A parallel plate capacitor of area \( A = 16 \, \text{cm}^2 \) and separation between the plates \( 10 \, \text{cm} \), is charged by a DC current. Consider a hypothetical plane surface of area \( A_0 = 3.2 \, \text{cm}^2 \) inside the capacitor and parallel to the plates. At an instant, the current through the circuit is 6A. At the same instant the displacement current through \( A_0 \) is _____ mA.
To calculate the displacement current in a capacitor, we begin with the formula: \(I_d = \varepsilon_0 \frac{d\phi_E}{dt}\). Here, \(\varepsilon_0\) is the permittivity of free space, and \(\frac{d\phi_E}{dt}\) represents the rate of change of electric flux. The electric flux is defined as \(\phi_E = E \cdot A = \frac{Q}{\varepsilon_0} \cdot A\), where \(Q\) is the charge and \(E\) is the electric field. Since the current \(I = \frac{dQ}{dt}\), we can express the rate of change of electric flux as \(\frac{d\phi_E}{dt} = \frac{1}{\varepsilon_0} \cdot \frac{dQ}{dt} \cdot A\). Substituting this into the displacement current equation yields: \(I_d = A \cdot \frac{1}{\varepsilon_0} \cdot I\).
Given the area \(A_0 = 3.2 \, \text{cm}^2 = 3.2 \times 10^{-4} \, \text{m}^2\), current \(I = 6 \, \text{A}\), and \(\varepsilon_0 = 8.854 \times 10^{-12} \, \text{F/m}\), we substitute these values into the formula: \(I_d = 3.2 \times 10^{-4} \cdot \frac{6}{8.854 \times 10^{-12}}\). The result of this calculation is approximately \(I_d \approx 2.17 \times 10^{-3} \, \text{A}\), which is equivalent to 2170 mA. Therefore, the displacement current through \(A_0\) is 2170 mA, which falls within the provided range of 1200 mA.