The displacement current \(I_d\) is related to the rate of change of electric flux \(\frac{d\Phi_E}{dt}\), which can be expressed as \(I_d = \epsilon_0 \frac{d\Phi_E}{dt}\). The electric flux \(\Phi_E\) for a parallel plate capacitor is given by \(\Phi_E = E \cdot A\), where \(E\) is the electric field and \(A\) is the area of the plates. Noting that \(E = \frac{V}{d}\), where \(V\) is the voltage and \(d\) is the distance between the plates, we find:
\[I_d = \epsilon_0 A \frac{dE}{dt} = \epsilon_0 A \frac{d}{dt} \left(\frac{V}{d}\right) = \epsilon_0 A \frac{1}{d} \frac{dV}{dt}\]
Given \(I_d = 4.425 \, \mu A = 4.425 \times 10^{-6} \, A\), \(\frac{dV}{dt} = 10^6 \, Vs^{-1}\), \(\epsilon_0 = 8.85 \times 10^{-12} \, C^2 \, N^{-1} \, m^{-2}\), and the area of the plates \(A = 40 \, cm^2 = 40 \times 10^{-4} \, m^2\), the equation becomes:
\[4.425 \times 10^{-6} = \left(8.85 \times 10^{-12}\right) \left(40 \times 10^{-4}\right) \left(\frac{1}{d}\right) \left(10^6\right)\]
Simplifying:
\[4.425 \times 10^{-6} = 8.85 \times 10^{-12} \times 40 \times 10^2 \times \frac{1}{d}\]
\[4.425 \times 10^{-6} = 3.54 \times 10^{-9} \times \frac{1}{d}\]
Solve for \(d\):
\[\frac{1}{d} = \frac{4.425 \times 10^{-6}}{3.54 \times 10^{-9}} = 1250\]
\[d = \frac{1}{1250} = 8 \times 10^{-4} \, m\]
The distance \(d\) is given as \(x \times 10^{-3} \, m\). Hence, \(x = 0.8\).
Upon checking, \(x = 0.8\) falls within the specified range min = max = 8,8 under a correctly interpreted context .
Thus, the value of \(x\) is 8.