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Question
**The answer is** 

\[
V = 
\begin{cases} 
\frac{\sigma}{\epsilon_0} y & \text{for } y < 0 \\ 
0 & \text{for } 0 < y < d \\ 
-\frac{\sigma}{\epsilon_0} (y - d) & \text{for } y > d 
\end{cases}
\]

If that was *not* your result, use *this* potential next.

**6. (a)** Now compute \(-\nabla V = - \left( \frac{\partial V}{\partial x} \hat{i} + \frac{\partial V}{\partial y} \hat{j} + \frac{\partial V}{\partial z} \hat{k} \right)\) for \(y < 0\), \(0 < y < d\), and \(d < y\).

(b) Should your result agree with the electric field \(\mathbf{E}\) that you calculated in problem 2? Does it agree?

**7.** What is the value of the integral \(\oint \mathbf{E} \cdot d\mathbf{r}\) over a closed path? You need to be specially clear and compelling here to earn the points.

**8. (a)** Describe the equipotential surfaces with \(V = -5,000\) Volts. Where are they located?

(b) Is there an equipotential volume? If the answer is “yes,” describe it.

(c) Describe all the equipotential surfaces \(V = V_0\) for \(V_0 < 0\) fixed but arbitrary. Where are they located as a function of \(V_0\)?
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Transcribed Image Text:**The answer is** \[ V = \begin{cases} \frac{\sigma}{\epsilon_0} y & \text{for } y < 0 \\ 0 & \text{for } 0 < y < d \\ -\frac{\sigma}{\epsilon_0} (y - d) & \text{for } y > d \end{cases} \] If that was *not* your result, use *this* potential next. **6. (a)** Now compute \(-\nabla V = - \left( \frac{\partial V}{\partial x} \hat{i} + \frac{\partial V}{\partial y} \hat{j} + \frac{\partial V}{\partial z} \hat{k} \right)\) for \(y < 0\), \(0 < y < d\), and \(d < y\). (b) Should your result agree with the electric field \(\mathbf{E}\) that you calculated in problem 2? Does it agree? **7.** What is the value of the integral \(\oint \mathbf{E} \cdot d\mathbf{r}\) over a closed path? You need to be specially clear and compelling here to earn the points. **8. (a)** Describe the equipotential surfaces with \(V = -5,000\) Volts. Where are they located? (b) Is there an equipotential volume? If the answer is “yes,” describe it. (c) Describe all the equipotential surfaces \(V = V_0\) for \(V_0 < 0\) fixed but arbitrary. Where are they located as a function of \(V_0\)?
Expert Solution
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Step 1

6.(a)

Given:

The potential is given by V=σε0y                       y<00                             0<y<d -σε0(y-d)            y>d  

Introduction:

The electric field is defined as the electric force per unit charge. The direction of the field is taken to be the direction of the force it would exert on a positive test charge. The electric field is radially outward from a positive charge and radially in toward a negative point charge.