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A NEW ELECTRODYNAMICS
BY
PARRY MOON 1 AND DOMINA EBERLE SPENC]~R 2
ABSTRACT
So successful have been Maxwell's equations that the electrodynamic formulations of Ampere, Weber, and Riemann have been almost forgotten. The purpose of this paper is to present a rejuvenation of the older theories, based entirely on the force between charged particles. The new formulation leads to the correct formulas for force, induced emf, and radiation. In fact, it may be regarded as an alternative to Maxwell's equations, with the advantages of Galilean relativity and a closer contact with reality (charges rather than fictitious flux lines).
I. INTRODUCTION
In the early part of the 19th century, Ampere (1), 3Gauss (2), Weber (3), and Riemann (4) developed a theory of electrodynamics, free from the magnetic-field fiction and based on an extension of the familiar equation of Coulomb. At that time, the electron was unknown and ideas of metallic conduction were of the haziest kind; yet a true particletheory was produced, both magnetic flux and the aether being ignored.
The attitude of these early investigators was surprisingly modern: their hard-headed phenomenological approach is much closer to the spirit of modern physics than is the mechanistic pictorialism of Faraday and Maxwell. It cannot be denied that the visualization of magnetic flux lines has been a genuine aid in electrical engineering. But there are advantages, both theoretical and practical, in the direct calculation of inter-particle forces in the pre-Maxwellian manner. It is interesting to see what can be done by a modernization of these older methods.

q

W

dr

P

FIG. I.

xDepartment of Electrical Engineering, Massachusetts Institute of Technology, Cambridge, Mass.
s Department of Mathematics, University of Connecticut, Storrs, Conn. s The boldface numbers in parentheses refer to the references appended to this paper.
369

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PARRY MOON AND DOMINA EBERLE SPENCER

[J. F. I.

Consider two charged particles (Fig. 1) separated by distance r. If there is no relative motion between the particles, Coulomb's equation applies. In the rationalized mks system,

Q1Q~

F, = a, 4~rer2.

(1)

This force is called the Coulombforce. If Q1 is moving a t constant velocity v with respect to Q,, the Ampere
force resulting from this motion is

= . ,_ 0 (2,

cos,

(2)

where 0 is the angle between v and the unit vector a,. We have shown (5) that Eq. 2 is the only equation t h a t is consistent with the Ampere experiments and with modern ideas of electronics.
The AmpSre force is a substitute for the magnetic field. Equation 2 handles all problems dealing with forces on conductors carrying direct current. Equations 1 and 2 cover the questions that are ordinarily treated under electrostatics and magnetostatics. To complete the theory, however, we must introduce additional terms dealing with the
acceleration of charge and with the time-variation of charge.
Consider all possible forces that can be exerted by charge Q1 on charge Q~ (Fig. 1). Evidently the possibilities may be classified as
(a) constant Q1, no relative motion. (b) constant Q1, uniform relative velocity. (c) constant Q~, accelerated motion. (d) Q1 a function of time.
Condition (a) gives the Coulomb force, (b) the Ampere force. The remainder of the paper will be concerned with (c) and (d).
2. THE WEBER FORCE
The next step consists in introducing a force caused by an accelerated
charge. This force may be called the Weberforce, since Wilhelm Weber
(3) was the first to include an acceleration term in the equations of electrodynamics. Reference to Fig. 1 shows that the force can depend
on only five variables: the charges Q1 and Q2, the distance r, the acceleration dv/dt, and the angle ~bbetween dv/dt and at.
The requirement of linearity means that the force must be directly
proportional to Q1Q2. The Weber force is directly proportional to acceleration because induced voltage is directly proportional to dI/dt or to Q dv/dt. Dimensional analysis then proves that the Weber force is
inversely proportional to the first power of r and inversely proportional

May, I954.]

