The electric field must be zero inside a conductor in electrostatic equilibrium, but not inside an insulator. It turns out that we can still apply Gauss's law to a Gaussian surface that is entirely within an insulator by replacing the right-hand side of Gauss's law, Qin /ɛ0, with Qin /e, where e is the permittivity of the material. (Technically, eo is called the vacuum permittivity.) Suppose that a 40 nC point charge is surrounded by a thin, 32-cm-diameter spherical rubber shell and that the electric field strength inside the rubber shell is 2500 N/C. Part A What is the permittivity of rubber? ? C /N • m? Submit Request Answer

College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
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**Concept:**

The electric field must be zero inside a conductor in electrostatic equilibrium, but not inside an insulator. It turns out that we can still apply Gauss's law to a Gaussian surface that is entirely within an insulator by replacing the right-hand side of Gauss's law, \( Q_{\text{in}}/\varepsilon_0 \), with \( Q_{\text{in}}/\varepsilon \), where \( \varepsilon \) is the permittivity of the material. (Technically, \( \varepsilon_0 \) is called the vacuum permittivity.) Suppose that a \( 40 \, \text{nC} \) point charge is surrounded by a thin, \( 32\text{-cm}\)-diameter spherical rubber shell and that the electric field strength inside the rubber shell is \( 2500 \, \text{N/C} \).

---

**Exercise: Part A**

**Question:**
What is the permittivity of rubber?

**Input Box:**
\[ \varepsilon = \, \]
\[ \text{C}^2/\text{N} \cdot \text{m}^2 \]

**Options:**
- Submit
- Request Answer

**Explanation:**
You are asked to determine the permittivity (\( \varepsilon \)) of the rubber based on the given scenario using the principles of electrostatics and Gauss's law.
Transcribed Image Text:**Concept:** The electric field must be zero inside a conductor in electrostatic equilibrium, but not inside an insulator. It turns out that we can still apply Gauss's law to a Gaussian surface that is entirely within an insulator by replacing the right-hand side of Gauss's law, \( Q_{\text{in}}/\varepsilon_0 \), with \( Q_{\text{in}}/\varepsilon \), where \( \varepsilon \) is the permittivity of the material. (Technically, \( \varepsilon_0 \) is called the vacuum permittivity.) Suppose that a \( 40 \, \text{nC} \) point charge is surrounded by a thin, \( 32\text{-cm}\)-diameter spherical rubber shell and that the electric field strength inside the rubber shell is \( 2500 \, \text{N/C} \). --- **Exercise: Part A** **Question:** What is the permittivity of rubber? **Input Box:** \[ \varepsilon = \, \] \[ \text{C}^2/\text{N} \cdot \text{m}^2 \] **Options:** - Submit - Request Answer **Explanation:** You are asked to determine the permittivity (\( \varepsilon \)) of the rubber based on the given scenario using the principles of electrostatics and Gauss's law.
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