Another special case turns out to be of considerable interest. Let's see what the electric field is like near the center of a uniformly charged disk (x small, but not zero, for the reasons just given). Suppose that we are so close to the disk that x is very small (x <> x). QIA Show that near the disk E- R

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### 4: The Electric Field of Distributed Charges

#### 4.4.2 Electric Field Near the Center of a Uniform Disk

Another special case turns out to be of considerable interest. Let's see what the electric field is like near the center of a uniformly charged disk (x small, but not zero, for the reasons just given). Suppose that we are so close to the disk that \( x \) is very small (\( x \ll R \)), or equivalently that we are some distance away but the disk is very large (\( R \gg x \)).

\[ 
\text{Show that near the disk } E = \frac{Q/A}{2 \varepsilon_0} \left[1 - \frac{x}{R}\right]. 
\]

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This section is designed to help students understand the behavior of the electric field near the center of a uniformly charged disk. The conditions being analyzed are that the distance \( x \) from the center of the disk is much smaller than the radius \( R \) of the disk, indicating either a small \( x \) or a large \( R \). This specific scenario leads to an approximation for the electric field close to the center. The students are required to show the given formula through appropriate derivations and explanations.
Transcribed Image Text:--- ### 4: The Electric Field of Distributed Charges #### 4.4.2 Electric Field Near the Center of a Uniform Disk Another special case turns out to be of considerable interest. Let's see what the electric field is like near the center of a uniformly charged disk (x small, but not zero, for the reasons just given). Suppose that we are so close to the disk that \( x \) is very small (\( x \ll R \)), or equivalently that we are some distance away but the disk is very large (\( R \gg x \)). \[ \text{Show that near the disk } E = \frac{Q/A}{2 \varepsilon_0} \left[1 - \frac{x}{R}\right]. \] --- This section is designed to help students understand the behavior of the electric field near the center of a uniformly charged disk. The conditions being analyzed are that the distance \( x \) from the center of the disk is much smaller than the radius \( R \) of the disk, indicating either a small \( x \) or a large \( R \). This specific scenario leads to an approximation for the electric field close to the center. The students are required to show the given formula through appropriate derivations and explanations.
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