A NEW ELECTRODYNAMICS

37I

to c2. W i t h o u t loss of generality, we can e m p l o y t h e constant of Eq. 1
and write for the Weber force,

F2 = Q1Q, dv F ~b

4~,c2---? ~" ( )'

(3)

where F(~b) is an u n k n o w n vector function of the angle ~b. Consider an element of conductor ds~ carrying a varying current
(Fig. 2). The current is taken in the direction of the vector ds~, and

I

,2,/ P

W

G r

FIG. 2.

I1 = N I A I [ Q , IVl, (4)
dI1/dt = N1A1 [Q, [ dv,/dt, where
N1 = n u m b e r of free electrons per unit volume of conductor (m-8),
A, = cross-sectional area of conductor (m2),
[Q, I -- magnitude of electronic charge (coulomb),
v, = drift velocity of electrons (m sec-1) with respect to the conductor.

The electrons in dsl constitute a charge

01 = - N1AII0.1 ~sl. From Eq. 3, the force per unit charge on Q, is

F , / Q , = N1AI [Q.. [ ds, dVl -- 4~r~c2r - ~ . F (~)

and from Eq. 4,

dSl dI1 - . F2/Q, = 4~-~c'r "~ "F (1/).

(5)

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Perhaps the simplest way of determining the unknown function F(~b) is to compare Eq. 5 with the corresponding expression based on Maxwell's equations. According to Maxwell's theory,

[ °'l
~/O = - v~ + u-oi '

where A is the vector potential and J is the current density.

element of Fig. 2,

J d v = 11 dsl,

SO

I~ ds, 0A

dsl dI~

A __ _ 4_1rr ' Ot

a. 4rcr dt '

For the

(!)/-

/

./

r y®

;

e

r,

FIG. 3.

where aa is a unit vector in the direction of the electron acceleration. Since the element dsl is uncharged, the scalar potential is zero and

1 OA

dsx dI,

F'/Q* = - , c ' Ot - a . ~ a t "

(6)

Comparison of Eqs. 5 and 6 shows that

F(~) = - a..

Thus the final equation for the Weber force for two charged particles

is, from Eq. 3,

O~ dv

F,/Q, = - a, 4r,c2~ dr'

(7)

where v is the relative velocity of charge 1 with respect to charge 2.

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A NEW E L E C T R O D Y N A M I C S

373

3. INDUCED E M F
The difference in potential between the ends of an element ds2 (Fig. 3), induced by the varying current in dsl, is

d V2 = - F~/Q2"ds2,

where the emf is taken positive for a potential rise in the direction of ds~. From Eq. 6, the induced emf in ds2 is

d 2V= --- d81"ds2 d I ,

(8)

4 7rec2r dt "

Introducing the mutual inductance M, we obtain

ds1 .ds2
d2 M ~ - -
4~-ec~r

or

1 ffdsl.ds2

M = 4~.~c~3 3

r "

(9)

This is the equation of F. Neumann (6). Equation 9 applies equally well to self inductance L when dsl and ds2 refer to elements in the same circuit. The result was obtained without reference to magnetic flux, and it is sometimes more convenient than the conventional method of flux linkages. Grover (7) says of Eq. 9:
This is the most general expression for finding the mutual inductance. It leads quite simply to a formal expression for the mutual inductance even though for most cases it is not possible to perform the integrations [analytically].... For inclined filaments . . . the Neumann formula has the advantage, and the formula for the mutual inductance of two straight filaments placed in any desired position has also been obtained by its use.
Thus the Weber force, caused by the acceleration of a charged particle, is given by Eq. 7. T h e emf induced in an element ds, is given by Eq. 8. The mutual inductance between closed circuits of any form is expressed by Eq. 9, and the induced emf is

_ dI1 V~= -- M dt "

(10)

As an illustration, consider the mutual inductance between two coaxial circles (Fig. 4). T a k e a charge Q2 a t a fixed point P on the outer circle; and determine the force on this charge, caused by a varying current in the inner circle.
According to Eq. 6,

dsl dI1

dF~/O, = -- 47r,c2r, d---t'

