AQA · A-Level · Physics

    Course version: 7408 · Version from Sept 2016

    Sinusoidal voltages and currents only; root mean square, peak and…

    Full specification wording

    Alternating currents (A-level only): Sinusoidal voltages and currents only; root mean square, peak and peak-to-peak values for sinusoidal waveforms only.

    For a sinusoidal alternating voltage or current, the value changes continuously, so a single representative value is needed for power calculations.

    Checked against the AQA 7408 specification (opens in a new tab) on .

    • Point 1 of 3
    • 4 key terms

    Study notes

    From the checked teaching notes for this specification point.

    The idea

    For a sinusoidal alternating voltage or current, the value changes continuously, so a single representative value is needed for power calculations. The root mean square value is the steady direct value that would dissipate the same average power in a given resistor. For a sinusoid, V_rms = V₀/√2 and I_rms = I₀/√2, where V₀ and I₀ are peak values. The peak-to-peak value is the difference between the maximum positive and maximum negative values, so V_pp = 2V₀. Average power is P = I_rms²R = V_rms²/R = I_rms V_rms for a resistor. These relationships apply only to sinusoidal waveforms; other waveforms need their own rms calculation.

    What earns the marks

    • Defines the root mean square value of an alternating current or voltage as the steady direct value that produces the same average power in a resistor.
    • States and applies the sinusoidal relationships V_rms = V₀/√2 and I_rms = I₀/√2, where V₀ and I₀ are peak values.
    • Calculates peak-to-peak values from peak values using V_pp = 2V₀, and converts between peak, peak-to-peak and rms values for sinusoidal waveforms.
    • Uses rms values to calculate average power in a resistor with P = I_rms²R, P = V_rms²/R or P = I_rms V_rms.
    • Explains that the √2 factor arises from averaging the square of a sinusoidal function over a complete cycle, and that it applies only to sinusoidal waveforms.

    Common mistakes and how to put them right

    • Using peak values directly in power equations such as P = I₀²R.

      Put it right: Use rms values, so P = I_rms²R = I₀²R/2 for a sinusoid.

    • Confusing peak-to-peak with peak and dividing by √2 twice.

      Put it right: Halve the peak-to-peak value first to obtain the peak, then divide by √2 for the rms value.

    • Applying the √2 relationships to non-sinusoidal waveforms such as square or triangular waves.

      Put it right: Use the defining average-power method or the specific rms value for that waveform.

    Exam tips

    • Write down whether a quoted value is peak, peak-to-peak or rms before substituting it, since mixing them is the most common source of error.
    • Show the conversion steps explicitly, for example peak-to-peak to peak by halving, then peak to rms by dividing by √2.
    • When calculating power, choose the form of the equation that matches the quantity given, such as P = V_rms²/R when the rms voltage is known.

    Try the lesson

    The start of the Alternating currents (A-level only): Sinusoidal voltages and currents only; root mean square, peak and peak-to-peak values for sinusoidal waveforms only. lesson, made from checked teaching notes for this specification point.

    Have a go first

    A sinusoidal alternating voltage has a peak value of 12 V. What is its root mean square value?

    Listen

    For a sinusoidal alternating voltage or current, the value changes continuously, so a single representative value is needed for power calculations. The root mean square value is the steady direct value that would dissipate the same average power in a given resistor. For a sinusoid, V_rms = V₀/√2 and I_rms = I₀/√2, where V₀ and I₀ are peak values. The peak-to-peak value is the difference between the maximum positive and maximum negative values, so V_pp = 2V₀. Average power is P = I_rms²R = V_rms²/R = I_rms V_rms for a resistor. These relationships apply only to sinusoidal waveforms; other waveforms need their own rms calculation. A strong answer earns marks for these points. Defines the root mean square value of an alternating current or voltage as the steady direct value that produces the same average power in a resistor. States and applies the sinusoidal relationships V_rms = V₀/√2 and I_rms = I₀/√2, where V₀ and I₀ are peak values. Calculates peak-to-peak values from peak values using V_pp = 2V₀, and converts between peak, peak-to-peak and rms values for sinusoidal waveforms. Uses rms values to calculate average power in a resistor with P = I_rms²R, P = V_rms²/R or P = I_rms V_rms. A common slip: Using peak values directly in power equations such as P = I₀²R. Instead, use rms values, so P = I_rms²R = I₀²R/2 for a sinusoid. Exam tip: Write down whether a quoted value is peak, peak-to-peak or rms before substituting it, since mixing them is the most common source of error.

    Key words

    Say what each word means before you turn the card.

    Root mean square value

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    Peak-to-peak value

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    Average power

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    Sinusoidal waveforms

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    See every definition
    Root mean square value
    The steady direct value that would dissipate the same average power in a given resistor.
    Peak-to-peak value
    The difference between the maximum positive and maximum negative values, so V_pp = 2V₀.
    Average power
    For a resistor, P = I_rms²R = V_rms²/R = I_rms V_rms.
    Sinusoidal waveforms
    The relationships V_rms = V₀/√2 and I_rms = I₀/√2 apply only to these; other waveforms need their own rms calculation.

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