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

    A top-down flowchart. The top node, 'Capacitor–resistor circuit', branches into two nodes: 'Discharging' and 'Charging'. From 'Discharging' a node reads 'Charge Q, p.d. V and current I decay', which leads to the equation 'x = x₀e^(−t/CR)'. From 'Charging', two branches emerge: one node reads 'Charge Q and p.d. V rise' and leads to 'x = x₀(1 − e^(−t/CR))'; the other reads 'Current I decays' and leads to 'I = I₀e^(−t/CR)'.
    It shows which equation applies to each quantity during discharging and charging in a capacitor–resistor circuit.

    Key words

    Say what each word means before you turn the card.

    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.

    Label the diagram

    Some boxes have lost their names. Pick the right name for each number.

    The diagram again, with 3 boxes numbered instead of named. A top-down flowchart. The top node, 'Capacitor–resistor circuit', branches into two nodes: 'Discharging' and 'Charging'. From 'Discharging' a node reads 'Charge Q, p.d. V and current I decay', which leads to the equation 'x = x₀e^(−t/CR)'. From 'Charging', two branches emerge: one node reads 'Charge Q and p.d. V rise' and leads to 'x = x₀(1 − e^(−t/CR))'; the other reads 'Current I decays' and leads to 'I = I₀e^(−t/CR)'.
    • 1Box 1

    • 2Box 2

    • 3Box 3

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