I. Fourier Transform & Signal Analysis
A. Properties of Fourier Transform
Let \(X(f) = \mathcal{F}\{x(t)\}\). Key properties:
| Property | Time Domain | Frequency Domain |
|---|---|---|
| Linearity | \(a x_1(t) + b x_2(t)\) | \(a X_1(f) + b X_2(f)\) |
| Time Shifting | \(x(t - t_0)\) | \(X(f) e^{-j2\pi f t_0}\) |
| Frequency Shifting | \(x(t) e^{j2\pi f_0 t}\) | \(X(f - f_0)\) |
| Time Scaling | \(x(a t)\) | \(\frac{1}{|a|} X\left(\frac{f}{a}\right)\) |
| Duality | \(X(t) \leftrightarrow 2\pi x(-f)\) | — |
| Convolution | \(x_1(t) * x_2(t)\) | \(X_1(f) X_2(f)\) |
| Multiplication | \(x_1(t) x_2(t)\) | \(X_1(f) * X_2(f)\) |
| Parseval's Theorem | \(\int_{-\infty}^{\infty} |x(t)|^2 dt = \int_{-\infty}^{\infty} |X(f)|^2 df\) | — |
[!TIP]
Exam Focus: Time scaling often confused: \(x(at)\) compresses if \(|a|>1\), and FT magnitude scales by \(1/|a|\). Duality is frequently tested—swap time/frequency with sign flip and \(2\pi\) factor.
B. Fourier Transform of Basic Signals
| Signal \(x(t)\) | Fourier Transform \(X(f)\) |
|---|---|
| Unit Impulse \(\delta(t)\) | \(1\) |
| Unit Step \(u(t)\) | \(\frac{1}{j2\pi f} + \frac{1}{2} \delta(f)\) |
| Signum \(\text{sgn}(t)\) | \(\frac{1}{j\pi f}\) |
| Sinusoid \(\sin(2\pi f_0 t)\) | \(\frac{j}{2} [\delta(f+f_0) - \delta(f-f_0)]\) |
| Cosinusoid \(\cos(2\pi f_0 t)\) | \(\frac{1}{2} [\delta(f-f_0) + \delta(f+f_0)]\) |
| Gate/Rectangular Pulse \(\text{rect}\left(\frac{t}{\tau}\right)\) | \(\tau \text{sinc}(f\tau)\) |
| Damped Sinusoid \(e^{-at} \sin(\omega_0 t) u(t)\), \(a>0\) | \(\frac{\omega_0}{(a+j2\pi f)^2 + \omega_0^2}\) |
[!TIP]
Common Pitfall: FT of \(u(t)\) includes an impulse at DC. Gate function FT is \(\tau \text{sinc}(f\tau)\)—remember \(\text{sinc}(x) = \sin(\pi x)/(\pi x)\).
C. Convolution Theorem
Statement:
Convolution in time domain ↔ Multiplication in frequency domain.
If \(y(t) = x_1(t) * x_2(t)\), then \(Y(f) = X_1(f) X_2(f)\).
Proof Sketch:
\[ Y(f) = \int_{-\infty}^{\infty} y(t) e^{-j2\pi f t} dt = \int_{-\infty}^{\infty} \left[ \int_{-\infty}^{\infty} x_1(\tau) x_2(t-\tau) d\tau \right] e^{-j2\pi f t} dt \]
Swap integrals and substitute \(u = t-\tau\):
\[ = \int_{-\infty}^{\infty} x_1(\tau) e^{-j2\pi f \tau} d\tau \cdot \int_{-\infty}^{\infty} x_2(u) e^{-j2\pi f u} du = X_1(f) X_2(f) \]
Applications:
-
Simplifying LTI system analysis: output FT = input FT × system FT.
-
Computing inverse FT of products via convolution.
D. Correlation
Auto-correlation:
\[ R_{xx}(\tau) = \int_{-\infty}^{\infty} x(t) x^*(t-\tau) dt \]
-
Even function: \(R_{xx}(-\tau) = R_{xx}^*(\tau)\).