(6a)

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PARRY MOON AND DOiKINA EBERLE SPENCER

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w h e r e dsl = a df, r 's = a s + bs + z ~ - 2ab cos f. T h e t a n g e n t i a l c o m -

ponent of force at P, caused by current in the complete loop of radius

~, is
a d A f s ~ c o s ~'d~"

F~/Q2 = 47r~c2 dt . o

r

a d_f/1( "

c o s ~"d~"

- 2~-ec s dt .!o ['(a s + b2 + z2) - 2ab c o s ~"]~ "

Leti" = r - 2¢, cos~ = - cos2¢ = - (1 - 2 sin 2 ¢),d~ = - 2d9.

Then

_ a dllfo'12

(1 -2sin 2¢,)d

F,/Q2 r~c 2 dt

[(a + b) 2 +z s-4absin 2~

where

a

dAfo"/2 (1 - 2 sin s ~)d,p

= 7r~cS[-(a + b) 2 + zS] ½ d-t-

['1 - k s sin 2 ~o]~ '

k 2 = 4ab/[-(a + b) 2 T zQ.

(11)

Z

r,

x

-

F"

FIG. 4.

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A N ~ w ELECTRODYNAMICS

375

Integration leads to

a

dA

Ft/Q: = - ~r~c~k2[(a 4- b) ~ + z;-]~ dt [(2 - k O F - 2E-I,

(12)

where F and E are complete elliptic integrals of the first and second kinds. Equation 12 gives the force per unit charge on a particle at P, produced by a varying current in the loop of radius a.
The emf induced in a complete loop of radius b is

V = dY(Ft/Q2) ds2 = 2 r b ( F J Q ~ )

2ab

dI

= - ,c~k2[(a + b) 2 + z~-]t d--[ [(2 - k~)F - 2E-I,

(13)

so the mutual inductance of two concentric circles is

M = 2~1c--~- [(a + b) ~ -5 z2]~['(2 -- k g F -- 2 E l .

(14)

This is exactly the equation obtained by Maxwell. It could have been found, of course, directly from Eq. 9, though the above derivation gives a better physical picture of what is taking place.

4. THE LOOP ANTENNA
The induced emf in a circular loop is considered in Section 3. The equations apply to relatively low frequencies so that the time lag caused by the finite velocity of propagation may be neglected. We now take the case where retardation must be included but where the current is still essentially in phase around the loop.
The unretarded Weber force per unit charge is

ds, dI(t)

(6a)

dF /Q2 = 4~r~c~r dt

and the retarded Weber force is therefore

dsi dI(t - r/c)

(6b)

dF/Q~ = 47rec~r

dt

Let I(t) = 4-2I*e~' and F(t) = 42F*e ~', where I* and F* are rms values (generally complex numbers). Then

dI(t -- r/c)

~"

= io~4~I*e~,e--7.

dt

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PARRY MOON AND DOMINA EBERLE SPENCER

Thus Eq. 6b becomes

[J. F. I.

=
dF/Q2

47r~c2 r

ei,ote c

and the tangential force per unit charge (Fig. 4) is

i~ ds1I* cos f ~'

dF**/Q2 = -

47recUr, e ~

(6c)

Consider two current elements situated diametrically opposite each other on a circle of radius a (Fig. 4). Distances from these elements to point P are r' and r'. The tangential force, produced at P by current in the pair of elements, is

[ - ] dFt*/Q2 = _ i,oaI*cos~'df

ior'
e c

*~0r"
e c

(15)

4~C ~

r t

r rt

,

with

r '2 = a s + r ~ - 2 a r s i n O c o s ~ ' ,

If r >> a,

#,2 = a 2 + r~ + 2ar sin Ocos f.

r ' ~--- r ( 1 a -- - sin 0 cos ~.) ,
r

r'''~--r (1+ r-asin0cos~-),

1 1 ( 1 + a sin 0 cos ~.) '

rp~ r

r

--rttl-1--1-(-r ---asinOc°s"f)r

Substitution in Eq. 15 gives

[ ( ) dFt*/Q~

=

--

io~aI*e ~ c__osr d [ 27rec2r

i sin

o~a sin 0 cos ~" c

If o:a/c << 1,

sin ( ~ sin 0 cos ~) ~ ~°£° sin 0 cos ~',
co~(~0co~ 0 _-_~.

