UGC NET · Electronic Science · Code 88 · Unit-Wise Notes

Unit 4 — Analog Circuits, Op-Amps & PLL: Complete Exam Notes

Rectifiers & filters · regulator ICs & regulated supplies · BJT/FET biasing and Q-point stability · amplifier classification · feedback · Hartley, Colpitts & phase-shift oscillators · op-amp characteristics & computational circuits · comparators & Schmitt trigger · instrumentation amplifiers · wave shaping · PLL · active filters · multivibrators · V/F & F/V converters.

SYLLABUS: NTA UGC NET (88) LEVEL: Asst. Professor / JRF FORMAT: Theory + Formulas + Revision

§ 4.1Rectifiers & Filters

A rectifier converts AC to pulsating DC. Three classic topologies — memorize the comparison table cold; it is among the most repeated numerical sources in the paper.

Half-wave vs full-wave (centre-tap) vs bridge — V_m = peak secondary voltage
ParameterHalf-waveFull-wave CTBridge
V_dcV_m/π ≈ 0.318V_m2V_m/π ≈ 0.636V_m2V_m/π
I_rmsI_m/2I_m/√2I_m/√2
Ripple factor r = √[(I_rms/I_dc)²−1]1.210.4820.482
Max efficiency η = P_dc/P_ac40.6%81.2%81.2%
PIV per diodeV_m2V_mV_m
Ripple frequencyf2f2f
Diodes (drops in path)1 (1)2 (1)4 (2)
Transformer utilization factor0.2870.6930.812
Form factor (I_rms/I_dc)1.571.111.11

Bridge wins: no centre-tap, PIV only V_m, best TUF — at the cost of two diode drops (significant for low-voltage outputs; remedy: Schottky or synchronous rectification).

Filters

  • Capacitor (peak) filter: C charges to V_m, discharges into load between peaks — sawtooth ripple.
    Capacitor-filter ripple (full-wave) $$ V_{r(pp)} = \frac{I_{dc}}{2fC}, \qquad r = \frac{1}{4\sqrt{3}fCR_L}, \qquad V_{dc} \approx V_m - \frac{V_{r(pp)}}{2} $$
    (Half-wave: replace 2f by f.) Light load → small ripple; penalty: large repetitive surge/peak diode current in narrow conduction angles.
  • Inductor filter: opposes current changes; ripple r = R_L/(3√2·ωL) — improves at heavy load (opposite of C filter).
  • LC (choke-input) filter: ripple ≈ independent of load, r = √2/(12ω²LC); critical (bleeder) inductance L_c = R_L/3ω needed for continuous conduction.
  • π (CLC) filter: best smoothing, poorer regulation; ripple ∝ 1/(C₁C₂LR_L).
UGC NET focus 1.21/0.482, 40.6/81.2%, PIV = 2V_m for centre-tap (the single most-asked rectifier fact); ripple-frequency doubling; V_r = I_dc/2fC numericals; C-filter vs L-filter load dependence contrast.

§ 4.2Voltage-Regulator ICs & Regulated Power Supply

Block chain of a linear regulated supply: transformer → rectifier → filter → regulator → load. The regulator holds V_out against input (line) and load variations.

Performance metrics $$ \text{Line regulation} = \frac{\Delta V_{out}}{\Delta V_{in}}, \qquad \text{Load regulation} = \frac{V_{NL} - V_{FL}}{V_{FL}}\times100\%, \qquad \text{Ripple rejection (dB)} = 20\log\frac{V_{r,in}}{V_{r,out}} $$
  • Zener shunt regulator (Unit-1 §1.8): simplest; poor efficiency at light load.
  • Series-pass (linear) regulator: error amplifier compares a sample of V_out (divider) with a reference (Zener/bandgap) and drives a series pass transistor — negative feedback holds V_out = V_ref(1 + R₁/R₂). Add current-limit (foldback for short-circuit safety) and a Darlington pass stage for current.
  • Three-terminal fixed ICs: 78xx (+5, +6, +9, +12, +15, +24 V) and 79xx (negative); need V_in ≥ V_out + ~2 V dropout; internal thermal shutdown and current limit; bypass capacitors at both pins for stability. LDOs reduce dropout to ~0.1–0.5 V.
  • LM317 adjustable: maintains 1.25 V between OUT and ADJ:
    LM317 output $$ V_{out} = 1.25\left(1 + \frac{R_2}{R_1}\right) + I_{ADJ}R_2 \quad (I_{ADJ} \approx 50\ \mu A,\ \text{usually negligible}) $$
  • IC 723: the classic building-block regulator — internal 7.15 V reference, error amp, pass transistor (150 mA, externally boostable), and current-limit sense; configurable as low-V (2–7) or high-V (7–37) regulator; basis of many lab supplies.
  • SMPS vs linear (detail in Unit-IX): linear — quiet, simple, efficiency ≈ V_out/V_in (often 30–50%); switching — 70–95% efficient, small magnetics at high f_sw, but switching noise/EMI.
UGC NET focus LM317 formula numericals; 78xx pinout/dropout (~2 V); load-regulation percentage computation; 723's 7.15 V reference; series regulator = negative-feedback error loop; foldback limiting purpose.

§ 4.3BJT Biasing, Operating Point & Stability

Biasing fixes the quiescent point Q(I_CQ, V_CEQ) on the DC load line \( V_{CE} = V_{CC} - I_C(R_C + R_E) \) so the signal swings linearly — for max symmetric swing place Q mid-line (V_CEQ ≈ V_CC/2). The Q-point drifts with temperature through three culprits: I_CO doubles every 10 °C, V_BE drops ~2.5 mV/°C, and β rises with T (and spreads unit-to-unit).

