A spherical capacitor is constructed from two concentric spherical conductors with radii R1R_1R1​ and R2R_2R2​, where R2>R1R_2 > R_1R2​>R1​. The region between the conductors is filled with a dielectric material whose permittivity varies with the radial distance rrr according to the relation:

Answer

Capacitance of Spherical Capacitor with Variable Dielectric | Physics Derivation

🔋 Capacitance of Spherical Capacitor with Radially Varying Dielectric

🧮 Part (a): Derivation

The permittivity varies with radial distance \( r \) as:

ε(r) = ε₀ (1 + k / (r – R₁))

The electric field from Gauss’s law is:

E(r) = Q / [4πr²ε(r)] = Q(r – R₁) / [4π ε₀ r² (r – R₁ + k)]

🔻 Potential Difference:

Using integration from R₁ to R₂:

V = ∫R₁R₂ E(r) dr = (Q / 4πε₀) ∫0R₂−R₁ [x / (x + R₁)²(x + k)] dx

After change of variables \( x = r – R₁ \), the expression for Capacitance becomes:

C = 4πε₀ / ∫0R₂−R₁ [x / (x + R₁)²(x + k)] dx

🧪 Part (b): Numerical Evaluation

ParameterValue
R₁1.00 cm = 0.01 m
R₂3.00 cm = 0.03 m
k0.50 cm = 0.005 m
ε₀8.854 × 10⁻¹² F/m

Approximating the integral numerically:

∫ ≈ 44.24

Then the capacitance is:

C ≈ (4π × 8.854 × 10⁻¹²) / 44.24 ≈ 2.52 × 10⁻¹² F = 2.52 pF

✅ Final Answer

Capacitance Expression:

C = 4πε₀ / ∫0R₂−R₁ [x / (x + R₁)²(x + k)] dx

Numerical Result:

C ≈ 2.52 picofarads (pF)

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