Capacitance calculations, energy storage, and dielectric materials
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V
Units: 1 farad (F) = 1 coulomb/volt
Parallel Plate Capacitor
Area A, separation d:
E=ϵ0σ=ϵ0AQ
V=Ed=ϵ0AQd
C=VQ=dϵ0A
Other Geometries
Cylindrical Capacitor
Inner radius a, outer radius b, length L:
C=ln(b/a)2πϵ0L
Spherical Capacitor
Inner radius a, outer radius b:
C=4πϵ0b−aab
Isolated Sphere
Radius R (other conductor at infinity):
C=4πϵ0R
Capacitors in Series
Same charge Q on each:
Ceq1=C11+C21+⋯
Two capacitors:Ceq=C1+C2C1C2
Capacitors in Parallel
Same voltage V across each:
Ceq=C1+C2+⋯
Energy Stored in Capacitor
Work to charge capacitor:
W=∫0QVdq=∫0QCqdq=2CQ2
Energy:U=21CQ2=21CV2=21QV
Energy density (parallel plate):
u=AdU=21ϵ0E2
Dielectrics
Insulating material inserted between plates:
Dielectric constant:κ (or K)
With dielectric:
Capacitance: C=κC0
Electric field: E=E0/κ
Potential: V=V0/κ (if charge constant)
Permittivity of material:ϵ=κϵ0
Modified equations:C=dκϵ0A
u=21κϵ0E2
Dielectric Breakdown
Maximum field before dielectric breaks down:
Air: ~3×106 V/m
Different materials have different breakdown strengths.
Gauss's Law with Dielectrics
∮E⋅dA=κϵ0Qfree
or using electric displacementD=κϵ0E:
∮D⋅dA=Qfree
Polarization
Dielectric polarizes in electric field:
Polarization:P=κϵ0(κ−1)E
Bound surface charge:σb=P
This reduces net field inside dielectric.
Energy with Dielectric
If dielectric inserted with:
Constant charge:Uf=Ui/κ (energy decreases)
Constant voltage:Uf=κUi (energy increases)
Force on dielectric:
Dielectric pulled into capacitor (lower energy state).