-
Maximum at \(\tau=0\): \(R_{xx}(0) = E_x\) (total energy for energy signals, average power for power signals).
-
Relation to Energy Spectral Density (ESD):
\[ \psi_{xx}(f) = |X(f)|^2 \quad \text{and} \quad R_{xx}(\tau) = \int_{-\infty}^{\infty} \psi_{xx}(f) e^{j2\pi f \tau} df \]
(Wiener-Khinchin for energy signals).
Cross-correlation:
\[ R_{xy}(\tau) = \int_{-\infty}^{\infty} x(t) y^*(t-\tau) dt \]
-
Not necessarily even.
-
Relation to Cross-Spectral Density:
\[ \psi_{xy}(f) = X(f) Y^*(f) \quad \text{and} \quad R_{xy}(\tau) = \int_{-\infty}^{\infty} \psi_{xy}(f) e^{j2\pi f \tau} df \]
-
For power signals, use time-averaged correlation and Power Spectral Density (PSD).
E. Power Spectral Density (PSD)
Definition:
For a wide-sense stationary (WSS) random process \(x(t)\), PSD \(S_{xx}(f)\) is the Fourier transform of its auto-correlation function \(R_{xx}(\tau)\):
\[ S_{xx}(f) = \int_{-\infty}^{\infty} R_{xx}(\tau) e^{-j2\pi f \tau} d\tau \]
\[ R_{xx}(\tau) = \int_{-\infty}^{\infty} S_{xx}(f) e^{j2\pi f \tau} df \]
Properties:
-
\(S_{xx}(f) \geq 0\) (non-negative).
-
Even function: \(S_{xx}(-f) = S_{xx}(f)\).
-
Total power: \(P = \int_{-\infty}^{\infty} S_{xx}(f) df = R_{xx}(0)\).
Wiener-Khinchin Theorem:
Auto-correlation and PSD are Fourier transform pairs.
II. Amplitude Modulation (AM)
A. Principles & Time-Domain Expression
Need for Modulation:
-
Efficient antenna size (high frequency).
-
Multiplexing (channel allocation).
-
Reduced noise and interference.
-
Flexibility in transmission.
Standard AM (DSB-TC):
\[ s(t) = [A_c + m(t)] \cos \omega_c t \]
where \(A_c\) = carrier amplitude, \(m(t)\) = message signal with \(|m(t)|_{\text{max}} \leq A_c\).
B. Spectrum & Modulation Index
Spectrum:
\[ S(f) = \frac{A_c}{2} [\delta(f-f_c) + \delta(f+f_c)] + \frac{1}{2} [M(f-f_c) + M(f+f_c)] \]
-
Carrier at \(\pm f_c\).
-
Upper Sideband (USB): \(M(f-f_c)\).
-
Lower Sideband (LSB): \(M(f+f_c)\).
Modulation Index \(m\):
\[
m = \frac{|m(t)|_{\text{max}}}{A_c}, \quad 0 \leq m \leq 1 \text{ (no overmodulation)}
\]
Bandwidth: \(BW = 2 f_m\), where \(f_m\) = max frequency in \(m(t)\).
