The objective is to determine the dielectric constant \(K_2\) of a parallel plate capacitor after two dielectric slabs have been inserted, resulting in a doubling of its capacitance.
The initial capacitance, without any dielectric, is defined as:
\(C_0 = \frac{\varepsilon_0 A}{d}\)
Here, \( \varepsilon_0 \) represents the permittivity of free space, and \(A\) is the area of the capacitor plates.
Upon inserting two dielectric slabs with constants \(K_1\) and \(K_2\), the effective capacitance \(C\) is expressed as:
\(\frac{1}{C} = \frac{d_1}{K_1 \varepsilon_0 A} + \frac{d_2}{K_2 \varepsilon_0 A}\)
Given that \(d_1 = d_2 = \frac{d}{2}\), substituting these values yields:
\(\frac{1}{C} = \frac{d}{2K_1 \varepsilon_0 A} + \frac{d}{2K_2 \varepsilon_0 A}\)
Simplifying this equation gives:
\(\frac{1}{C} = \frac{d(K_2 + K_1)}{2K_1 K_2 \varepsilon_0 A}\)
Since the final capacitance is twice the original capacitance, \(C = 2C_0\), we can write:
\( \frac{1}{2C_0} = \frac{d(K_2 + K_1)}{2K_1 K_2 \varepsilon_0 A}\)
This simplifies to:
\(2K_1 K_2 = K_2 + K_1\)
Substituting \(K_1 = 1.25K_2\) into the equation:
\(2(1.25K_2)K_2 = K_2 + 1.25K_2\)
Further simplification results in:
\(2.5K_2^2 = 2.25K_2\)
Assuming \(K_2 eq 0\), we can cancel \(K_2\) from both sides:
\(2.5K_2 = 2.25\)
Solving for \(K_2\):
\(K_2 = \frac{2.25}{2.5} = 1.60\)
Therefore, the required value for \(K_2\) is 1.60.