Stability factors $$ S = \frac{\partial I_C}{\partial I_{CO}}, \qquad S' = \frac{\partial I_C}{\partial V_{BE}}, \qquad S'' = \frac{\partial I_C}{\partial \beta}; \qquad \text{general: } S = \frac{1+\beta}{1 + \beta\,\dfrac{R_E}{R_E + R_B}} $$
Bias circuits ranked
CircuitStability factor SVerdict
Fixed bias (R_B to V_CC)S = 1 + β (worst, ~101)β-dependent; never used alone
Collector-to-base feedbackS = (1+β)/(1 + βR_C/(R_C+R_B))moderate; negative feedback via R_B
Voltage-divider + R_E (self bias)S = (1+β)(1+R_B/R_E)/(1+β+R_B/R_E) → ≈ 1 + R_B/R_Ebest practical; design standard
Emitter bias (dual supply)≈ 1 for R_B ≪ βR_Eexcellent
  • Voltage-divider design: Thevenin V_B = V_CC·R₂/(R₁+R₂), R_B = R₁∥R₂; \( I_C \approx \dfrac{V_B - V_{BE}}{R_E + R_B/\beta} \) — β-insensitive when R_B ≪ βR_E (rule: R_B ≤ 0.1βR_E) and V_E ≈ 1–2 V. Ideal S → 1; S ranges 1 … 1+β.
  • R_E = DC negative feedback: I_C rises → V_E rises → V_BE falls → I_C pulled back. Bypass capacitor C_E restores AC gain while keeping DC stability.
  • Thermal runaway: I_C↑ → junction power ↑ → T_J↑ → I_CO/β↑ → I_C↑… Avoided when \( \partial P_C/\partial T_J < 1/\theta_{JA} \); inherently safer when V_CE < V_CC/2. Heat sinks lower θ.
  • Compensation techniques: diode in the base divider tracks V_BE(T); thermistor/sensistor adjusts bias; matched-pair (current-mirror) bias in ICs.
UGC NET focus S = 1 + β for fixed bias; compute Q-point for divider bias; why R_E stabilizes and C_E bypasses; thermal-runaway condition; mid-point biasing for maximum swing; I_CO doubling/V_BE −2.5 mV/°C numbers.

§ 4.4FET Biasing

  • JFET / depletion MOSFET (needs V_GS < 0 for n-channel):
    • Fixed (gate) bias: negative supply through R_G — poor, parameter-sensitive.
    • Self bias: source resistor; I_D through R_S makes \( V_{GS} = -I_D R_S \); solve with the square law \( I_D = I_{DSS}(1 - V_{GS}/V_P)^2 \) graphically (bias line through origin, slope −1/R_S) or algebraically. Self-correcting: I_D↑ → V_GS more negative → I_D↓.
    • Voltage-divider bias: \( V_{GS} = V_G - I_DR_S \) with V_G = V_DD·R₂/(R₁+R₂) — flattest bias line, least sensitivity to device spread (best).
    • Current-source bias: a BJT/JFET current source in the source lead pins I_D exactly.
  • Enhancement MOSFET (needs V_GS > V_T): drain-to-gate feedback bias (R_F from drain; since I_G = 0, V_GS = V_DS — guarantees saturation) or voltage-divider bias; use \( I_D = K(V_{GS} - V_T)^2 \).
  • Gate current ≈ 0 in all FETs → huge R_G permissible (MΩ) without bias shift — the input-impedance advantage.
  • Q-point checks: confirm \( V_{DS} > V_{GS} - V_P \) (JFET) or \( > V_{GS} - V_T \) (MOS) for saturation-region operation.
UGC NET focus Self-bias quadratic numericals (find I_D, V_GS given I_DSS, V_P, R_S); why divider bias beats self bias (bias-line geometry); drain-feedback bias forces saturation; V_GS polarity rules per device type.

§ 4.5BJT Amplifiers: CE, CB, CC

Small-signal models: h-parameter (h_ie, h_re, h_fe, h_oe — Unit-3 two-port heritage) or hybrid-π with \( g_m = I_C/V_T \) (≈ 40·I_C at room T), \( r_\pi = \beta/g_m = h_{ie} \), \( r_e = V_T/I_E \approx 26/I_{E(mA)}\ \Omega \).

The three configurations (typical, R_E bypassed where applicable)
PropertyCommon EmitterCommon BaseCommon Collector (EF)
Voltage gainHigh, \( A_v = -g_mR_C' \) (inverting)High, +g_mR_C′ (non-inv.)≈ 1 (slightly <1, non-inv.)
Current gainHigh (β)≈ 1 (α)High (1+β)
Power gainHighestModerateModerate
R_inModerate (r_π ≈ kΩ)Low (r_e ≈ Ω–tens Ω)High (r_π + (1+β)R_E′)
R_outModerate–high (≈ R_C)HighLow (≈ r_e + R_s/(1+β))
Phase shift180°
Frequency behaviourMiller-limitedBest HF (no Miller)Wide
UseGeneral gain stageHF/RF, cascode upper device, current bufferBuffer / level shifter / output stage
  • Unbypassed R_E (swamping): \( A_v \approx -R_C/(r_e + R_E) \) — gain stabilized against r_e (temperature/bias) at the price of magnitude; R_in rises to r_π + (1+β)R_E.
  • Emitter follower impedance transformation: looking into the base, emitter impedances appear ×(1+β); looking into the emitter, base-side impedances ÷(1+β) — the universal buffering identity.
  • Cascode (CE + CB): CE gain into the low input impedance of CB kills the Miller effect → wide bandwidth with high gain; standard in RF and op-amp internals.
  • Darlington pair: composite β ≈ β₁β₂, very high R_in, two V_BE drops, slower.
UGC NET focus Configuration-property matching (CE inverts; CB lowest R_in/best HF; CC buffer); r_e = 26/I_E numericals; gain −R_C/(r_e+R_E) with swamping; cascode = CE+CB beats Miller; Darlington β-product.