C. Power Analysis & Power Saving
For single-tone \(m(t) = A_m \cos \omega_m t\):
-
Carrier Power: \(P_c = \frac{A_c^2}{2R}\)
-
Sideband Power (each): \(P_{sb} = \frac{m^2 A_c^2}{4R}\)
-
Total Power: \(P_t = P_c \left(1 + \frac{m^2}{2}\right)\)
-
Power Efficiency: \(\eta = \frac{P_{sb,\text{total}}}{P_t} = \frac{m^2}{2 + m^2}\)
% Power Saving in Suppressed Carrier Systems:
-
DSB-SC: Carrier suppressed → saving = \(\frac{P_c}{P_t} \times 100 = \frac{1}{1 + m^2/2} \times 100\)
-
SSB-SC: Carrier + one sideband suppressed → saving = \(\frac{P_c + P_{sb}}{P_t} \times 100 = \frac{1 + m^2/2}{1 + m^2/2} \times 100 = 100\%\)? Wait: Actually for SSB-SC, only one sideband transmitted, so power = \(P_{sb}\). Compared to AM: saving = \(\frac{P_c + P_{other\,sb}}{P_t} \times 100 = \left(1 - \frac{P_{sb}}{P_t}\right) \times 100 = \left(1 - \frac{m^2/2}{1 + m^2/2}\right) \times 100 = \frac{1}{1 + m^2/2} \times 100\)? That's same as DSB-SC? No: In DSB-SC, both sidebands transmitted, no carrier: power = \(2 P_{sb} = \frac{m^2 A_c^2}{2R}\). AM total power = \(P_c + 2P_{sb}\). So DSB-SC saving vs AM: \(\frac{P_c}{P_t} \times 100 = \frac{1}{1 + m^2/2} \times 100\). SSB-SC: only one sideband, power = \(P_{sb}\). Saving vs AM: \(\frac{P_c + P_{sb}}{P_t} \times 100 = \frac{1 + m^2/2}{1 + m^2/2} \times 100?\) Actually:
\(P_t^{\text{AM}} = P_c + 2P_{sb}\)
\(P^{\text{SSB}} = P_{sb}\)
Saving = \(\frac{P_c + P_{sb}}{P_t^{\text{AM}}} \times 100 = \frac{P_c + P_{sb}}{P_c + 2P_{sb}} \times 100 = \frac{1 + m^2/2}{1 + m^2} \times 100\)? Let's compute:
\(P_c = A_c^2/(2R)\), \(P_{sb} = m^2 A_c^2/(4R)\)
So \(P_c + P_{sb} = \frac{A_c^2}{2R} (1 + m^2/2)\)
\(P_t^{\text{AM}} = \frac{A_c^2}{2R} (1 + m^2/2)\)? Wait: \(P_t^{\text{AM}} = P_c + 2P_{sb} = \frac{A_c^2}{2R} + 2 \cdot \frac{m^2 A_c^2}{4R} = \frac{A_c^2}{2R} (1 + m^2/2)\). So \(P_c + P_{sb} = P_t^{\text{AM}} - P_{sb}\). So saving = \(\frac{P_t^{\text{AM}} - P_{sb}}{P_t^{\text{AM}}} \times 100 = \left(1 - \frac{P_{sb}}{P_t^{\text{AM}}}\right) \times 100 = \left(1 - \frac{m^2/2}{1 + m^2/2}\right) \times 100 = \frac{1}{1 + m^2/2} \times 100\). That's same as DSB-SC? But DSB-SC transmits both sidebands, so its power is \(2P_{sb}\), saving vs AM: \(\frac{P_c}{P_t^{\text{AM}}} \times 100 = \frac{1}{1 + m^2/2} \times 100\). So both DSB-SC and SSB-SC have same % saving? That can't be right. Actually SSB-SC saves more because it also removes one sideband. So saving should be larger. Let's recalc:
AM total power: \(P_t = P_c + P_{USB} + P_{LSB} = P_c + 2P_{sb}\) (since symmetric).
DSB-SC: no carrier, both sidebands → \(P_{DSB} = 2P_{sb}\).
SSB-SC: no carrier, one sideband → \(P_{SSB} = P_{sb}\).
Saving vs AM:
-
DSB-SC: \(\frac{P_c}{P_t} \times 100 = \frac{P_c}{P_c+2P_{sb}} \times 100 = \frac{1}{1 + 2P_{sb}/P_c} \times 100 = \frac{1}{1 + m^2/2} \times 100\)? Since \(P_{sb}/P_c = m^2/2\).
