PhysicsElectronics › Band-pass, band-stop and RC filters

Band-pass, band-stop and RC filters

A resistor and a capacitor in series make a low-pass or a high-pass filter, and the cut-off where the output has fallen to 0.71 sits at 1/2πRC. One tuned circuit gives band-pass across the resistor and band-stop across the inductor and capacitor together. No cut-off is a wall.

Resonant circuits and filters, part 2 of 2. Part 1 is Tuned circuits and the Q factor.

IN THIS TOPIC

  • Tell band-pass from band-stop and high-pass from low-pass, and find an RC filter's cut-off.
  • Say why no filter passes a single frequency, and set a passband against the width of the signal it has to carry.

COMMON MISCONCEPTION

A low-pass filter blocks every frequency above its cut-off.

It attenuates rather than blocks. At the cut-off itself the output is still 1/21/\sqrt{2}, about 0.71, of full size, and the response slides away from there over a decade or more, so a frequency ten times the cut-off still comes through at about a tenth of its size.

Two filters from one tuned circuit

A tuned circuit on its own is a curve, not yet a filter. It becomes one as soon as a pair of output terminals is chosen, and the same components give opposite responses depending on which pair.

Where the output is taken determines what the circuit does. Take it across the resistor and the response peaks at f0f_{0}, since that is where the current, and so the pd across the resistor, is largest. That is a band-pass filter, passing a band of width fBf_{B} centred on resonance. Take the output across the series inductor and capacitor instead and the result is the mirror image. Their combined reactance vanishes at resonance, so the output there falls to zero while everything well away from resonance gets through. That is a band-stop filter, or a notch.

Two response curves against frequency for one tuned circuit. The band-pass rises to a peak of one at the resonant frequency and falls away either side; the band-stop is its mirror, near one far from resonance and dropping to zero at the resonant frequency.
FIG. 1The two responses of one tuned circuit. The band-pass peaks at the resonant frequency; the band-stop is its mirror, near full output far from resonance and zero at the resonant frequency itself.

Both have uses. A receiver's band-pass keeps one station and rejects its neighbours. A band-stop removes a single unwanted frequency, such as 50 Hz mains hum on an audio line or an interfering transmitter close to the wanted frequency.

No tuned circuit passes a single frequency, and one that came close would be useless, because a real signal occupies a band of frequencies rather than a single line. The passband has to be wide enough to carry that band: if Q is too high, the higher audio frequencies of a broadcast are attenuated.

GUIDED PRACTICE

How fussy must a radio be

Medium-wave stations sit 9 kHz apart. A receiver tuned to 909 kHz has to keep its own station and reject the next one along. Estimate the Q its tuned circuit needs.

Show the working

The bandwidth it can afford is about the channel spacing, 9 kHz.

Q = f0/fBf_{0}/f_{B} = 909/9 = about 100, an ordinary figure for a coil and capacitor.

Check a designed bandwidth against the channel spacing rather than making it as narrow as the components allow. Sharper than 9 kHz here would start cutting into the station's own sidebands.

Filters without an inductor

Most filtering is done with a resistor and a capacitor and nothing else. Wire the pair in series across the signal and take the output from one of them. Across the capacitor, whose reactance is large at low frequency and small at high, low frequencies survive and high ones are shorted away, giving a low-pass filter. Across the resistor the two roles swap, and the same components become a high-pass filter.

Neither has a sharp edge. The response slides away over a decade or more, so the agreed marker of where a filter starts to act is the cut-off frequency, the frequency at which the reactance equals the resistance and the output has fallen to 1/21/\sqrt{2}, about 0.71, of its full value. Setting 1/2πfC1/2\pi f C equal to R gives it:

fc=12πRCf_{c} = \frac{1}{2\pi RC}NOT ON THE AQA DATA SHEET: LEARN IT
Gain against frequency on a logarithmic scale for two RC filters sharing the same resistor and capacitor. The low-pass holds its output flat and then falls away past the cut-off; the high-pass does the reverse, and the two cross at about seven tenths at a cut-off near one kilohertz.
FIG. 2One 1.6 kΩ resistor and one 0.10 μF capacitor, read two ways. The low-pass and high-pass curves cross at 0.71 of full output, at a cut-off just under 1.0 kHz.

For the drawn pair fcf_{c} = 1/(2π × 1600 × 0.10 × 10−6) = 995 Hz, about a kilohertz. Speech below that passes the low-pass version almost untouched, while a 10 kHz hiss, ten times the cut-off, comes out at a tenth of its size.

INDEPENDENT PRACTICE

Killing the hum

Speech from 300 Hz upward shares a line with 50 Hz mains hum. Choose the filter, and with R = 10 kΩ find the capacitor that puts the cut-off at 150 Hz. Estimate how much of the hum survives.

Show the working

A high-pass filter, since the wanted signal lies above the interference.

C = 1/(2πfcf_{c}R) = 1/(2π × 150 × 10 × 103) = 1.1 × 10−7 F, about 0.11 μF.

At 50 Hz the frequency is a third of the cut-off, and the high-pass response there is 0.32, so about a third of the hum gets through. Speech at 300 Hz and above passes at 0.89 or better, so the wanted signal is barely touched.

ASSESSMENT FOCUS

  • Name the output terminals in a filter answer. Output across the capacitor is low-pass, across the resistor is high-pass, and the cut-off is where the output has dropped to 0.71 of full size.
  • The tuned circuit is read the same way. Across the resistor is band-pass, across the inductor and capacitor together is band-stop, and a response sketched without saying where it was measured has not answered the question.
  • Convert before dividing in fc=1/2πRCf_{c} = 1/2\pi RC. Kilohms with microfarads give the product in seconds directly, so 1.6 kΩ with 0.10 μF is 1.6 × 10−4 s and a cut-off just under a kilohertz.
  • A cut-off is not a wall. Say that the response falls away gradually and that the output at the cut-off itself is still 0.71 of full size, then estimate what survives; an answer that stops the signal dead at fcf_{c} has described a filter nobody can build.

CHECK YOURSELF

An audio line carries speech from 300 Hz upwards together with 50 Hz mains hum. A filter is to be built from a 15 kΩ resistor and one capacitor, with its cut-off at 150 Hz. (a) State which kind of filter is needed and which component the output is taken across. (b) Calculate the capacitance. (c) State the output at the cut-off frequency itself, as a fraction of the full output.

Show a hint

Which side of the cut-off does the wanted signal lie on?

Show the answer

(a) The speech lies above the hum, so the filter must keep the high frequencies: a high-pass filter, with the output taken across the resistor.

(b) C = 1/(2πfcf_{c}R) = 1/(2π × 150 × 15 × 103) = 7.1 × 10−8 F, about 71 nF.

(c) At the cut-off the reactance equals the resistance, so the output is 1/21/\sqrt{2}, about 0.71, of the full output.

The 150 Hz cut-off is chosen to sit between the two, not on either. Putting it at 50 Hz would leave the hum at 0.71 of full size, and putting it at 300 Hz would attenuate the lowest speech the line is meant to carry.

Where the output is taken decides what the filter does.

A cut-off is where the output has fallen to 0.71 of full size, not where the signal stops.

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  • Tell band-pass from band-stop and high-pass from low-pass, and find an RC filter's cut-off.
  • Say why no filter passes a single frequency, and set a passband against the width of the signal it has to carry.

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