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If the gap between the plates of a paral...

If the gap between the plates of a parallel plate capacitor is filled with medium of dielectric constant k=2 , then the field between them

A

Increases by a factor 2

B

Increases by a factor `sqrt(2)`

C

Decreased by a factor `sqrt(2)`

D

Decreased by a factor `1//2`

Text Solution

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To solve the problem of finding the electric field between the plates of a parallel plate capacitor when a dielectric medium with a dielectric constant \( k = 2 \) is introduced, we can follow these steps: ### Step 1: Understand the Initial Condition Initially, we have a parallel plate capacitor with air (or vacuum) between the plates. The electric field \( E \) in this case can be expressed as: \[ E = \frac{Q}{A \epsilon_0} \] where \( Q \) is the charge on one plate, \( A \) is the area of the plates, and \( \epsilon_0 \) is the permittivity of free space. ### Step 2: Introduce the Dielectric Medium When a dielectric medium with dielectric constant \( k \) is introduced between the plates, the electric field \( E' \) in the presence of the dielectric is given by: \[ E' = \frac{E}{k} \] This means the electric field is reduced by a factor of \( k \). ### Step 3: Substitute the Dielectric Constant Given that the dielectric constant \( k = 2 \), we can substitute this value into the equation: \[ E' = \frac{E}{2} \] ### Step 4: Relate the New Electric Field to the Original Electric Field Since we already established that the original electric field \( E \) is: \[ E = \frac{Q}{A \epsilon_0} \] We can express the new electric field as: \[ E' = \frac{1}{2} \cdot \frac{Q}{A \epsilon_0} \] ### Step 5: Conclusion Thus, the electric field between the plates when the dielectric medium is introduced is reduced by a factor of 2: \[ E' = \frac{E}{2} \] ### Final Answer The electric field between the plates is decreased by a factor of 2. ---

To solve the problem of finding the electric field between the plates of a parallel plate capacitor when a dielectric medium with a dielectric constant \( k = 2 \) is introduced, we can follow these steps: ### Step 1: Understand the Initial Condition Initially, we have a parallel plate capacitor with air (or vacuum) between the plates. The electric field \( E \) in this case can be expressed as: \[ E = \frac{Q}{A \epsilon_0} \] where \( Q \) is the charge on one plate, \( A \) is the area of the plates, and \( \epsilon_0 \) is the permittivity of free space. ...
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