仮紙面

g=φ=BA
∂g/∂t=∂φ/∂t=∂BA/∂t
V=∂g/∂t=∂φ/∂t=∂BA/∂t
V=∂BA/∂t
V=EL
EL=∂BA/∂t
∫EdL=∫∂BdA/∂t
∫rotEdA=∫∂BdA/∂t
rotE∫dA=∂B∫dA/∂t
rotEA=∂BA/∂t
rotE=∂B/∂t

g=φ=BA
∂g/∂t=∂φ/∂t=∂BA/∂t
V=-∂g/∂t=-∂φ/∂t=-∂BA/∂t
V=-∂BA/∂t
V=EL
EL=-∂BA/∂t
∫EdL=-∫∂BdA/∂t
∫rotEdA=-∫∂BdA/∂t
rotE∫dA=-∂B∫dA/∂t
rotEA=-∂BA/∂t
rotE=-∂B/∂t

e=ψ=DA
∂e/∂t=∂ψ/∂t=∂DA/∂t
V=∂e/∂t=∂ψ/∂t=∂DA/∂t
V=∂DA/∂t
V=HL
HL=∂DA/∂t
∫HdL=∫∂DdA/∂t
∫rotHdA=∫∂DdA/∂t
rotH∫dA=∂D∫dA/∂t
rotHA=∂DA/∂t
rotH=∂D/∂t

e=ψ=DA
∂e/∂t=∂ψ/∂t=∂DA/∂t
V=-∂e/∂t=-∂ψ/∂t=-∂DA/∂t
V=-∂DA/∂t
V=HL
HL=-∂DA/∂t
∫HdL=-∫∂DdA/∂t
∫rotHdA=-∫∂DdA/∂t
rotH∫dA=-∂D∫dA/∂t
rotHA=-∂DA/∂t
rotH=-∂D/∂t

Fe=eE
Fe=ee/4πε0r^2
Fe=eE=ee/4πε0r^2
eE=ee/4πε0r^2
E=e/4πε0r^2
E=e/ε04πr^2
E=e/ε0A
ε0EA=e
D=ε0E
DA=e
e=DA
e=ψ=DA
eV/V=ψV/V=DA
(e/V)V=(ψ/V)V=DA
ρV=(e/V)V=(ψ/V)V=DA
ρV=DA
ρ=DA/V
ρ=Ddxyz/dxyz
ρ=Dd/dx
ρ=▽•D
ρ=divD
▽•D=ρ
divD=ρ

Fe=eE
Fe=ee/4πε0r^2
Fe=eE=ee/4πε0r^2
eE=ee/4πε0r^2
E=e/4πε0r^2
E=e/ε04πr^2
E=e/ε0A
ε0EA=e
D=ε0E
DA=e
e=DA
e=ψ=DA
DA=e=ψ
DA=eV/V=ψV/V
DA=e/V*V=ψ/V*V
DA=ρ*V=e/V*V=ψ/V*V
∫DdA=∫ρ*dV=∫e/V*dV=∫ψ/V*dV
∫divDdV=∫ρ*dV=∫e/V*dV=∫ψ/V*dV
divD∫dV=ρ*∫dV=e/V*∫dV=ψ/V*∫dV
divDV=ρ*V=e/V*V=ψ/V*V
divD=ρ=e/V=ψ/V
divD=ρ

Fg=gH
Fg=gg/4πμ0r^2
Fg=gH=gg/4πμ0r^2
gH=gg/4πμ0r^2
H=g/4πμ0r^2
H=g/μ04πr^2
H=g/μ0A
μ0HA=g
B=μ0H
BA=g
g=BA
g=φ=BA
gV/V=φV/V=BA
(g/V)V=(φ/V)V=BA
ρV=(g/V)V=(φ/V)V=BA
ρV=BA
ρ=BA/V
ρ=Bdxyz/dxyz
ρ=Bd/dx
ρ=▽•B
ρ=divB
▽•B=ρ
divB=ρ

Fg=gH
Fg=gg/4πμ0r^2
Fg=gH=gg/4πμ0r^2
gH=gg/4πμ0r^2
H=g/4πμ0r^2
H=g/μ04πr^2
H=g/μ0A
μ0HA=g
B=μ0H
BA=g
g=BA
g=φ=BA
BA=g=φ
BA=gV/V=φV/V
BA=g/V*V=φ/V*V
BA=ρ*V=g/V*V=φ/V*V
∫BdA=∫ρ*dV=∫g/V*dV=∫φ/V*dV
∫divBdV=∫ρ*dV=∫g/V*dV=∫φ/V*dV
divB∫dV=ρ*∫dV=g/V*∫dV=φ/V*∫dV
divBV=ρ*V=g/V*V=φ/V*V
divB=ρ=g/V=φ/V
divB=ρ