where Q is charge on each plate, is potential difference.
📚 Practice Problems
1Problem 1medium
❓ Question:
A parallel-plate capacitor has circular plates of radius R = 5.0 cm separated by distance d = 2.0 mm. (a) Find the capacitance in vacuum. (b) If a dielectric material with κ = 3.5 is inserted, what is the new capacitance? (c) If the capacitor is charged to 12 V with the dielectric in place, how much charge is stored?
Capacitance calculations, energy storage, and dielectric materials
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Start by reading the study notes and working through the examples on this page. Then use the flashcards to test your recall. Practice with the 3 problems provided, checking solutions as you go. Regular review and active practice are key to retention.
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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).
A=πR2=π(0.05)2=7.85×10−3 m2
The capacitance is:
C0=dϵ0A=0.002(8.85×10−12)(7.85×10−3)
C0=3.47×10−11 F=34.7 pF
(b) Capacitance with dielectric:
With a dielectric, the capacitance increases by factor κ:
C=κC0=(3.5)(34.7 pF)
C=121 pF
(c) Charge stored:
Using Q = CV:
Q=CV=(121×10−12)(12)
Q=1.45×10−9 C=1.45 nC
2Problem 2hard
❓ Question:
Three capacitors (C₁ = 4.0 μF, C₂ = 6.0 μF, C₃ = 3.0 μF) are connected with C₁ and C₂ in series, and this combination is in parallel with C₃. The entire network is connected to a 24 V battery. Find: (a) the equivalent capacitance, (b) the charge on each capacitor, and (c) the voltage across each capacitor.
💡 Show Solution
Given:
C₁ = 4.0 μF, C₂ = 6.0 μF, C₃ = 3.0 μF
V = 24 V
(a) Equivalent capacitance:
C₁ and C₂ in series:
C121=C1
C12=2.4 μF
C₁₂ in parallel with C₃:
Ceq=C12+C
Ceq=5.4 μF
(b) Charges:
Total charge from battery:
Qtotal=CeqV
For parallel combination:
Q₃ = C₃V = (3.0)(24) = 72 μC
Q₁₂ = C₁₂V = (2.4)(24) = 57.6 μC
In series, C₁ and C₂ have same charge:
Q₁ = Q₂ = Q₁₂ = 57.6 μC
(c) Voltages:
V1=C1
V2=C2
V3=24 V
Note: V₁ + V₂ = 14.4 + 9.6 = 24 V ✓
3Problem 3medium
❓ Question:
A parallel-plate capacitor with capacitance C₀ = 50 pF is charged to voltage V₀ = 100 V and then disconnected from the battery. A dielectric slab with κ = 2.5 is then inserted between the plates. Find: (a) the charge on the capacitor (before and after), (b) the new voltage, and (c) the change in stored energy.
💡 Show Solution
Given:
C₀ = 50 pF
V₀ = 100 V
κ = 2.5
Capacitor is isolated (Q constant)
(a) Charge:
Initial charge:
Q=C0V0=(50×10−12)(100)=
Since capacitor is isolated, charge remains constant:
Qbefore=Qafter
(b) New voltage:
With dielectric:
C=κC0=(2.5)(50)=125 pF
Voltage decreases:
V=CQ=125
V=40 V
(c) Change in energy:
Initial energy:
U0=2
Final energy:
U=21CV
Change in energy:
ΔU=U−U0=1.0×10
ΔU=−1.5×10−7 J
Energy decreases (absorbed by dielectric being pulled in).
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Yes, this page includes 3 practice problems with detailed solutions. Each problem includes a step-by-step explanation to help you understand the approach.