|
Gaussian CGS |
SI |
Units and |
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|
Charge |
2.997 92 ´ 109 esu |
= 1 C = 1 A s |
Potential |
(1/299.792) statvolt |
= 1 V = 1 J C–1 |
Magnetic field |
104 gauss = 104 dyne/esu |
= 1 T = 1 N A–1 m–1 |
Electron charge |
e = 4.803 204 ´ 10–10 esu |
= 1.602 176 ´ 10–19 C |
Lorentz force |
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Maxwell equations |
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Linear media |
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Permittivity of free space |
|
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Permeability of free space |
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Fields from potentials |
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Static
potentials |
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Relativistic |
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Impedances (SI units)
r = resistivity at room temperature in 10–8 W m:
~ 1.7 for Cu ~ 5.5 for W
~ 2.4 for Au ~ 73 for SS 304
~ 2.8 for Al ~ 100 for Nichrome
(Al alloys may have
double this value.)
For alternating currents, instantaneous current I, voltage V, angular frequency w:
.
Impedance of self-inductance L: Z = jwL .
Impedance of capacitance C: Z = 1/jwC .
Impedance of free space: .
High-frequency surface impedance of a good conductor:
, where d = effective skin depth ;
for Cu .
Capacitance and inductance per unit length (SI units)
Flat rectangular plates of width w, separated by d << w with linear medium (e, m) between:
;
= 2 to 6 for plastics; 4 to 8 for porcelain, glasses;
Coaxial cable of inner radius r1, outer radius r2:
.
Transmission lines (no loss):
Impedance: .
Velocity: .
Motion of charged particles in a uniform, static magnetic field
The path of motion of a charged particle of momentum p is a helix of constant radius R and constant pitch angle l, with the axis of the helix along B:
,
where the charge q is in units of the electronic charge. The angular velocity about the axis of the helix is
,
where E is the energy of the particle.
This section was adapted, with permission, from the 1999 web edition of the Review of Particle Physics (http://pdg. lbl.gov). See J. D. Jackson, Classical Electrodynamics, 2d ed. (John Wiley & Sons, New York, 1975) for more formulas and details. A PDF version of this table is also available.