the electric force of a current - portal...
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The Electric Force of a Current
A. K. T. Assis
University of Campinas – Brazil
www.ifi.unicamp.br/~assis
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Assis and Hernandes,
The Electric Force of a Current
(Apeiron, Montreal, 2007)
www.ifi.unicamp.br/~assis2
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?F
• Is there a force between a stationary charge
and a stationary circuit carrying a steady
current?
• Is the wire neutral at all points?
• Where are the charges which generate the
electric field inside the resistive wire? 3
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Maxwell (Treatise of Electricity and
Magnetism, 1873, article 848):
“Such an action has never been observed.”
Clausius (1877): “We accept as criterion the
experimental result that a constant current in
a stationary conductor exerts no force on
stationary charge.”
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Feynman Lectures on Physics, Vol. 2, Section
13-6 (1964): “In a normal conductor, like
copper, the electric currents come from the
motion of some of the negative electrons. (...)
There is thus no electric field outside the wire.”
Jackson, Classical Electrodynamics, 1975,
Exc. 14.13: “For a real circuit the stationary
positive ions in the conductor will produce an
electric field which just cancels that due to
the moving charges.”5
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Continuity of the tangential component of E
There must be an electric field outside resistive
wires carrying steady currents. Reasons:
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Bending a wire:
JE
Ohm’s law
Where are the electric charges which generate the
electric field inside a wire carrying a constant current?
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Weber and Kirchhoff in 1850-7:
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Consequences:
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Solution of the problem:
|'|
''
4
1
|'|
'
4
1)(
00 rr
dar
rr
qr
02 and the boundary
conditions over the
surface of the wire.
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Straight wire with steady current:
a
z0
ˆˆln
ln
)(
ˆ)(
0
0
zk
a
EaE
kEaE
11
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Bergmann and Schaefer
(Elektrizität und
Magnetismus, 1950).
V = 30 kV.
Jefimenko, AJP 30,
19 (1962).
V = 10 kV.
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Jefimenko et al., Proc. West Virginia Acad.
Sci. 34, 163 (1962).
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Transmission line:
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Coaxial cable: Analogous situation to that
of a straight wire.
E outside ≠ 0. There should be interference
between two coaxial cables.16
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Infinite solenoid, Heald,
AJP 52, 522 (1984): 2tan0
E outside ≠ 0 17
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Resistive ring with steady current
J. A. Hernandes and A. K. T. Assis,
Phys. Rev. E 68, 046611 (2003). 18
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Toroidal coordinates , , :
x
y
azyx
za
azyx
yxatan ,
2tan ,
2tan
22222222
22
)()()( coscosh ,02 XH
1 0
2/1
0
2/1
)(cosh)cos()sin(
)(cosh)cos(coscosh
q p
q
ppq
p
pp
PpBq
PpA
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Weber in 1852: “The electric charge of the
circuit increases from the neutral point to the
contact point not uniformly, but accelerates
gradually.”
Density of surface charges in the resistive
ring with steady current:
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Sansbury, Rev. Scientific Instruments 56, 415 (1985)
Cq 1010
NFkAICq 710 10 , ,1022
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AIMRRkVV 13 ,75 ,2 21
Moreau et al., AJP 53, 552 (1985).
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Chabay and Sherwood, Electric and Magnetic
Interactions (2002).
24
Video showing this experiment:
www.matterandinteractions.org/Content/Materials/Videos/SurfaceCharge.mov
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Assis and Hernandes,
The Electric Force of a Current
(Apeiron, Montreal, 2007)
www.ifi.unicamp.br/~assis25
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Conclusion:
www.ifi.unicamp.br/~assis
But Weber got there first!
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Additional material
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Weber, 1852:
BxA
iExE ˆln)( 0
BxAL
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Resistive strip
Elliptic-cylindrical coordinates
22
21
ya
zkk
V = 10 kV.
Jefimenko, AJP
30, 19 (1962).
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Lumped resistor, Heald, AJP 52, 522 (1984):
30