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A N E W ELECTRODYNAMICS

377

Thus,

dF,*/Q2 ~-- ioa'[I*l[27rec,[r i~c + 1 ]sin 0 c o s ' : d~',

(16)

where

ior
[-I*] = I*e

The tangential force per unit charge at P, caused by current in the complete loop of radius a, is

F,*/Q, = - iwa'~I*-] sin O[~ + l ] fo't' cos2 ~ d

or

~°(Ira~)[I*]sinO[c_~] F*/Q, = a~ 47recUr

(17)

where a~ is a unit vector in the tangential direction. This equation agrees with the usual formula derived from Maxwell's equations. It shows that the force at P is directly proportional to the area of the loop and directly proportional to the sine of the angle from the loop axis. The first term of Eq. 17, which varies inversely as the first power of the distance, represents the ordinary radio wave. The second term varies inversely as the second power of r and thus becomes negligible at very large distances.
5. THE MAXWELL FORCE
The preceding sections have evaluated cases (a), (b), and (c) of Section 1. There remains the rather unusual case (d) of a charge that is not constant. For example, with a linear conductor in the stationary or quasi-stationary state, the conduction current entering an elementary length of conductor is equal to the current leaving it, in accordance with Kirchhoff's second law. But at sufficiently high frequency, this relation no longer holds: the charge on the element depends on both time and position. Because (d) is closely related to Maxwell's displacement
current, the corresponding force will be called the Maxwell force.
Suppose t h a t Q1 of Fig. 1 varies sinusoidally with t i m e :
Q~(t) = 4-2Q*e,,,.

The corresponding retarded quantity is

Ql(t - r/c) = 42Q*e,~(,-,m.

According to Maxwell's theory, this varying charge produces a force on Q2:

F*/Q, = a,--

+ Tr '

(18)

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PARRY MOON AND DOMINA EBERLE SPENCER

[3. F. I.

where

[Q*~ = ~[2Q*e - ' ~ ' ' , Y = ~ F * e '°'t.

This same result is obtained from the new theory if we assume for

the Maxwell force,

1o[1 ]

F / Q 2 = - a ~ -4-rr e O-r r Qx(t - r / c ) .

(19)

T h e n for the charged particles of Fig. 1, Eq. 19 gives

F/Q2 = -

47tel r2 cr j

or

F*/Q, = a, ~

-~ + ~ .

(18)

For the special case of Ql(t) = Q1 = const, Eq. 19 reduces to the Cou-

lomb force,
Q,

F/Q2 = ar 47rer2.

(1)

Thus the Maxwell force includes the Coulomb force as a special case, and no separate term for the Coulomb force is needed.
Just as the Ampere force replaces the magnetic field, so the Maxwell force replaces the displacement current, t h o u g h of course Eq. 19 was not formulated by Maxwell. In fact, none of the previous theories seems to include such a force, which may account for the rather unsatisfactory nature of the theories of Weber, Riemann, Ritz (8), and Warburton (9).
As an example, take an electric dipole (Fig. 5) with the charges varying sinusoidally with time:

Q = ~]2Q*e,,,.