§ 4.6FET Amplifiers: CS, CG, CD

FET configurations (g_m from Unit-1 §1.11–1.12)
PropertyCommon SourceCommon GateCommon Drain (SF)
Voltage gain\( -g_m(R_D \| r_d) \), inverting+g_mR_D′, non-inv.\( \dfrac{g_mR_S'}{1+g_mR_S'} \) < 1
R_in≈ R_G (very high)Low ≈ 1/g_mVery high
R_out≈ R_D≈ R_D≈ 1/g_m (low)
Rolegain stage (FET's CE)RF / cascode (FET's CB)buffer (FET's CC)
  • Unbypassed R_S: \( A_v = \dfrac{-g_mR_D}{1 + g_mR_S} \) — source degeneration, same stabilization logic as the BJT's R_E.
  • FET vs BJT amplifier: FET gives higher R_in, lower noise, but lower g_m at equal current (g_m(BJT) = I_C/V_T beats g_m(FET) = 2I_D/(V_GS−V_T)) → less gain per stage.
  • MOSFET versions identical in form; CMOS active-load stages (current-mirror load) achieve \(A_v = -g_m(r_{o,n}\|r_{o,p})\) — the IC gain cell.
UGC NET focus A_v = −g_mR_D plug-ins; source-follower output resistance 1/g_m; degenerated-gain formula; why BJT out-gains FET at the same bias current.

§ 4.7Classification of Amplifiers & Power Classes

Classification axes

  • By signal size: small-signal (linear models valid) vs large-signal (power).
  • By frequency: DC/audio (20 Hz–20 kHz) / video (wideband) / RF tuned (narrowband).
  • By coupling: RC-coupled (cheap, flat mid-band, blocks DC), transformer-coupled (impedance matching, efficient power transfer, bulky, poor response), direct-coupled (amplifies DC, drift problem — op-amp internals).
  • By quantity amplified: voltage/current/transconductance/transresistance — pairs with the four feedback topologies (§4.9).

Power-amplifier classes (conduction angle)

Class comparison — efficiency values are the most-asked numbers
ClassConduction angleMax efficiencyDistortionUse
A360°25% (resistive load) / 50% (transformer-coupled)Lowestsmall-signal, hi-fi driver
B180°78.5% (π/4)Crossoverpush-pull output
AB180°–360°50–78.5%Low (bias kills crossover)standard audio output
C< 180°> 78.5% (→ ~90%+)Severe — needs tankRF tuned amps, freq. multipliers
Dswitching (PWM)90–98% (ideal 100%)Switching artifacts → LC filtermodern audio, motor drive
  • Class A: Q mid-line, device always on; dissipation maximum at zero signal — P_D(max) = 2P_o(max) for transformer-coupled.
  • Class B push-pull: complementary (NPN+PNP) or transformer-phase-split pair, each handles a half cycle; crossover distortion near zero (both off for |v_in| < V_BE). Even harmonics cancel in ideal push-pull.
  • Class AB: slight forward bias (diode/V_BE-multiplier) removes crossover; thermal tracking via the bias diodes mounted on the heat sink.
  • Class C: narrow current pulses re-shaped to a sine by a resonant tank; efficiency rises as conduction angle shrinks (at falling output power).
  • Figures of merit: efficiency η = P_ac/P_dc, collector dissipation, harmonic distortion \( THD = \sqrt{D_2^2 + D_3^2 + \cdots} \), power-output capability.
UGC NET focus 25/50/78.5% set; crossover distortion cause and the AB cure; class-C for RF with tank; even-harmonic cancellation in push-pull; conduction-angle classification.

§ 4.8Frequency Response of Amplifiers

  • Mid-band gain flat; low-frequency roll-off from coupling and bypass capacitors (each forms a high-pass with its seen resistance, f_L = 1/2πRC; the largest individual f_L dominates); high-frequency roll-off from device/stray shunt capacitances (C_π, C_µ, C_wiring).
  • Miller effect: feedback capacitance across an inverting gain A appears at the input multiplied:
    Miller capacitance $$ C_{in(Miller)} = C_f(1 + |A|), \qquad C_{out(Miller)} = C_f\left(1 + \tfrac{1}{|A|}\right) \approx C_f $$
    — dominant HF limit of CE/CS stages; defeated by cascode (CB/CG sees no Miller) or by the CC/CD buffer.
  • BJT HF figures: \( f_\beta \) (β falls 3 dB), \( f_T = \beta f_\beta = g_m/2\pi(C_\pi + C_\mu) \) — gain–bandwidth of the device.
  • Multistage: overall gain multiplies (dB add); bandwidth shrinks:
    n identical stages $$ f_{H(n)} = f_H\sqrt{2^{1/n} - 1}, \qquad f_{L(n)} = \frac{f_L}{\sqrt{2^{1/n}-1}} \quad (n = 2: \times 0.644) $$
  • Gain–bandwidth conservation: in a single-pole stage, trading gain (e.g., by feedback) buys bandwidth — see §4.9, §4.11.
  • Square-wave testing: LF tilt/sag ↔ f_L; rounded edges ↔ f_H (t_r ≈ 0.35/f_H, Unit-3).
UGC NET focus Miller-capacitance numericals; bandwidth-shrinkage factor √(2^{1/n}−1); f_T = βf_β; which capacitor sets which end of the response; sag/rise-time diagnostics.

§ 4.9Concept of Feedback

Closed-loop gain (negative feedback) $$ A_f = \frac{A}{1 + A\beta}, \qquad \text{loop gain } = A\beta, \qquad \text{desensitivity } D = 1 + A\beta; \qquad A\beta \gg 1 \Rightarrow A_f \approx \frac{1}{\beta} $$

What negative feedback buys (all by the factor 1 + Aβ)

  • Gain stability: \( \dfrac{dA_f}{A_f} = \dfrac{1}{1+A\beta}\,\dfrac{dA}{A} \) — gain set by passive β network.
  • Bandwidth extension: \( f_{H,f} = f_H(1+A\beta) \), \( f_{L,f} = f_L/(1+A\beta) \); gain×bandwidth constant.
  • Distortion & noise (inside the loop) reduced ÷(1+Aβ); input-referred noise of the first stage is not improved.
  • Impedances re-shaped per topology (below) — the design lever.
  • Cost: gain ÷(1+Aβ); risk: instability if phase reaches 180° while |Aβ| ≥ 1 (gain/phase margins, Unit-3 §3.12).
The four topologies — sampling–mixing names (memorize the impedance arrows)
Topology (sampling–mixing)Amplifier type stabilizedR_inR_outExample
Voltage-series (shunt-derived, series-fed)Voltage amp (A_v)↑ ×(1+Aβ)↓ ÷(1+Aβ)non-inverting op-amp, emitter follower
Voltage-shuntTransresistance (R_m)inverting op-amp, collector-base feedback
Current-seriesTransconductance (G_m)CE with unbypassed R_E
Current-shuntCurrent amp (A_i)two-stage I-feedback pair

Memory rule: series mixing raises R_in, shunt mixing lowers it; voltage sampling lowers R_out, current sampling raises it.

