OCR · A-Level · Physics
Course version: H556 · Version from Sept 2015
(c) equations of the form x = x₀e^(−t/CR) and x = x₀(1 − e^(−t/CR)) for…
Full specification wording
Charging and discharging capacitors: (c) equations of the form x = x₀e^(−t/CR) and x = x₀(1 − e^(−t/CR)) for capacitor–resistor circuits
In a capacitor–resistor circuit, the time constant \(\tau = CR\) determines the rate of charging and discharging.
Checked against the OCR H556 specification (opens in a new tab) on .
- Point 4 of 6
- 3 key terms
Study notes
From the checked teaching notes for this specification point.
The idea
In a capacitor–resistor circuit, the time constant \(\tau = CR\) determines the rate of charging and discharging. For a discharging capacitor, charge \(Q\), potential difference \(V\), and current \(I\) all decay exponentially according to \(x = x_0 e^{-t/CR}\), where \(x_0\) is the initial value. During charging, the charge and potential difference rise towards a maximum steady value according to \(x = x_0(1 - e^{-t/CR})\). However, the charging current does not rise; it decays exponentially from an initial maximum as the capacitor opposes further charge flow, following \(I = I_0 e^{-t/CR}\). The exponent \(-t/CR\) must be dimensionless, requiring \(t\) and \(CR\) to be in seconds.
For example: After \(t = CR\), a discharging quantity falls to \(x_0 e^{-1} \approx 0.37 x_0\), while a charging \(V\) or \(Q\) rises to \(x_0(1 - e^{-1}) \approx 0.63 x_0\).
What earns the marks
- Select and apply the discharging equation \(x = x_0 e^{-t/CR}\) for charge, potential difference, or current.
- Select and apply the charging equation \(x = x_0(1 - e^{-t/CR})\) for charge and potential difference only.
- Recognise that current decays exponentially as \(I = I_0 e^{-t/CR}\) during both charging and discharging processes.
- Ensure the exponent \(-t/CR\) is dimensionless by using consistent units of seconds for both \(t\) and \(CR\).
Common mistakes and how to put them right
Assuming current rises during charging.
Put it right: Current always decays exponentially in both charging and discharging circuits, following \(I = I_0 e^{-t/CR}\).
Using the charging equation for a discharging process or vice versa.
Put it right: Use \(x = x_0 e^{-t/CR}\) for decreasing quantities and \(x = x_0(1 - e^{-t/CR})\) for increasing quantities.
Treating \(x_0\) as the final value in the discharging equation.
Put it right: In \(x = x_0 e^{-t/CR}\), \(x_0\) is the initial value at \(t = 0\).
Exam tips
- Always check which quantity is being asked for during charging; use the \((1 - e^{-t/CR})\) form for \(Q\) and \(V\), but the \(e^{-t/CR}\) form for \(I\).
- To find \(\tau\) from a graph, plot \(\ln x\) against \(t\) for a decaying quantity; the gradient is \(-1/CR\).
- Remember that after one time constant, a decaying quantity is about 37% of its initial value, and a rising quantity is about 63% of its final value.
Try the lesson
The start of the Charging and discharging capacitors: (c) equations of the form x = x₀e^(−t/CR) and x = x₀(1 − e^(−t/CR)) for capacitor–resistor circuits lesson, made from checked teaching notes for this specification point.
Listen
In a capacitor–resistor circuit, the time constant \(\tau = CR\) determines the rate of charging and discharging. For a discharging capacitor, charge \(Q\), potential difference \(V\), and current \(I\) all decay exponentially according to \(x = x_0 e^{-t/CR}\), where \(x_0\) is the initial value. During charging, the charge and potential difference rise towards a maximum steady value according to \(x = x_0(1 - e^{-t/CR})\). However, the charging current does not rise; it decays exponentially from an initial maximum as the capacitor opposes further charge flow, following \(I = I_0 e^{-t/CR}\). The exponent \(-t/CR\) must be dimensionless, requiring \(t\) and \(CR\) to be in seconds. For example, after \(t = CR\), a discharging quantity falls to \(x_0 e^{-1} \approx 0.37 x_0\), while a charging \(V\) or \(Q\) rises to \(x_0(1 - e^{-1}) \approx 0.63 x_0\). A strong answer earns marks for these points. Select and apply the discharging equation \(x = x_0 e^{-t/CR}\) for charge, potential difference, or current. Select and apply the charging equation \(x = x_0(1 - e^{-t/CR})\) for charge and potential difference only. Recognise that current decays exponentially as \(I = I_0 e^{-t/CR}\) during both charging and discharging processes. Ensure the exponent \(-t/CR\) is dimensionless by using consistent units of seconds for both \(t\) and \(CR\). A common slip: Assuming current rises during charging. Instead, current always decays exponentially in both charging and discharging circuits, following \(I = I_0 e^{-t/CR}\). Exam tip: Always check which quantity is being asked for during charging; use the \((1 - e^{-t/CR})\) form for \(Q\) and \(V\), but the \(e^{-t/CR}\) form for \(I\).
See it
Key words
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Exponential decay and growth
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Time constant
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Capacitor charging and discharging
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See every definition
- Exponential decay and growth
- Describing quantities that fall according to x = x₀e^(−t/CR) or rise towards a maximum steady value according to x = x₀(1 − e^(−t/CR)).
- Time constant
- The quantity τ = CR, which determines the rate of charging and discharging in a capacitor–resistor circuit.
- Capacitor charging and discharging
- Processes in which charge and potential difference rise towards a maximum steady value during charging, or decay exponentially during discharging.
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