-
SSB-SC: \(\frac{P_c + P_{sb}}{P_t} \times 100 = \frac{P_c + P_{sb}}{P_c+2P_{sb}} \times 100 = \frac{1 + P_{sb}/P_c}{1 + 2P_{sb}/P_c} \times 100 = \frac{1 + m^2/2}{1 + m^2} \times 100\).
For \(m=1\): DSB-SC saving = \(1/(1+0.5) \times 100 = 66.67\%\); SSB-SC saving = \((1+0.5)/(1+1) \times 100 = 1.5/2 \times 100 = 75\%\). Yes, SSB-SC saves more. So formula:
\[ \text{% Saving (SSB-SC)} = \frac{1 + \frac{m^2}{2}}{1 + m^2} \times 100 \]
D. Generation Techniques
-
Square Law Modulator:
-
Uses nonlinear device (diode): \(i = a_1 v + a_2 v^2\).
-
Input: \(v = A_c \cos \omega_c t + m(t)\).
-
Squaring term generates \(A_c m(t) \cos \omega_c t\) (DSB-SC) and carrier/sideband terms.
-
Filter out carrier → DSB-SC.
-
-
Balanced Modulator:
-
Two nonlinear devices in push-pull, carrier fed in opposite phase.
-
Carrier cancels at output → DSB-SC directly.
-
DiagramSEARCH: balanced modulator circuit diagram
-
-
Phase Discrimination Method (SSB-SC):
-
Filter Method: Generate DSB-SC, then filter out one sideband (sharp cutoff filter).
-
Phasing Method (Hilbert Transform):
\[ s_{\text{SSB}}(t) = \frac{A_c}{2} m(t) \cos \omega_c t \mp \frac{A_c}{2} \hat{m}(t) \sin \omega_c t \]
where \(\hat{m}(t)\) is Hilbert transform (90° phase shift).
-
DiagramSEARCH: phasing method SSB generator block diagram
-
E. Demodulation Techniques
-
Envelope Detector:
Diode + RC filter. Works if \(m \leq 1\) (no overmodulation). Output \(\propto |A_c + m(t)|\).
-
Synchronous Detector (Coherent):
Multiply received signal by locally generated \(\cos \omega_c t\) (phase-locked), then LPF.
Works for DSB-SC and SSB-SC (with proper carrier phase).
-
Costas Loop (for DSB-SC):
Uses two phase-sensitive detectors (0° and 90° references) to recover carrier and data simultaneously.
DiagramSEARCH: Costas loop block diagram
F. Comparison of AM, DSB-SC, SSB-SC, VSB-SC
| Feature | AM (DSB-TC) | DSB-SC | SSB-SC | VSB-SC |
|---|---|---|---|---|
| Bandwidth | \(2f_m\) | \(2f_m\) | \(f_m\) | \(\approx f_m\) |
| Power Efficiency | Low (carrier waste) | Medium (no carrier) | High (no carrier, one sideband) | Medium-High |
| Spectral Occupancy | Carrier + USB + LSB | USB + LSB | USB or LSB | Carrier + one full sideband + vestige of other |
| Complexity | Simple (envelope detect) | Moderate (coherent detect) | Complex (carrier recovery) | Moderate (filter design) |
| Applications | Broadcast AM | Telemetry, TV (audio) | Military, long-distance | TV video transmission |
G. Vestigial Sideband (VSB-SC)
Need:
-
TV video: baseband 0–4 MHz (video) + audio at 4.5 MHz.
-
SSB requires ideal filters (impossible). VSB transmits one full sideband + partial other (vestige) to ease filtering.
Generation:
-
Filter Method: Generate DSB-SC, pass through vestigial filter (passes one sideband fully, partial other).
-
Phasing Method: Similar to SSB but with imperfect 90° shift.
Detection:
-
Use coherent detection (carrier synchronization) because VSB still has carrier.
-
If carrier is transmitted (VSB-TC), envelope detection possible if modulation index small.
