A coaxial conductor has radii \(a=0.8 \mathrm{~mm}\) and \(b=3 \mathrm{~mm}\) and a polystyrene dielectric for which \(\epsilon_{r}=2.56 .\) If \(\mathbf{P}=(2 / \rho) \mathbf{a}_{\rho} \mathrm{nC} / \mathrm{m}^{2}\) in the dielectric, find (a) \(\mathbf{D}\) and \(\mathbf{E}\) as functions of \(\rho ;(b) V_{a b}\) and \(\chi_{e} \cdot(c)\) If there are \(4 \times 10^{19}\) molecules per cubic meter in the dielectric, find \(\mathbf{p}(\rho)\)

Short Answer

Expert verified
Question: Calculate the electric field (E), electric displacement field (D), potential difference (V_ab), electric susceptibility (χe), and the polarization (P) of a polystyrene dielectric in a coaxial conductor with radii a and b. Solution: 1. Write the formula for the electric displacement field (D) in cylindrical coordinates: D = Dρ(ρ)ar. 2. Express D in terms of polarization P: Dρ(ρ) = ε0Eρ + Pρ. 3. Solve for the electric field (E) as a function of ρ: E(ρ) = (Dρ(ρ) - Pρ) / ε0 ar. 4. Write the formula for potential difference in a coaxial conductor: Vab = -∫[a,b] Eρ(ρ) dρ. 5. Calculate the potential difference V_ab using the expression for E from step 3. 6. Write the formula for electric susceptibility (χe): χe = Pρ / (ε0Eρ). 7. Calculate the electric susceptibility χe using the given values of P and E, and the value of ε0. 8. Write the formula for polarization p(ρ) in terms of the number of molecules per unit volume: p(ρ) = P(ρ) / N. 9. Calculate p(ρ) using the given values of P and N.

Step by step solution

01

Write the formula for the electric displacement field (D) in cylindrical coordinates

To find the electric displacement field in cylindrical coordinates, we can use the following formula: \[\mathbf{D} = D_{\rho}(\rho) \mathbf{a_{\rho}}\]
02

Express D in terms of the polarization P

The relationship between electric displacement field (D) and polarization (P) is given by the following equation: \[\mathbf{D} = \epsilon_0 \mathbf{E} + \mathbf{P}\] Now, we already know the polarization P in the dielectric, so we can express D in terms of P: \[D_{\rho}(\rho) = \epsilon_0 E_{\rho} + P_{\rho}\]
03

Solve for the electric field (E) as a function of ρ

Using the formula from Step 2, we can solve for the electric field (E) as a function of ρ: \[\mathbf{E}(\rho) = \frac{D_{\rho}(\rho) - P_{\rho}}{\epsilon_0} \mathbf{a_{\rho}}\] Now we have the electric field as a function of ρ. #Phase 2: Finding V_ab, χe, and p(ρ)# Next, let's find the potential difference V_ab, the electric susceptibility χe, and the polarization p(ρ).
04

Write the formula for potential difference in a coaxial conductor

For a coaxial conductor, we can find the potential difference between the inner and outer conductors using the following equation: \[V_{ab} = -\int_{a}^{b} E_{\rho}(\rho) d\rho\]
05

Calculate the potential difference V_ab

Substitute the expression for E from Step 3 and evaluate the integral to find V_ab.
06

Write the formula for electric susceptibility (χe)

The electric susceptibility is defined as the ratio of the polarization to the electric field times the vacuum permittivity: \[\chi_{e} = \frac{P_{\rho}}{\epsilon_0 E_{\rho}}\]
07

Calculate the electric susceptibility χe

Substitute the given values of P and E, and the value of ε0, to find the electric susceptibility χe.
08

Write the formula for polarization p(ρ) in terms of the number of molecules per unit volume

The polarization in a medium can be expressed in terms of the electric field and the number of molecules per unit volume (N): \[\mathbf{p}(\rho) = \frac{\mathbf{P}(\rho)}{N}\]
09

Calculate p(ρ)

Substitute the given values of P and N to find the polarization p(ρ).

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