Links ]

[23] A.I. Miller, *Albert Einstein's Special Theory of Relativity* (Addison-Wesley Publ. Co., Inc., Reading, Ma., 1981), p. 16. [ Links ]

[24] Y. Choquet-Bruhat, C. DeWitt-Morette and M. Dillard-Bleick, *Analysis, Manifolds and Physics* (revised edition), (North-Holland Publ. Co., Amsterdam, 1982). [ Links ]

[25] B. Felsager, *Geometry, Particles and Fields* (SpringerVerlag, New York, 1998). [ Links ]

Recebido em 17/1/2011; Aceito em 20/11/2011; Publicado em 27/2/2012

1 E-mail: fabior@mpcnet.com.br or ra008618@ime.unicamp.br.

2 For a mathematical defintion of an inertial reference frame in Minkowski spacetime see, e.g., Refs. [1,2].

3 In this paper we use a system of units such that the numerical value of the speed of light is c =1.

4 Also called a stream line.

5 Mind that the material derivative is a derivative taken along a path σ* _{t}* with tangent vector . It is frequently used in fluid mechanics, where it describes the total time rate of change of a given quantity as viewed by a fluid particle moving on σ

_{x}. In the present case it appears because in the integral we need the values of

**X**for each t at all points of .

6 Take notice that dl is not an explicit function of the cartesian coordinates (x, y, z).

7 See the Appendix for a proof of this identity.

8 Which may be intelligible for readers with working knowledge of the mathematical methods of modern field theory [1, 2, 24].

9 Minkowski spacetime [2,24] is a manifold diffeomorphic to equipped with a metric field η and its Levi-Civita connection. In a standard coordinates of an inertial reference frame where the matrix with entries η

_{µv}is diag(1,-1,-1,-1).