III. Angle Modulation (FM & PM)
A. Fundamentals & Equations
-
FM:
\[ s_{\text{FM}}(t) = A_c \cos\left[\omega_c t + k_f \int_{-\infty}^{t} m(\tau) d\tau\right] \]
Instantaneous frequency: \(\omega_i(t) = \omega_c + k_f m(t)\).
-
PM:
\[ s_{\text{PM}}(t) = A_c \cos[\omega_c t + k_p m(t)] \]
Instantaneous phase: \(\phi_i(t) = \omega_c t + k_p m(t)\).
Relationship:
FM is integral of PM. If \(m(t)\) is a sinusoid, both produce same waveform but with different interpretation of modulation index.
B. Narrowband FM (NBFM) vs Wideband FM (WBFM)
-
NBFM (\(\beta \ll 1\)):
\[ s(t) \approx A_c \cos \omega_c t - A_c \beta \sin \omega_c t \cdot m(t) \]
Spectrum: carrier + two sidebands at \(f_c \pm f_m\), similar to DSB-SC but with carrier.
Bandwidth \(\approx 2f_m\).
-
WBFM (\(\beta \gg 1\)):
Many sidebands (Bessel functions). Bandwidth given by Carson’s Rule.
C. Modulation Index, Frequency Deviation & Bandwidth
-
Modulation Index \(\beta\):
For sinusoidal \(m(t) = A_m \sin 2\pi f_m t\):
\[ \beta = \frac{k_f A_m}{f_m} = \frac{\Delta f}{f_m} \]
where \(\Delta f = k_f A_m\) = peak frequency deviation.
-
Carson’s Rule:
\[ \boxed{BW = 2(\Delta f + f_m)} \]
Approximate bandwidth containing ~98% power.
Example:
Given \(s(t) = 10 \cos(2\pi f_c t + 5 \sin 8\pi t)\):
-
Modulating frequency: \(8\pi t = 2\pi \cdot 4 \cdot t \Rightarrow f_m = 4 \text{ Hz}\)
-
Peak phase deviation = 5 rad → \(\beta = 5\) (since for FM, \(\beta\) = peak phase deviation).
-
\(\Delta f = \beta f_m = 5 \times 4 = 20 \text{ Hz}\)
-
\(BW = 2(20 + 4) = 48 \text{ Hz}\).
D. Generation Methods
-
Direct Method:
-
Varactor Diode Modulator: Varactor capacitance varies with modulating voltage, placed in oscillator tank circuit.
-
Reactance Modulator: Transistor reactance converter.
-
-
Indirect Method (Armstrong):
-
Phase modulator (NBFM) + frequency multipliers (×2, ×3, ...) to increase \(\beta\) and \(f_c\).
-
Advantage: stable carrier frequency.
-
E. Demodulation Methods
-
Phase-Locked Loop (PLL) Detector:
-
PLL tracks FM signal; error voltage (after LPF) is demodulated output.
-
Wide capture range, good SNR.
-
-
Foster-Seeley Discriminator:
-
Two tuned RF circuits (primary & secondary) with 90° phase shift.
-
Frequency changes → amplitude variations at output.
-
DiagramSEARCH: Foster-Seeley discriminator circuit
-
-
Balanced Frequency Discriminator:
- Variation of Foster-Seeley with center tap.
-
Phase Shift Discriminator:
- RC network creates 90° phase shift at \(f_c\).
F. Pre-emphasis & De-emphasis
Need:
-
FM noise power spectral density increases with frequency (\( \propto f^2 \)).
-
High-frequency components of message signal more degraded.
Solution:
-
Pre-emphasis (Transmitter): Boost high-frequency components using high-pass filter (differentiator).
Transfer: \(H_{\text{pre}}(f) = 1 + j\frac{f}{f_c}\) (first-order).
-
De-emphasis (Receiver): Attenuate high frequencies using low-pass filter (integrator).
Transfer: \(H_{\text{de}}(f) = \frac{1}{1 + j\frac{f}{f_c}}\).
