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146 Electromagnetism<br />
Electromagnetic energy<br />
Electromagnetic field<br />
energy density (in free u = 1<br />
space)<br />
2 ɛ 0E 2 + 1 B 2<br />
(7.128)<br />
2 µ 0<br />
Energy density in<br />
media<br />
Energy flow (Poynting)<br />
vector<br />
u<br />
E<br />
B<br />
energy density<br />
electric field<br />
magnetic flux density<br />
ɛ 0 permittivity <strong>of</strong> free space<br />
u = 1 2 (D ·E +B ·H) (7.129) µ 0 permeability <strong>of</strong> free space<br />
D electric displacement<br />
H magnetic field strength<br />
N = E×H (7.130)<br />
c<br />
N<br />
speed <strong>of</strong> light<br />
energy flow rate per unit<br />
area ⊥ to the flow direction<br />
Mean flux density at a<br />
distance r from a short 〈N〉 = ω4 p 2 0 sin2 r vector from dipole<br />
θ<br />
oscillating dipole<br />
32π 2 ɛ 0 c 3 r 3 r (7.131) (≫wavelength)<br />
θ angle between p and r<br />
p 0 amplitude <strong>of</strong> dipole moment<br />
ω oscillation frequency<br />
Total mean power<br />
from oscillating W = ω4 p 2 0 /2<br />
dipole a 6πɛ 0 c 3 (7.132) W total mean radiated power<br />
Self-energy <strong>of</strong> a<br />
charge distribution<br />
U tot = 1 2<br />
Energy <strong>of</strong> an assembly<br />
<strong>of</strong> capacitors b U tot = 1 2<br />
Energy <strong>of</strong> an assembly<br />
<strong>of</strong> inductors c U tot = 1 2<br />
Intrinsic dipole in an<br />
electric field<br />
Intrinsic dipole in a<br />
magnetic field<br />
∫<br />
volume<br />
φ(r)ρ(r)dτ (7.133)<br />
∑∑<br />
C ij V i V j (7.134)<br />
i<br />
j<br />
∑∑<br />
i<br />
j<br />
U tot<br />
dτ<br />
r<br />
φ<br />
ρ<br />
V i<br />
C ij<br />
total energy<br />
volume element<br />
position vector <strong>of</strong> dτ<br />
electrical potential<br />
charge density<br />
potential <strong>of</strong> ith capacitor<br />
mutual capacitance between<br />
capacitors i and j<br />
L ij I i I j (7.135) L ij mutual inductance between<br />
inductors i and j<br />
U dip = −p ·E (7.136)<br />
U dip energy <strong>of</strong> dipole<br />
p electric dipole moment<br />
U dip = −m·B (7.137) m magnetic dipole moment<br />
Hamiltonian <strong>of</strong> a<br />
charged particle in an H = |p m −qA| 2<br />
+qφ (7.138)<br />
EM field d 2m<br />
a Sometimes called “Larmor’s formula.”<br />
b C ii is the self-capacitance <strong>of</strong> the ith body. Note that C ij = C ji .<br />
c L ii is the self-inductance <strong>of</strong> the ith body. Note that L ij = L ji .<br />
d Newtonian limit, i.e., velocity ≪ c.<br />
H<br />
p m<br />
q<br />
m<br />
A<br />
Hamiltonian<br />
particle momentum<br />
particle charge<br />
particle mass<br />
magnetic vector potential