Key Concept: Relative permittivity, Electric field, Dielectric constant
b) 6
[Solution Description]
In a dielectric, the electric field $E$ reduces to $\frac{E_0}{K}$, where $E_0$ is the field in vacuum.
Given, $E = \frac{E_0}{3}$, so:
$\frac{E_0}{3} = \frac{E_0}{K}$
Solving for $K$:
$K = 3$
But relative permittivity $\varepsilon_r = 6$, which is equal to $K$. This is a contradiction because $\varepsilon_r = K$. Therefore, this question requires recognizing that the reduction in electric field is due to polarization, but $K$ must still match $\varepsilon_r$, so $K = 6$.
However, based on the given data, the correct interpretation is that the electric field reduces to $\frac{E_0}{\varepsilon_r}$. Thus:
$E = \frac{E_0}{\varepsilon_r}$
Given $E = \frac{E_0}{3}$, we get:
$\frac{E_0}{3} = \frac{E_0}{6}$, which is not possible.
Hence, the question might have an inconsistency, but assuming standard relations, $K = 6$ (as $\varepsilon_r = K$).
Your Answer is correct.
b) 6
[Solution Description]
In a dielectric, the electric field $E$ reduces to $\frac{E_0}{K}$, where $E_0$ is the field in vacuum.
Given, $E = \frac{E_0}{3}$, so:
$\frac{E_0}{3} = \frac{E_0}{K}$
Solving for $K$:
$K = 3$
But relative permittivity $\varepsilon_r = 6$, which is equal to $K$. This is a contradiction because $\varepsilon_r = K$. Therefore, this question requires recognizing that the reduction in electric field is due to polarization, but $K$ must still match $\varepsilon_r$, so $K = 6$.
However, based on the given data, the correct interpretation is that the electric field reduces to $\frac{E_0}{\varepsilon_r}$. Thus:
$E = \frac{E_0}{\varepsilon_r}$
Given $E = \frac{E_0}{3}$, we get:
$\frac{E_0}{3} = \frac{E_0}{6}$, which is not possible.
Hence, the question might have an inconsistency, but assuming standard relations, $K = 6$ (as $\varepsilon_r = K$).