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At which distance along the centre axis ...

At which distance along the centre axis of a uniformaly charged plastic disc of radius R is the magnitude of the electric field equal to one-half the magnitude of the field at the centre of the surface of the disc ?

A

`(R)/(sqrt2)`

B

`(R)/(sqrt3)`

C

`sqrt2R`

D

`sqrt(3R)`

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The correct Answer is:
To solve the problem, we need to find the distance \( x \) along the center axis of a uniformly charged plastic disc of radius \( R \) where the electric field is equal to one-half the magnitude of the electric field at the center of the disc. ### Step-by-Step Solution: 1. **Understanding the Electric Field at the Center of the Disc:** The electric field \( E_C \) at the center of a uniformly charged disc is given by the formula: \[ E_C = 2k \pi \sigma \] where \( k \) is Coulomb's constant and \( \sigma \) is the surface charge density. 2. **Electric Field at a Distance \( x \) Along the Axis:** The electric field \( E_x \) at a distance \( x \) along the axis of the disc is given by: \[ E_x = 2k \pi \sigma \left(1 - \frac{x}{\sqrt{x^2 + R^2}}\right) \] 3. **Setting Up the Equation:** According to the problem, we need to find the distance \( x \) such that: \[ E_x = \frac{1}{2} E_C \] Substituting the expression for \( E_C \): \[ E_x = \frac{1}{2} (2k \pi \sigma) = k \pi \sigma \] 4. **Equating the Two Expressions:** Now we set \( E_x \) equal to \( k \pi \sigma \): \[ 2k \pi \sigma \left(1 - \frac{x}{\sqrt{x^2 + R^2}}\right) = k \pi \sigma \] 5. **Simplifying the Equation:** Dividing both sides by \( k \pi \sigma \) (assuming \( \sigma \neq 0 \)): \[ 2 \left(1 - \frac{x}{\sqrt{x^2 + R^2}}\right) = 1 \] Simplifying further: \[ 2 - 2\frac{x}{\sqrt{x^2 + R^2}} = 1 \] \[ 2\frac{x}{\sqrt{x^2 + R^2}} = 1 \] \[ \frac{x}{\sqrt{x^2 + R^2}} = \frac{1}{2} \] 6. **Squaring Both Sides:** Squaring both sides to eliminate the square root: \[ x^2 = \frac{1}{4}(x^2 + R^2) \] 7. **Rearranging the Equation:** Rearranging gives: \[ 4x^2 = x^2 + R^2 \] \[ 3x^2 = R^2 \] 8. **Solving for \( x \):** Finally, we solve for \( x \): \[ x^2 = \frac{R^2}{3} \] \[ x = \frac{R}{\sqrt{3}} \] ### Final Answer: The distance \( x \) along the center axis of the uniformly charged plastic disc where the electric field is equal to one-half the magnitude of the field at the center of the disc is: \[ x = \frac{R}{\sqrt{3}} \]
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