For the upper charge, according to Eq. 19,

But if l << r,

4~Q*[ 1 i~ ] e'o~'-~"o'.
F / G = at, -Tg-i-~, L -~ +

r' -----r(1 -- ( l / 2 r ) cos 0), r " ~ r(1 + ( 1 / 2 r ) c o s 0),

1 ~ 1 (1 + ( l / 2 r ) cos 0), r1" ~ 1 (1 ( l / 2 r ) cos 0).

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A NEw ELECTRODYNAMICS

.....

379

Then

/car /colcos 0

F*/Q2 I*e ;e w
= io~47r~

If (1 +/cosO)+i°~(1

-r 2

r

cr \

+

l 2r

cos

)} 0

X [ a r + a0 l sin 0 ]]

where I is the current between the two spheres :

421*el-t I = 4-2I*ei% Q = ioo "

,Z

,0(
lI o,
"Q i

Fro. 5.
Similarly, for the lower charge,

I /*e ' e 2c

F*/Q2 =

U~

[1[
1--

cosO +--

1 --

cosO

X --a,+ao~

.

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PARRY MOON AND DOMINA EBERLE SPENCER

[J. F. I.

The sum of the two forces has a radial component,

ioar

Fr /Q2

=

I--i*o-e-.47r~c-

11[ ~

2isin

(c01 ) ~cC°SO

+

-2r - l

cos

0

cos

(o0l 2c

cos

0) ]

+ i~r[2isin (~c/cos O) + !cosOcos ( ~ c/ cos 0 ) ] } .

But
sin(O~/cosO)_=w2cl C°SO' cos (o~~closO ) ,~=1,

SO

Fr*/Q2 = [ I * ] l c o s O [ r2 i2Co~r+ i_~]cr "

(20)

Similarly, the component of force perpendicular to the radius is

F°*/Q2 = [f*]l sin O[ r~ o8oirt]"

(21)

6. THEDIPOLE ANTENNA
Consider the dipole antenna (Fig. 5), assuming that the current in the vertical wire between + Q and - Q is not a function of z. The dipole itself produces the force given by Eqs. 20 and 21. To this must be added the Weber force, Eq. 6, caused by the varying current in the wire. For I(t -- r/c) = ~f2I*e i~t-rl°), the retarded Weber force is

~f2ioolI* F/Q2 = -- a, _4rr_~c2r elf(t--r/c)

or

+ ae (F*/Q,)~

¢,oEI*]Z cos 0 = - a, 4 7r~c2r

i,oEI*-]zsin 0
4 7r~c2r

(22)

Equations 20 and 21 express the Maxwell force

[/*]l cos 0[ 2 (F*/Q2)u = a~ 4~,c r2

i2c+ io~] ~wr ~r
[I*]lsinO[1 + a, 47r~c r'

ic ] (23) wr* "

The Ampere force is a double-frequency force because of the second power of the velocity, Eq. 2. Thus the total force at fundamental frequency is the sum of the Weber and the Maxwell forces, or

May, I954.]

A NEW ELECTRODYNAMICS

381

[I*]l cos O[1

P*/Q2 = a, 2,~c

r'

ic ]

,or8
[I*]l sin O[1

+ ao 4~-~c

r 2

ic + i~o] (24)
o~r 3 c r "

At very great distances, Eq. 24 reduces to

io~[I*]l sin 0

(24a)

F*/Q2 = ae 47r~cr~ ,

showing that the force per unit charge at the receiver varies directly as the length of the anteflna, directly as the frequency, and inversely as the distance. Equations 24 and 24a agree with the classical results obtained from Maxwell's equations.
7. SUMMARY
The paper has developed an electrodynamics that is in agreement with Galilean relativity and free from the aether and the magneticfield concept. The fundamental equation expresses the force on a charged particle, caused by another charged particle (Fig. 1). The particles may be stationary with respect to each other, or they may be in relative motion. The charges may be constant or they may vary with time. In any case, the force per unit charge at point 2 is

F/Q2 = a, ~ ( ~ ) ~ [1 - ] cos20] - aa ~4~rQ~c12 ddt v ( t - r/c)

