What is analogue signal processing?
An analogue signal is a voltage that can take any value and changes smoothly, like the voltage from a microphone. Processing means changing it in a useful way: choosing some frequencies (filtering) or making it bigger (amplifying).
Two key tools: the LC resonance filter and the operational amplifier.
LC resonance filters
An inductor (coil, L) and a capacitor (C) joined together make an LC circuit. Energy moves back and forth: electric field in C → magnetic field in L → back to C. This is called oscillation.
It oscillates naturally at the resonant frequency:
f₀ = 1 / (2π√(LC))
If signals of many frequencies arrive, the circuit gives a big output only near f₀. So it works as a band-pass filter (a tuner).
Energy loss and damping
Resistance in the wire turns some energy into heat each cycle. The oscillation dies away (damping). More resistance = flatter, wider peak.
Q factor and bandwidth
The bandwidth Δf is the width of the peak where the output voltage is at least 1/√2 ≈ 0.707 of the maximum (the half-power points). The quality factor is Q = f₀ / Δf. A high Q means a sharp, narrow peak: the filter is very selective.
The ideal operational amplifier
An op-amp is a chip with two inputs: non-inverting (V₊) and inverting (V₋). Its output is
Vout = A₀ (V₊ − V₋)
where A₀ is the open-loop gain (gain with no feedback).
Properties of an ideal op-amp
- Infinite open-loop gain A₀
- Infinite input resistance (no current goes into the inputs)
- Zero output resistance (output voltage does not drop when loaded)
- Infinite bandwidth and infinite slew rate
- Output is 0 when V₊ = V₋
The op-amp as a comparator
With no feedback, even a tiny difference is multiplied hugely, so the output jumps to the positive or negative supply (it saturates). If V₊ > V₋ the output is +Vs; if V₊ < V₋ it is −Vs. This compares two voltages, for example a light sensor turning on a street lamp.
Try it: feel resonance on a swing
Push a child on a swing. Push at the swing's own rhythm and it goes higher and higher; push at a random rhythm and it hardly moves. That is resonance. In the 3D, set L = 5 and C = 5, then L = 20 and C = 20, and see f₀ drop.
Key formulas and definitions
- f₀ = 1 / (2π√(LC))
- Q = f₀ / Δf
- Vout = A₀(V₊ − V₋)
- Energy stored: E = ½CV² = ½LI²
Worked examples
1. Find f₀ for L = 10 mH and C = 10 nF.
LC = 0.010 × 10×10⁻⁹ = 1×10⁻¹⁰. √LC = 1×10⁻⁵. f₀ = 1/(2π × 10⁻⁵) ≈ 15 900 Hz ≈ 15.9 kHz.
2. A tuner has f₀ = 1.0 MHz and bandwidth 20 kHz. Find Q.
Q = f₀/Δf = 1 000 000 / 20 000 = 50.
3. You need f₀ = 1.0 kHz with C = 100 nF. What L do you need?
L = 1/(4π²f₀²C) = 1/(4π² × 10⁶ × 10⁻⁷) = 1/3.95 ≈ 0.25 H.
4. An op-amp comparator has supply ±12 V and A₀ = 10⁵. V₊ = 2.001 V, V₋ = 2.000 V. Find Vout.
A₀(V₊ − V₋) = 10⁵ × 0.001 = 100 V. That is more than 12 V, so the output saturates at +12 V.
5. If C is made 4 times bigger, what happens to f₀?
f₀ ∝ 1/√C, so f₀ becomes 1/√4 = 1/2 of the old value.
6. An op-amp has A₀ = 2×10⁵ and the output is 6 V (not saturated). What is V₊ − V₋?
V₊ − V₋ = Vout/A₀ = 6 / (2×10⁵) = 3×10⁻⁵ V = 30 μV. Almost zero, which is why we say V₊ ≈ V₋.
Common mistakes
- Forgetting the square root: f₀ = 1/(2π√LC), not 1/(2πLC).
- Not converting mH and nF to H and F before using the formula.
- Thinking high Q means wide bandwidth. High Q means narrow bandwidth.
- Thinking an op-amp comparator can give an output bigger than its supply. It can never go past ±Vs.