Positive feedback (loop phase 0°): |Aβ| < 1 → regenerative gain boost (historic); |Aβ| = 1 → oscillation (§4.10); |Aβ| > 1 → latching (Schmitt trigger §4.13).

UGC NET focus Identify topology from a circuit and state the impedance changes; A_f, bandwidth, distortion numericals with (1+Aβ); A_f ≈ 1/β for large loop gain; sensitivity computation.

§ 4.10Oscillators: Phase-Shift, Wien, Hartley, Colpitts, Crystal

Barkhausen criterion Sustained oscillation ⟺ loop gain |Aβ| = 1 and loop phase = 0° (2nπ) at one frequency. Start-up needs |Aβ| slightly > 1 (noise grows, amplitude limited by nonlinearity/AGC).

RC oscillators (audio range)

  • RC phase-shift: inverting amplifier (180°) + three RC sections contributing the other 180° (60° each at f₀).
    Phase-shift oscillator $$ f_0 = \frac{1}{2\pi RC\sqrt{6}}, \qquad |A| \ge 29 \ (\text{the RC ladder attenuates } 1/29) $$
    (FET version as stated; BJT loading modifies to \( f_0 = \tfrac{1}{2\pi RC\sqrt{6 + 4R_C/R}} \), h_fe(min) ≈ 44.5 for R_C = R.)
  • Wien bridge: non-inverting amp (0°) + lead-lag network (0° at f₀, β = 1/3).
    Wien bridge $$ f_0 = \frac{1}{2\pi RC}, \qquad A \ge 3 \ \Rightarrow\ R_f = 2R_1 $$
    Amplitude stabilization: lamp/thermistor or diode-limited R_f. The standard lab audio oscillator (tunable, low distortion).

LC oscillators (RF) — the general three-reactance form

Amplifier with reactances X₁ (input side), X₂ (output side), X₃ (feedback): oscillation needs X₁ + X₂ + X₃ = 0 with X₁, X₂ alike and X₃ opposite.

  • Hartley ("H = henry → two inductors"): tapped L (L₁, L₂, mutual M) + one C.
    Hartley $$ f_0 = \frac{1}{2\pi\sqrt{(L_1 + L_2 + 2M)\,C}}, \qquad |A|_{min} = \frac{L_1}{L_2}\ (\text{feedback ratio } \beta = L_2/L_1) $$
  • Colpitts ("C → two capacitors"): tapped C (C₁, C₂) + one L.
    Colpitts $$ f_0 = \frac{1}{2\pi\sqrt{L\,C_{eq}}}, \quad C_{eq} = \frac{C_1C_2}{C_1+C_2}, \qquad |A|_{min} = \frac{C_2}{C_1} $$
    Preferred at HF (capacitive divider absorbs device capacitances); Clapp adds a small series C₃ ≪ C₁,C₂ that dominates f₀ → frequency nearly independent of transistor capacitance (better stability).

Crystal oscillators

  • Quartz piezoelectric resonator ≡ series R-L-C (motional) ∥ parallel C₀ (holder). Two resonances: series \( f_s = \tfrac{1}{2\pi\sqrt{LC}} \) and parallel/antiresonant \( f_p = f_s\sqrt{1 + C/C_0} \) slightly above; crystal operates inductive between f_s and f_p (replaces L in a Colpitts → Pierce configuration).
  • Extraordinary Q ~ 10⁴–10⁶ → frequency stability ~ppm (TCXO/OCXO to ppb); clocks, µP timing, carrier generation. Overtone operation for > ~30 MHz.
UGC NET focus f₀ formulas with the √6 (phase-shift) and gain minima 29 / 3 / C₂/C₁ / L₁/L₂; identify Hartley vs Colpitts from the tank; crystal inductive-window operation and huge Q; Barkhausen statement; Wien needs A = 3 exactly.

§ 4.11Op-Amp Characteristics

A direct-coupled, very-high-gain differential amplifier: diff input pair → gain stage(s) with internal compensation capacitor → class-AB output buffer. Output \( V_o = A_{OL}(V_+ - V_-) \).

Ideal vs practical (741 values — quote these)
ParameterIdealµA741 typical
Open-loop gain A_OL2×10⁵ (106 dB)
Input resistance2 MΩ
Output resistance075 Ω
Bandwidthunity-gain f_T ≈ 1 MHz (A_OL to ~10 Hz)
CMRR90 dB
Slew rate0.5 V/µs
Input offset voltage01–6 mV
Input bias / offset current080 nA / 20 nA
  • Golden rules (negative feedback active): (1) no current into the inputs; (2) V₊ = V₋ — the inverting input of an inverting amp sits at virtual ground.
  • CMRR = A_d/A_cm (dB: 20 log) — rejection of signals common to both inputs (hum, sensor common-mode).
  • Gain–bandwidth product: single-pole compensated op-amp: \( A_{CL} \times f_{3dB} = f_T \) (e.g., gain 100 → 10 kHz BW on a 741).
  • Slew rate \( SR = \max|dV_o/dt| = I_{tail}/C_{comp} \); large-signal limit. Maximum undistorted sine ("full-power bandwidth"):
    Slew-rate limit $$ f_{max} = \frac{SR}{2\pi V_{peak}} $$
    Small signals are bandwidth-limited; large signals slew-limited (triangular distortion).
  • Offsets: V_io and I_B drive output errors ×(1 + R_f/R₁); bias-current compensation resistor \( R_{comp} = R_1 \| R_f \) at V₊; nulling pins on the 741.
  • PSRR, output swing within rails (rail-to-rail types), input common-mode range, latch-up free modern devices.
UGC NET focus Slew-rate numericals f_max = SR/2πV_p; GBW trade-off computations; virtual-ground reasoning; CMRR in dB; offset-voltage output error ×noise gain; 741 catalogue numbers.

