Example: Charging RC

Solution
  • 2: Circuit diagram
  • 3: ℰ = 2.8V, C = 1.0F, R = 6.0Ω
  • 4: Capacitor, and charging RC circuit
  • 5: Q = C ΔV ← capacitor PE = 1/2 C (ΔV)2
    ΔV = ℰ (1 - e^(-t/τ)) ← charging RC circuit
    τ = R C
  • 6/7: τ = 6.0s
    Initially, ΔV = 0, Q = 0, PE = 0, and I = ℰ / R = 0.47A.
    I = 2.8V / 6.0Ω × e^(-15s/6s) = 0.038A
    ΔV = 2.8V (1-e^(-15s/6.0s)) = 2.57V
    Q = ΔV / C = 2.57C
    t = -τ ln(1-ΔV / ℰ) = -6.0s * ln(.64) = 2.7s
    PE = 1/2 C (ΔV)2 = 3.3J
  • 8: Units (charge = C, potential difference = V, PE = J)
    15s = 2.5 time constants. After 1 time constant, the capacitor will be 63% (1-1/e) charged. So, we expect the charge to be nearly its maximum (ΔV = 2.8V, Q = ΔV/C = 2.8C) and the current to be relatively low compared to initial (I ≪ 0.47A).
    Note: A charge of 2.57C would be extraordinary, but remember that is not the net charge of the capacitor (0C), but the amount of charge that has been separated.

Problem: discharging RC (worksheet?)

Solution
  • τ = 2.88s
    at 0s ΔV = 3V, at 4s ΔV = 0.75V
    at 0s I = 25μA, at 3.6s I = 7.2μA
    at 0s PE = 0.11mJ, at 2.4s PE = 6.7μJ