Analog Electronics (Electronics)

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Diodes, transistors, amplifiers, op-amps, filters.

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Analog Electronics (Electronics) — Overview

Diodes, transistors, amplifiers, op-amps, filters.

Analog Electronics — diodes, transistors, amplifiers
Notes

Analog electronics is where raw alternating current becomes the clean, amplified, stable signals that power every device from your smartphone charger to a radio receiver — and RRB JE, diploma, and GATE exams test these circuits precisely.

Definition: A diode is a two-terminal semiconductor device that allows current to flow primarily in one direction (forward bias); it acts as a one-way valve for electric current.

Definition: A transistor is a three-terminal semiconductor device used to amplify or switch electronic signals; a small input current or voltage controls a much larger output current.

Definition: An operational amplifier (op-amp) is a high-gain, differential-input voltage amplifier used as a fundamental building block for analog signal processing.

Diodes — The One-Way Gate

A p-n junction diode is formed by joining p-type and n-type semiconductors. At the junction, a depletion region forms. Under:

  • Forward bias (positive to p, negative to n): depletion region narrows, current flows freely above the threshold voltage (~0.6–0.7 V for silicon, ~0.2–0.3 V for germanium).
  • Reverse bias: depletion region widens, very little current flows until breakdown voltage is reached.

Special diodes:

Diode Key property Application
Zener diode Operates in controlled reverse breakdown at V_Z Voltage regulation
LED (Light Emitting Diode) Emits photons when forward biased Displays, indicators
Photodiode Generates reverse current proportional to light intensity Light sensors, optical communication
Schottky diode Very low forward voltage drop (~0.2 V), very fast switching High-frequency rectifiers
Varactor (Varicap) Junction capacitance varies with reverse voltage Tuning circuits

Rectifiers — AC to DC Conversion

Half-wave rectifier: one diode conducts on positive half-cycle only. Output: pulsating DC with frequency = input frequency. Efficiency ≈ 40.6%. Ripple factor = 1.21.

Full-wave rectifier (centre-tap): two diodes alternately conduct. Output frequency = 2 × input frequency. Efficiency ≈ 81.2%. Ripple factor = 0.48.

Bridge rectifier (most common): four diodes arranged in a bridge. No centre-tap transformer needed. Output frequency = 2 × input. Same efficiency as full-wave centre-tap. Ripple factor = 0.48.

Capacitor filter: a large capacitor in parallel with the load smooths pulsating DC by storing charge during peaks and releasing during troughs. The ripple voltage V_r ≈ V_m/(2fRC) for a full-wave rectifier.

Voltage regulators: 78xx series (positive: 7805 = +5 V, 7812 = +12 V); 79xx series (negative). These IC regulators maintain constant output despite load or input variation.

Real-world example: Your mobile charger contains exactly this chain — transformer steps 230 V AC down to about 12 V, bridge rectifier converts to pulsating DC, capacitor smooths it, and a regulator IC (or switching circuit) holds it at 5 V for USB charging.

Bipolar Junction Transistors (BJT)

A BJT has three terminals: Emitter (E), Base (B), Collector (C). Two types: NPN and PNP. In NPN, electrons are majority carriers; current flows Collector → Emitter when base is forward biased.

Operating regions:

  • Active region: B-E junction forward biased, B-C junction reverse biased. Used for amplification.
  • Saturation region: both junctions forward biased. Transistor is fully "ON" (like a closed switch).
  • Cutoff region: both junctions reverse biased. Transistor is fully "OFF" (like an open switch).

Current relationships:

  • I_E = I_B + I_C
  • β (hFE) = I_C / I_B (common-emitter current gain, typically 50–300)
  • α (hFB) = I_C / I_E (common-base current gain, typically 0.95–0.99)
  • Relation: β = α/(1−α) and α = β/(β+1)

:::compare BJT Configurations

Configuration Input Output Voltage gain Current gain Power gain Phase shift Use
Common Emitter (CE) Base Collector High (moderate) High Highest 180° General amplifier
Common Base (CB) Emitter Collector High < 1 Moderate HF amplifier
Common Collector (CC) / Emitter follower Base Emitter ≈ 1 High Moderate Buffer, impedance matching
:::

Common misconception: A transistor does not "create" power when it amplifies. A small base current controls a larger collector current drawn from the power supply (V_CC). The transistor is like a valve that steers energy from the supply — energy comes from V_CC, not from the input signal.

Field Effect Transistors (FET)

FETs are voltage-controlled devices (unlike BJTs which are current-controlled). Very high input impedance (MΩ to GΩ) — ideal for op-amp inputs and sensor interfaces.

  • JFET (Junction FET): gate-channel junction is reverse biased; gate voltage controls channel width.
  • MOSFET (Metal-Oxide-Semiconductor FET):
    • Depletion type: channel exists at zero gate voltage; gate can deplete or enhance it.
    • Enhancement type: no channel at zero gate bias; positive gate voltage creates channel (normally OFF).
    • MOSFETs are the building blocks of all digital ICs (billions in a single microprocessor).

Terminals: Gate (G), Drain (D), Source (S) — analogous to Base, Collector, Emitter in BJT.

Amplifiers

Amplifier gain: expressed as voltage gain Av = V_out/V_in, current gain Ai = I_out/I_in, or power gain Ap = P_out/P_in. In decibels: A_dB = 20 log(V_out/V_in).