§ 4.12Op-Amp Computational Applications

The canonical linear circuits
CircuitOutputNotes
Inverting\( V_o = -\dfrac{R_f}{R_1}V_{in} \)R_in = R₁; virtual ground; noise gain 1 + R_f/R₁
Non-inverting\( V_o = \left(1 + \dfrac{R_f}{R_1}\right)V_{in} \)R_in huge; gain ≥ 1
Voltage followerV_o = V_inbuffer; max feedback → max BW, watch stability/capacitive loads
Summing (inverting)\( V_o = -R_f\left(\dfrac{V_1}{R_1} + \dfrac{V_2}{R_2} + \cdots\right) \)audio mixer, weighted DAC
Difference\( V_o = \dfrac{R_2}{R_1}(V_2 - V_1) \) (matched ratios)CMRR limited by resistor matching → §4.14
Integrator\( V_o = -\dfrac{1}{RC}\displaystyle\int V_{in}\,dt \)−20 dB/dec; add R_f∥C to tame DC drift (practical/lossy)
Differentiator\( V_o = -RC\,\dfrac{dV_{in}}{dt} \)+20 dB/dec → noisy/unstable; add series R_in to roll off
Log amp\( V_o = -\eta V_T\ln\dfrac{V_{in}}{I_sR} \)diode/BJT in feedback; T-sensitive
Antilog amp\( V_o = -I_sR\,e^{V_{in}/\eta V_T} \)log+antilog → analog multiply/divide
V→I converter\( I_L = V_{in}/R \) (load-independent)floating or Howland (grounded load)
I→V converter\( V_o = -I_{in}R_f \)transimpedance: photodiode readout
  • Integrator + summer + inverter = analog computer solving ODEs (the "computational" in the syllabus); integrator also generates triangles from squares (§4.17) and is the core of dual-slope ADCs.
  • Frequency view: integrator |H| = 1/ωRC (unity at ω = 1/RC); differentiator |H| = ωRC.
UGC NET focus Gain-formula plug-ins (watch the +1 in non-inverting); integrator output for square/step inputs (ramps!); summing-amp weighted outputs; transimpedance for photodiodes; why the pure differentiator is impractical.

§ 4.13Comparators & Schmitt Trigger

Comparator

  • Op-amp open-loop (or dedicated IC — LM311/LM339: faster, open-collector, no compensation): \( V_o = +V_{sat} \) if V₊ > V₋ else −V_sat. Zero-crossing detector (reference = 0) and level detector (reference = V_R).
  • Weakness: noise near the threshold causes multiple output chatter; slow inputs dwell in the linear region. Cure: hysteresis.

Schmitt trigger (regenerative comparator)

Positive feedback to V₊ creates two thresholds — a bistable transfer characteristic with a hysteresis loop.

Inverting Schmitt thresholds (divider R₁ to ground, R₂ to output) $$ V_{UT} = +\beta V_{sat}, \quad V_{LT} = -\beta V_{sat}, \quad \beta = \frac{R_1}{R_1 + R_2}; \qquad V_H = V_{UT} - V_{LT} = 2\beta V_{sat} $$
  • Input must cross V_UT to switch one way and fall below V_LT to switch back — noise smaller than V_H cannot retrigger. Reference offset shifts the loop center.
  • Applications: squaring any waveform, noise-immune level detection, switch debouncing, ON–OFF (bang-bang) control with deadband, relaxation oscillator core (§4.17), wave regeneration in digital receivers (74HC14 hex Schmitt inverter).
  • Speed: output transitions at slew rate regardless of input speed — regenerative snap.
UGC NET focus UTP/LTP numericals from the divider; hysteresis width 2βV_sat; why hysteresis defeats noise (draw the loop); comparator IC vs op-amp differences; identify inverting vs non-inverting Schmitt from feedback node.

§ 4.14Instrumentation Amplifiers

Precision differential amplifier for low-level transducer signals (strain gauges, thermocouples, biopotentials) riding on large common-mode voltages. Requirements: very high R_in on both inputs, high CMRR, precise gain set by one resistor, low drift.

Three op-amp architecture

Stage 1: two non-inverting buffers sharing gain resistor R_G (their inverting inputs joined through it). Stage 2: unity (or fixed-gain) difference amplifier.

In-amp gain $$ V_o = \left(1 + \frac{2R}{R_G}\right)\frac{R_3}{R_2}\,(V_2 - V_1) \qquad \big(\text{commonly } R_3 = R_2:\ A = 1 + 2R/R_G\big) $$
  • Why it wins: input stage gives differential gain but unity common-mode gain (common-mode passes un-amplified to the matched difference stage) → CMRR multiplies; both inputs see op-amp R_in directly; single-resistor (R_G) gain programming without disturbing matching.
  • Monolithic in-amps (AD620, INA128): laser-trimmed internal resistors, CMRR 100–120 dB, gain 1–1000 via external R_G.
  • Bridge measurement: in-amp across a Wheatstone bridge senses mV-level imbalance \( V_d \approx V_{ex}\,\Delta R/4R \); guard drives and shield techniques preserve CMRR at the cable.
  • Difference-amp alone fails: R_in unequal/low, CMRR collapses with 0.1% resistor mismatch (CMRR ≈ (1+R₂/R₁)/4ε).
UGC NET focus Gain formula 1 + 2R/R_G numericals; why CMRR is high (CM gain of stage 1 = 1); single-resistor gain set; in-amp vs plain difference amplifier; bridge + in-amp as the standard sensor front end.

§ 4.15Wave-Shaping Circuits

Clippers (limiters) — remove part of a waveform

  • Series (diode in signal path) or shunt (diode across output); positive/negative/biased variants — clipping level = V_R ± 0.7 V; combination (two biased diodes) → slicer/amplitude limiter (e.g., ±V_Z ± 0.7 with back-to-back Zeners).
  • Applications: protection, FM amplitude limiting, generating trapezoids/squares from sines.

