Home / Edexcel A Level / A Level (IAL) Physics (YPH11) / 4.22 Charge & Discharge Curves- Study Notes

Edexcel A Level (IAL) Physics-4.22 Charge & Discharge Curves- Study Notes- New Syllabus

Edexcel A Level (IAL) Physics -4.22 Charge & Discharge Curves- Study Notes- New syllabus

Edexcel A Level (IAL) Physics -4.22 Charge & Discharge Curves- Study Notes -Edexcel A level Physics – per latest Syllabus.

Key Concepts:

  •  

Edexcel A level Physics-Study Notes- All Topics

RC Circuits: Charge and Discharge Curves & the Time Constant \( RC \)

An RC circuit consists of a resistor and a capacitor connected in series. When connected to a d.c. supply, the capacitor charges; when disconnected and allowed to empty through the resistor, it discharges.

 Charging a Capacitor in an RC Circuit

When a capacitor is connected to a battery through a resistor:

  • Charge on the capacitor increases with time.
  • Potential difference across the capacitor increases.
  • Current in the circuit decreases with time.

Key equations during charging:

\( Q = CV\left(1 – e^{-t/RC}\right) \)

\( V_C = V\left(1 – e^{-t/RC}\right) \)

\( I = \dfrac{V}{R} e^{-t/RC} \)

Interpreting Charging Curves

  • The charge–time and voltage–time graphs rise exponentially.
  • The current–time graph falls exponentially.
  • The capacitor never becomes fully charged instantly.
  • As \( t \to \infty \), current approaches zero.

Discharging a Capacitor in an RC Circuit

When a charged capacitor is allowed to discharge through a resistor:

  • Charge on the capacitor decreases with time.
  • Potential difference across the capacitor decreases.
  • Current decreases with time.

Key equations during discharging:

\( Q = Q_0 e^{-t/RC} \)

\( V = V_0 e^{-t/RC} \)

\( I = I_0 e^{-t/RC} \)

 Interpreting Discharge Curves

  • Charge, voltage, and current decrease exponentially.
  • None of these quantities reach zero instantly.
  • The curve is steep at first and then gradually flattens.

The Time Constant \( RC \)

The time constant of an RC circuit is defined as:

\( \tau = RC \)

  • \( R \) = resistance (Ω)
  • \( C \) = capacitance (F)
  • \( \tau \) = time constant (s)

Physical Significance of the Time Constant

Charging:

  • After time \( RC \), the charge and voltage reach about 63% of their final values.

Discharging:

  • After time \( RC \), the charge and voltage fall to about 37% of their initial values.

Rule of thumb:

  • After \( 5RC \), charging or discharging is effectively complete.

 Effect of Changing \( R \) or \( C \)

  • Increasing \( R \) increases the time constant → slower charging/discharging.
  • Increasing \( C \) increases the time constant → slower charging/discharging.
  • Decreasing either makes the process faster.

Example (Easy)

A capacitor of \( 1000\ \mathrm{\mu F} \) is connected in series with a \( 2.0\ \mathrm{k\Omega} \) resistor. Calculate the time constant.

▶️ Answer / Explanation

\( \tau = RC = 2000 \times 1000\times10^{-6} = 2.0\ \mathrm{s} \)

Example (Medium)

State the fraction of maximum charge on a capacitor after one time constant during charging.

▶️ Answer / Explanation

After one time constant, charge ≈ \( 0.63Q_{\text{max}} \)

Example (Hard)

A charged capacitor discharges through a resistor with time constant \( 4.0\ \mathrm{s} \). Find the fraction of its initial voltage remaining after \( 4.0\ \mathrm{s} \).

▶️ Answer / Explanation

Use the discharge equation:

\( \dfrac{V}{V_0} = e^{-t/RC} = e^{-1} \approx 0.37 \)

Voltage remaining ≈ 37%

Scroll to Top