Related Formula
Capacitive reactance:
XC = (1)/(ω C)$$X_C = \frac{1}{\omega C}$$
Conduction Current (Irms$I_{\text{rms}}$):
Irms = VrmsXC = Vrms · ω C$$I_{\text{rms}} = \frac{V_{\text{rms}}}{X_C} = V_{\text{rms}} \cdot \omega C$$
Continuity relation:
Ic = Id$I_c = I_d$
Core Logic
Given parameters:
C = 200~pF = 200 × 10⁻¹²~F$C = 200\mathrm{~pF} = 200 \times 10^{-12}\mathrm{~F}$, Vrms = 230~V$V_{\text{rms}} = 230\mathrm{~V}$, ω = 300~rad/s$\omega = 300\mathrm{~rad/s}$.
Calculate current:
I = Vrms · ω C = 230 × 300 × 200 × 10⁻¹²$$I = V_{\text{rms}} \cdot \omega C = 230 \times 300 \times 200 \times 10^{-12}$$
Step 1: Simplify Numerical Calculation
I = 230 × 60000 × 10⁻¹² = 13.8 × 10⁻⁶~A = 13.8~μ A$I = 230 \times 60000 \times 10^{-12} = 13.8 \times 10^{-6}\mathrm{~A} = 13.8\mathrm{~\mu A}$
By Maxwell's electromagnetic formulation, the displacement current Id$I_d$ within the dielectric space matches the exterior conduction current Ic$I_c$ seamlessly in magnitude.
Pattern Recognition
Factual invariant: Conduction current always equals displacement current inside a standard layout loop context (Ic = Id$I_c = I_d$).
Chapter Mix
Class 12 Physics: Electromagnetic Waves
Class 12 Physics: Alternating Current