Clampers (DC restorers) — shift the whole waveform

  • C + diode (+ R): diode pins one peak near 0 (or V_R), capacitor stores the required DC; output swings entirely above (positive clamper) or below (negative clamper) the clamp level. Peak-to-peak is preserved; need RC ≫ T.
  • Memory rule: output ≈ input + V_C; diode direction decides the sign. Application: video DC restoration, voltage doubler front ends.

RC shaping & precision circuits

  • RC differentiator (RC ≪ T): square → spikes (edge detector); RC integrator (RC ≫ T): square → triangle-ish ramps (cf. §3.13 regimes).
  • Precision (super) diode / precision rectifiers: diode inside an op-amp loop divides V_γ by A_OL → rectifies mV signals; half-wave and full-wave (absolute-value) versions; peak detector = precision diode + hold capacitor (+ buffer); sample-and-hold as its switched cousin.
  • Voltage multipliers (half/full-wave doubler, Cockcroft–Walton ladder) — clamp + peak-rectifier cascades.
UGC NET focus Sketch-the-output questions for given clipper/clamper with bias V_R (track the 0.7 V); clamper preserves p-p value; RC ≪ T vs ≫ T shaping outcomes; why precision rectifier beats a bare diode for small signals.

§ 4.16Active Filters

Op-amp + RC networks replace inductors: gain possible, near-ideal cascading (low Z_out), tunable — limited by op-amp GBW. (Passive/image filters: Unit-3 §3.13.)

  • First-order LP: \( H = \dfrac{A_0}{1 + j f/f_c} \), \( f_c = \dfrac{1}{2\pi RC} \), −20 dB/dec; HP is the RC-swapped mirror.
  • Second-order Sallen–Key (VCVS) LP: two RC + non-inverting gain A₀ = 1 + R_f/R₁:
    Sallen–Key equal-component design $$ f_c = \frac{1}{2\pi RC}, \qquad Q = \frac{1}{3 - A_0} \;\Rightarrow\; \textbf{Butterworth (Q = 0.707): } A_0 = 1.586,\ \ A_0 \ge 3 \Rightarrow \text{oscillation} $$
  • −40 dB/dec per second-order section; cascade sections (with tabulated Q's) for higher order: overall slope −20n dB/dec.
  • Band-pass: multiple-feedback (MFB) single-op-amp for Q ≲ 10: f₀, BW = f₀/Q; narrowband Q > 10 conventions; band-reject: twin-T with bootstrap, or LP + HP summed (wideband notch); 50 Hz hum notch is the standard example.
  • State-variable (universal) filter: two integrators + summer give simultaneous LP/BP/HP outputs, independent f₀ and Q tuning; add a summer for notch/all-pass. All-pass: flat magnitude, phase shifter/delay equalizer.
  • Response families recap (match-the-property): Butterworth — maximally flat; Chebyshev — equiripple, steeper; Elliptic — steepest; Bessel — linear phase/constant delay.
  • Op-amp limits: f_c·gain ≪ GBW; slew rate caps large-signal output (f_max = SR/2πV_p); switched-capacitor filters (MF10) emulate R = 1/f_clkC for clock-tunable f_c.
UGC NET focus Sallen–Key Q = 1/(3−A₀) and the 1.586 Butterworth gain; order ↔ slope arithmetic; state-variable simultaneous outputs; family-property matching; notch for 50 Hz interference.

§ 4.17Multivibrators & the 555 Timer

The three multivibrators
TypeStable statesFunctionRealizations
Astable0 (free-running)square-wave clockop-amp relaxation, 555, CMOS gate RC, emitter-coupled pair
Monostable1 (one-shot)fixed-width pulse per trigger555, 74121/123
Bistable2 (flip-flop)storage / Schmittcross-coupled pair, latch

Op-amp astable (Schmitt + RC)

Op-amp relaxation oscillator $$ T = 2RC\ln\!\frac{1+\beta}{1-\beta} \;\xrightarrow{\ \beta = 1/2\ (R_1 = R_2)\ }\; T = 2RC\ln 3 \approx 2.2RC $$

Triangular-wave generator: Schmitt trigger + integrator loop — triangle at the integrator, square at the Schmitt; \( f = \dfrac{R_2}{4R_1RC} \) for the standard pair.

555 timer (the exam favourite)

Internals: three 5 kΩ divider (thresholds 2V_CC/3 and V_CC/3), two comparators, SR flip-flop, discharge transistor, output buffer. Pins: 1 GND, 2 Trigger, 3 Out, 4 Reset, 5 Control (bypass 0.01 µF), 6 Threshold, 7 Discharge, 8 V_CC.

555 design equations $$ \textbf{Monostable: } T = 1.1\,RC $$ $$ \textbf{Astable: } T_{H} = 0.693(R_A + R_B)C,\quad T_L = 0.693R_BC,\quad f = \frac{1.44}{(R_A + 2R_B)C},\quad D = \frac{R_A + R_B}{R_A + 2R_B} > 50\% $$
  • Duty cycle always > 50% in the basic astable (charge through R_A+R_B, discharge through R_B); 50% via diode across R_B or R_A ≪ R_B tricks.
  • Control pin (5) varies the 2V_CC/3 threshold → VCO / pulse-position modulation; timing independent of V_CC (ratiometric thresholds).
  • Applications: timers, clocks, PWM, missing-pulse detector, frequency divider, touch switch.
UGC NET focus 1.1RC and 1.44/(R_A+2R_B)C are guaranteed numericals; 2V_CC/3–V_CC/3 thresholds; duty-cycle > 50% reasoning; op-amp astable 2.2RC; triangle generator block pairing.

§ 4.18Phase-Locked Loops (PLL)

Negative-feedback loop locking a local oscillator to an input's phase/frequency. Blocks: phase detector (PD)loop (low-pass) filter → error voltage → VCO; VCO output feeds back to the PD.