Common-Emitter amplifier circuit: most widely used. Voltage gain Av ≈ −R_C/r_e where r_e = 26mV/I_C (small signal emitter resistance). Negative sign = 180° phase inversion.

Amplifier classes (by biasing/conduction angle):

:::compare Amplifier Classes

Class Conduction angle Efficiency Linearity Use
A 360° (full cycle) ≤ 25% Excellent Audio preamplifiers
B 180° (half cycle) ≤ 78.5% Poor (crossover distortion) Push-pull output stages
AB 180°–360° Moderate Good Practical audio amplifiers
C < 180° > 78.5% Poor RF power amplifiers
D (switching) Switches ON/OFF >90% Needs filtering Switch-mode power supplies
:::

Operational Amplifiers (Op-Amps)

An ideal op-amp has:

  • Open-loop gain A_OL = ∞ (real: 10⁵ to 10⁷)
  • Input impedance = ∞ (real: MΩ to GΩ)
  • Output impedance = 0 (real: 10–100 Ω)
  • Bandwidth = ∞ (real: limited by gain-bandwidth product)

Golden rules for ideal op-amp analysis (with negative feedback):

  1. The two input terminals are at the same voltage (virtual short: V⁺ = V⁻).
  2. No current flows into either input terminal (infinite input impedance).

Inverting amplifier: Input through R_in to inverting (−) input; R_f from output to inverting input; non-inverting (+) grounded.

Gain = −R_f / R_in (negative = 180° phase inversion)

Non-inverting amplifier: Input directly to non-inverting (+) input; voltage divider R_in and R_f from output to inverting input.

Gain = 1 + R_f / R_in (positive, in-phase)

Unity gain buffer (voltage follower): R_f = 0, R_in = ∞. Gain = 1. Used for impedance matching.

Summing amplifier (inverting): V_out = −R_f(V₁/R₁ + V₂/R₂ + ...). Used in DAC circuits.

Integrator: V_out = −(1/RC) ∫V_in dt. Capacitor replaces R_f. Used in waveform generation.

Differentiator: V_out = −RC(dV_in/dt). Capacitor replaces R_in. Used in edge detection.

Comparator: op-amp without negative feedback (open loop). Output is +V_sat or −V_sat depending on which input is larger. Schmitt trigger adds positive feedback (hysteresis), preventing noise-induced oscillation at threshold.

Filters

Filters select which frequencies pass through and which are blocked.

:::compare Filter Types

Filter Passes Blocks Key parameter
Low-pass Low frequencies (< f_c) High frequencies Cut-off frequency f_c = 1/(2πRC)
High-pass High frequencies (> f_c) Low frequencies Same formula
Band-pass Frequencies near f_0 Others Centre frequency, bandwidth
Band-stop (Notch) All except near f_0 Frequencies near f_0 Notch frequency
:::

Active filters (using op-amps) allow gain + filtering with no inductors. Sallen-Key is a common second-order active filter topology. Second-order filter: −40 dB/decade roll-off vs −20 dB/decade for first-order.

Real-world example: The noise-cancelling microphone in Indian Railways station PA systems uses a notch filter to cut the 50 Hz mains hum while passing speech frequencies (300 Hz–3.4 kHz).

Oscillators

An oscillator generates a continuous periodic signal without an external AC input — it takes DC power and converts it to AC.

Barkhausen criterion: for sustained oscillation, the loop gain must equal 1 and the total phase shift around the feedback loop must equal 0° (or 360°).

:::compare Oscillator Types

Type Frequency Stability Application
RC phase-shift Audio (up to ~1 MHz) Moderate Audio test signals
Wien bridge Audio Good Audio oscillators, function generators
Hartley LC RF Good Radio transmitters
Colpitts LC RF Good Local oscillators, RF
Crystal 1 kHz – 100 MHz Excellent (±0.001%) Clocks, frequency references
:::

Crystal oscillators use the piezoelectric resonance of a quartz crystal — the most stable frequency source at low cost.

:::keypoints Key points

  • p-n junction conducts in forward bias; Zener uses reverse breakdown for regulation.
  • BJT current gain β = I_C/I_B; three configs: CE (high gain, 180°), CB (HF), CC (buffer).
  • α = β/(β+1) and β = α/(1−α).
  • Op-amp golden rules: V⁺ = V⁻, zero input current (with negative feedback).
  • Inverting gain = −R_f/R_in; non-inverting gain = 1 + R_f/R_in.
  • Rectifier efficiency: half-wave 40.6%, full-wave/bridge 81.2%.
  • Crystal oscillators are most stable; LC oscillators (Hartley, Colpitts) for RF.
  • Barkhausen criterion: loop gain = 1, total phase shift = 0°.
    :::

:::memory
"BACE for BJT regions: Both Active, Both Cutoff, Both Emitter/Saturation": Active = BE forward, BC reverse; Cutoff = both reverse; Saturation = both forward. Op-amp gains: "Inverting MINUS, Non-inverting PLUS ONE" — Av = −Rf/Rin vs 1 + Rf/Rin.
:::

:::recap

  • Bridge rectifier: 4 diodes, output frequency = 2 × input, ripple factor = 0.48.
  • A transistor controls power from the supply — it steers, not generates, energy.
  • CE configuration inverts phase (180°); CC and CB do not.
  • Op-amp: use virtual short (V⁺ = V⁻) to analyse any negative-feedback circuit.
  • Filters: low-pass and high-pass both have f_c = 1/(2πRC).
  • Class A is most linear but least efficient; Class AB is the practical audio standard.
    :::