1 a

The first term represents the Ampere force, which is particularly important with direct currents. The second term represents the Weber force, which gives induced emf's. The third term represents the Maxwell force. It includes the Coulombforce as a special case where Q -
const., but it is especially useful where the frequency is high enough so that O is a function of both time and position.
Note that Eq. 25 is inherently relativistic, without the need of Lorentz contraction or Einstein pseudo-relativity. The only velocity
is t h e relative velocity v of charge 1 with respect to charge 2 ; t h e only
acceleration is the rate of change of relative velocity. Equation 25 may be used as the basis for all of electrodynamics. Thus questions dealing with aggregates of charge are handled by summation (or inte-
gration) of F/Q2, and problems dealing with currents are treated by
considering large numbers of electrons in motion. The only limitation of Eq. 25 seems to be that it applies only to ordinary velocities. It is probable that the functions of Eq. 25 will require slight modification if they are applied to electrons at extreme velocities.

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PARRY MOON AND DOMINA EBERLE SPENCER

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The new formulation of electrodynamics is built on the foundations laid by Weber and by Ritz. It differs from all previous theories, however, particularly in the term for the Maxwell force. This formulation may be regarded as an alternative to Maxwell's equations. Maxwell based his work on the closed circuit, on the aether, and on the Faraday visualization of flux lines. The Maxwell equations give the correct answers to a great number of questions; but the application of these equations to open circuits is sometimes ambiguous and uncertain. Particularly in considering the magnetic field produced by electrons in motion, one may find the classical field concepts to be clumsy tools. The new formulation generally leads to exactly the same results as Maxwell's equations, but in some cases it may give a more direct approach and one that is free from ambiguity.

REFERENCES
(1) A-M. AMP~'RE,"Mdmoire sur la thdori~ math~matique des phdnomenes dlectrodynamiques, uniquement ddduite de l'expdrience," M~m. de rAead. Sci., Vol. 6, p. 175 (1823) ; "Collection de M6moires relatifs a la physique," Paris, Gauthier-Villars, 1887, Vol. 3, p. 1.
(2) C. F. GAUSS, "Zur mathematischen Theorie der elektrodynamischen Wirkung," Werke, G6ttingen, I867, Vol. V, p. 602.
(3) WILHELMWEBER, "Elektrodynamische Maassbestimmungen fiber ein allgemeines Grundgesetz der elektrischen Wirkung," Wilhelm Weber's Werke, Berlin, Julius Springer, 1893, Vol. 3, p. 25.
(4) B. RIEMANN, "Schwere, Elektrizit~it, und Magnetismus," Hannover, C. Rtimpler, 1876, p. 327.
(5) P. Moon AND D. E. SPENCER, "The Coulomb Force and the Ampere Force," JOUR. FRANKLININST.,Vol. 257, p. 305 (1954). Note that the sign of the Amp&re force has been changed to positive in the present paper because the relative velocity of Q1 is now used.
(6) FRANZNEUMANN, "Die mathematischen Gesetze der inducirten elektrischen Str6me," Berlin Akad. d. Wissen., Abh. 1845; "Ober ein allgemeines Princip der mathematischen Theorie inducirter elektrischer Str6me," Berlin Akad. d. Wissen., Abh. 1848; Ostwald's Klassiker d. exakten Wissenschaften, W. Englemann, Leipzig, 1892, No. 36.
(7) F. W. GROVER,"Inductance Calculations," New York, D. Van Nostrand Co., 1946, p. 8. (8) W. RITZ, "Recherches critique sur l'dlectrodynamique gdn~rale," Ann. de Chimie et de
Phys., Vol. 13, p. 145 (1908);Gesammelte Werke, Paris, Gauthier-Villars, 1911, p. 317. (9) F. W. WARBURTON,"Reciprocal Electric Force," Phys. Rev., Vol. 69, p. 40 (1946).