  • Operation: free-running (unlocked) → capture (pull-in toward f_in) → lock (f_VCO = f_in exactly; residual phase error supplies the control voltage). In lock, frequency error = 0.
  • Key ranges $$ \textbf{Lock range } \Delta f_L \;>\; \textbf{Capture range } \Delta f_C; \qquad \Delta f_C \approx \sqrt{\frac{\Delta f_L}{2\pi\,\tau_{filter}}}\ \ (\text{narrower filter} \Rightarrow \text{smaller capture}) $$
    Lock range set by PD/VCO gains \(K_\phi K_v\); capture additionally throttled by the loop filter — the classic conceptual MCQ.
  • Components: PD types — analog multiplier (K_φ sin φ_e), XOR (digital, 90° quiescent), phase-frequency detector + charge pump (infinite pull-in, no false lock); VCO conversion gain K_v (Hz/V); loop order/type sets tracking of steps/ramps.
  • IC 565: classic analog PLL — free-running \( f_o \approx \dfrac{1.2}{4R_TC_T} \), lock range \( \Delta f_L = \pm\dfrac{8f_o}{V_{CC,total}} \), capture \( \Delta f_C = \pm\sqrt{\dfrac{\Delta f_L}{2\pi(3.6\times10^3)C}} \). CMOS 4046 for digital work.
  • Applications (each is a one-line exam answer):
    • FM demodulation: VCO control voltage is the message.
    • FSK decoding (modems), AM synchronous detection (PLL regenerates the carrier).
    • Frequency synthesis: ÷N counter in the feedback → f_out = N·f_ref; programmable channel spacing = f_ref.
    • Frequency multiplication/translation, clock recovery from data, motor-speed control, carrier tracking in receivers.
UGC NET focus Block diagram order; lock > capture and which element controls which; in-lock error is phase, not frequency; ÷N synthesis arithmetic f_out = Nf_ref; FM demod = read the VCO input; 565 f_o formula.

§ 4.19V/F & F/V Converters

Voltage-to-Frequency (V/F)

  • Output frequency ∝ input voltage — a linear VCO. Architectures:
    • Integrator + comparator (multivibrator type): input current charges C to a threshold, reset, repeat → f = V_in/(V_ref·RC)-type linearity.
    • Charge-balance (the precision standard, LM331/VFC32): each output pulse removes a fixed charge packet Q = I_ref·t; balance forces \( f = \dfrac{V_{in}}{R\,Q} \) — linearity ~0.01%, wide dynamic range.
  • IC 566 (function-generator VCO): \( f_o = \dfrac{2(V_{CC} - V_C)}{R_TC_TV_{CC}} \) — simultaneous square + triangle outputs; control via pin 5 (pairs with the 565 PLL).
  • Applications: cheap high-resolution ADC (count pulses over a gate time — inherent integration averages noise), telemetry over a single line / optocoupler (frequency is noise-immune and isolation-friendly), light/temperature transmitters, integrating DVMs.

Frequency-to-Voltage (F/V)

  • Inverse function: input conditioned (Schmitt) → fixed-width, fixed-height pulse per cycle (monostable/charge pump) → averaging low-pass → \( V_o = k\,f_{in} \) (e.g., LM331 reversed, LM2907 with built-in comparator + charge pump).
  • Design trade-off: larger filter C → less ripple but slower response (ripple ∝ 1/f_inRC).
  • Applications: tachometer (speed from encoder/ignition pulses), FSK/FM demodulation, frequency meters, motor-speed feedback for control loops, RPM gauges.
  • A V/F at the sender and F/V at the receiver = robust analog telemetry link; both functions are also subsumed by a PLL (VCO = V/F; PD+filter = F/V).
UGC NET focus Charge-balance principle (fixed charge per pulse → linearity); V/F-based ADC by pulse counting; LM331/566/2907 role recognition; tachometer = F/V; ripple-vs-response filter trade-off.

§ 4.20Unit-4 Formula Sheet

One-stop formula table — Unit 4
TopicFormulaNotes
Rectifier DC valuesHW: V_m/π; FW: 2V_m/πripple 1.21 / 0.482
EfficiencyHW 40.6%; FW/bridge 81.2%PIV: CT = 2V_m, bridge = V_m
C-filter ripple\( V_{r(pp)} = I_{dc}/2fC;\ r = 1/4\sqrt3 fCR_L \)FW; HW: drop the 2
LC filter\( r = \sqrt2/12\omega^2LC;\ L_c = R_L/3\omega \)load-independent ripple
Load regulation(V_NL − V_FL)/V_FL × 100%
LM317\( V_o = 1.25(1 + R_2/R_1) \)+I_ADJ·R₂ correction
Stability factor\( S = \dfrac{1+\beta}{1+\beta R_E/(R_E+R_B)} \)fixed bias: 1+β; ideal → 1
Divider-bias I_C\( (V_B - V_{BE})/(R_E + R_B/\beta) \)R_B ≤ 0.1βR_E rule
JFET self-bias\( V_{GS} = -I_DR_S \) with square lawsolve quadratic
BJT small-signal\( g_m = I_C/V_T;\ r_e = 26/I_{E(mA)}\,\Omega \)r_π = β/g_m
CE gain\( A_v = -R_C'/(r_e + R_E) \)bypassed: −R_C′/r_e
Emitter followerR_in(base) = r_π + (1+β)R_ER_out ≈ r_e + R_s/(1+β)
Class efficienciesA: 25/50%; B: 78.5%; C > 78.5%conduction angle order
Miller\( C_{in} = C_f(1+|A|) \)cascode defeats it
n-stage bandwidth\( f_{H(n)} = f_H\sqrt{2^{1/n} - 1} \)n = 2 → 0.644 f_H
Feedback\( A_f = A/(1+A\beta) \); BW ×(1+Aβ)distortion ÷(1+Aβ)
Phase-shift osc.\( f_0 = 1/2\pi RC\sqrt6;\ A \ge 29 \)3×60° RC sections
Wien bridge\( f_0 = 1/2\pi RC;\ A = 3 \)β = 1/3; R_f = 2R₁
Hartley\( f_0 = 1/2\pi\sqrt{(L_1+L_2+2M)C} \)gain ≥ L₁/L₂
Colpitts\( f_0 = 1/2\pi\sqrt{LC_1C_2/(C_1+C_2)} \)gain ≥ C₂/C₁
Crystal\( f_p = f_s\sqrt{1 + C/C_0} \)inductive between f_s, f_p; Q ~ 10⁵
Slew limit\( f_{max} = SR/2\pi V_p \)741: 0.5 V/µs, GBW 1 MHz
GBWA_CL × f_{3dB} = f_Tsingle-pole op-amp
Op-amp basicsinv: −R_f/R₁; non-inv: 1 + R_f/R₁integrator −(1/RC)∫v dt
Schmitt\( V_{UT,LT} = \pm\beta V_{sat};\ V_H = 2\beta V_{sat} \)β = R₁/(R₁+R₂)
In-amp\( A = (1 + 2R/R_G)(R_3/R_2) \)one-resistor gain set
Sallen–Key\( Q = 1/(3 - A_0) \); Butterworth A₀ = 1.586f_c = 1/2πRC
Op-amp astable\( T = 2RC\ln\frac{1+\beta}{1-\beta} \to 2.2RC \)β = ½
555 monostableT = 1.1 RCthresholds V_CC/3, 2V_CC/3
555 astable\( f = 1.44/(R_A + 2R_B)C \)D = (R_A+R_B)/(R_A+2R_B)
PLLlock > capture; \( f_{out} = N f_{ref} \) (synth)565: f_o ≈ 1.2/4R_TC_T
VCO 566\( f_o = 2(V_{CC}-V_C)/R_TC_TV_{CC} \)square + triangle out

