4.10.4

Capacitor Discharge

Test yourself

Discharging a Capacitor

When a charged capacitor with capacitance C is connected to a resistor with resistance R, then the charge stored on the capacitor decreases exponentially.

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Discharge graph

  • Q=Q0etRCQ=Q_0e^{-\frac{t}{RC}}
  • Where Q0Q_0 is the initial charge on the capacitor.
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Time to halve

  • The time for the charge to reach half of the initial charge, T1/2T_{1/2}, can be found:
    • Q=Q02=Q0eT1/2RCQ=\frac{Q_0}{2}=Q_0e^{-\frac{T_{1/2}}{RC}}
    • 0.5=eT1/2RC0.5=e^{-\frac{T_{1/2}}{RC}}
    • ln(0.5)=ln(eT1/2RC)\ln (0.5)=\ln (e^{-\frac{T_{1/2}}{RC}})
    • ln(2)=T1/2RC-\ln(2)=-\frac{T_{1/2}}{RC}
    • T1/2=RCln2T_{1/2}=RC\ln 2
  • Because ln(2)=0.69, T1/2=0.69RC\ln(2) = 0.69,\space T_{1/2}=0.69RC.
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Time constant

  • The product RC is known as the time constant.
  • It is a property of exponential decay graphs that the curve will decrease by a constant fraction with each time constant.

Potential Difference and Current in a Discharging Capacitor

The potential difference and the current in a discharging capacitor have similar forms.

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Potential difference

  • The potential difference across a capacitor with time constant RC, initial potential difference V0, and having been discharged for a time t is:
    • V=V0etRCV=V_0e^{-\frac{t}{RC}}
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Current

  • The current passing through a capacitor with time constant RC, initial current I0, and having been discharged for a time t is:
    • I=I0etRCI=I_0e^{-\frac{t}{RC}}
    • R is the resistance across the capacitor
  • I0=V0RI_0=\frac{V_0}{R}

Jump to other topics

1Space, Time & Motion

2The Particulate Nature of Matter

3Wave Behaviour

4Fields

4.1Circular Motion

4.2Newton's Law of Gravitation

4.3Fields

4.4Fields at Work

4.5Electric Fields

4.6Magnetic Effect of Electric Currents

4.7Heating Effect of Currents

4.8Electromagnetic Induction

4.9Power Generation & Transmission

4.10Capacitance

5Nuclear & Quantum Physics

6Measurements

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