§ 4.21Quick Revision Notes — Unit 4 in 25 Points

Rapid-fire recap (last-day revision)

  1. Rectifier core set: ripple 1.21 (HW) / 0.482 (FW); efficiency 40.6 / 81.2%; PIV = 2V_m only for centre-tap; ripple frequency doubles in FW.
  2. C-filter: V_r = I_dc/2fC, better at light load, brutal diode surge currents; L-filter improves at heavy load; LC ≈ load-independent.
  3. Regulators: 78xx needs ~2 V headroom; LM317 → 1.25(1 + R₂/R₁); 723 reference = 7.15 V; load regulation = (V_NL−V_FL)/V_FL.
  4. Bias stability: S = 1+β (fixed) → ≈ 1 + R_B/R_E (divider); design rule R_B ≤ 0.1βR_E; R_E is DC negative feedback, C_E restores AC gain.
  5. Drift drivers: I_CO ×2 per 10 °C, V_BE −2.5 mV/°C, β↑ with T; diode/thermistor compensation; thermal runaway avoided if V_CE < V_CC/2 (rule of thumb).
  6. JFET self-bias: V_GS = −I_D R_S into the square law; divider bias flattens the bias line; MOS drain-feedback bias guarantees saturation.
  7. CE: inverts, max power gain; CB: lowest R_in, best HF, current buffer; CC: A_v ≈ 1, low R_out — the buffer. FET mirror: CS/CG/CD with source follower R_out = 1/g_m.
  8. r_e = 26 mV/I_E; g_m = I_C/V_T ≈ 40I_C — BJT out-transconducts FET at equal current.
  9. Swamped CE gain ≈ −R_C/(r_e + R_E): stable but smaller; impedance reflection ×(1+β) into the base, ÷(1+β) into the emitter.
  10. Cascode = CE + CB → kills Miller, keeps gain; Darlington β ≈ β₁β₂ with two V_BE drops.
  11. Classes: A 360°/25% (50% transformer); B 180°/78.5% with crossover; AB the audio standard; C <180° tuned RF; D switching 90%+.
  12. Miller: C_in = C_f(1+A); n-stage bandwidth shrinks by √(2^{1/n}−1); f_T = βf_β.
  13. Negative feedback: everything good scales with (1+Aβ) — gain stability, bandwidth, distortion; A_f → 1/β; series-in raises R_in, shunt-in lowers; V-sample lowers R_out, I-sample raises.
  14. Barkhausen: |Aβ| = 1, ∠ = 0°; start with |Aβ| slightly > 1.
  15. Oscillator gains: phase-shift ≥ 29 (f = 1/2πRC√6); Wien = 3 (f = 1/2πRC); Colpitts ≥ C₂/C₁; Hartley ≥ L₁/L₂.
  16. Crystal: works inductive between f_s and f_p, Q ~ 10⁴–10⁶ → ppm stability; Pierce = crystal Colpitts.
  17. 741 card: A_OL 2×10⁵, GBW 1 MHz, SR 0.5 V/µs, CMRR 90 dB; f_max = SR/2πV_p; gain × bandwidth = f_T.
  18. Golden rules under NFB: zero input current, V₊ = V₋ (virtual ground in the inverting amp).
  19. Circuit outputs: inverting −R_f/R₁; non-inverting 1 + R_f/R₁ (never below 1); integrator turns squares into triangles; differentiator is noise-prone; log+antilog = multiplier.
  20. Schmitt: V_UT/LT = ±βV_sat, hysteresis 2βV_sat — noise immunity + waveform squaring; it is a bistable.
  21. In-amp: A = 1 + 2R/R_G, one-resistor gain, CMRR high because stage-1 CM gain = 1; front end for bridges/biopotentials.
  22. Clipper removes (level = V_R ± 0.7); clamper shifts (p-p preserved, RC ≫ T); precision rectifier hides V_γ inside the loop.
  23. Sallen–Key: Q = 1/(3−A₀), Butterworth needs A₀ = 1.586, A₀ → 3 oscillates; state-variable gives LP/BP/HP at once.
  24. 555: mono T = 1.1RC; astable f = 1.44/(R_A+2R_B)C, duty > 50%; thresholds V_CC/3 and 2V_CC/3; pin 5 = VCO/PWM.
  25. PLL: PD → LPF → VCO; lock range > capture range (filter throttles capture); in lock the error is phase; ÷N loop synthesizes Nf_ref; VCO voltage = demodulated FM. V/F = linear VCO (charge balance for precision); F/V = pulse + average (tachometer).

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