SNR Improvement:
Net signal transfer: \(H_{\text{pre}} H_{\text{de}} = 1\) (flat).
Noise: Pre-emphasis amplifies noise at high \(f\), but FM demodulator output noise \(\propto f^2\), and de-emphasis attenuates by \(1/\sqrt{1+(f/f_c)^2}\).
Overall, output SNR at frequency \(f\) improved by factor:
\[ \text{Improvement} = 1 + \left(\frac{f}{f_c}\right)^2 \]
For \(f \gg f_c\), improvement \(\approx (f/f_c)^2\).
IV. Noise in Analog Communication
A. Sources & Classification
| External Noise | Internal Noise |
|---|---|
| Atmospheric (lightning) | Thermal (Johnson-Nyquist) |
| Galactic (cosmic) | Shot (electron discreteness) |
| Man-made (industrial) | Transit-time (high freq) |
| Flicker (1/f noise) |
B. Noise Parameters
-
Noise Figure \(F\):
\[ F = \frac{\text{SNR}_{\text{in}}}{\text{SNR}_{\text{out}}} \quad (\text{at same bandwidth}) \]
\(F \geq 1\); in dB: \(F_{\text{dB}} = 10 \log_{10} F\).
-
Noise Temperature \(T_e\):
\[ T_e = (F - 1) T_0 \]
where \(T_0 = 290 \text{ K}\) (standard).
-
Noise Bandwidth \(B_N\):
Equivalent rectangular bandwidth of filter that passes same noise power as actual filter.
C. Noise in AM Systems
-
Envelope Detector:
-
Threshold effect: when carrier-to-noise ratio (CNR) drops below ~10 dB, output SNR degrades rapidly.
-
Output SNR for single-tone AM:
\[ \left(\frac{S}{N}\right)_{\text{out}} = \frac{m^2 A_c^2}{8 R N_0 B} = \frac{m^2}{2} \cdot \frac{P_c}{N_0 B} \]
where \(N_0\) = noise PSD, \(B\) = baseband bandwidth.
-
D. Noise in FM Systems
-
Threshold Effect:
When input CNR falls below threshold (~10–15 dB), demodulator loses lock, output SNR plummets.
-
Capture Effect:
FM receiver captures stronger signal, rejects weaker (within capture range).
-
Output SNR (Wideband FM):
\[ \left(\frac{S}{N}\right)_{\text{out}} \approx \frac{3}{2} \beta^2 \left(\frac{S}{N}\right)_{\text{IF}} \quad \text{for large } \beta \]
Improves with \(\beta^2\).
E. Figure of Merit
Definition:
\[ F = \frac{(S/N)_{\text{out, baseband}}}{(S/N)_{\text{in, IF}}} \]
Derivation for AM (Envelope Detection):
\[ F_{\text{AM}} = \frac{m^2}{2 + m^2} \]
Derivation for DSB-SC (Coherent Detection):
\[ F_{\text{DSB-SC}} = \frac{m^2}{2} \]
(Assumes perfect carrier synchronization).
[!TIP]
Key Insight: DSB-SC has better figure of merit than AM because no carrier power wasted. For same modulation index, DSB-SC \(F\) is \(\frac{m^2}{2}\) vs AM \(\frac{m^2}{2+m^2}\).
F. Comparative Noise Performance
-
FM vs AM:
FM has superior noise immunity because:
-
Limiter removes amplitude noise.
-
Output SNR \(\propto \beta^2\) (can be very high).
-
Capture effect rejects co-channel interference.
-
-
Threshold Extension: FM systems use phase-locked demodulators to lower threshold effect.
V. Receivers
A. Tuned Radio Frequency (TRF) Receiver
Block Diagram:
RF amplifier → Mixer (not always) → Detector → Audio amplifier.
All stages tuned to carrier frequency.
Advantages:
- Simple, no image frequency.
Disadvantages:
-
Instability (many tuned circuits).
-
Poor selectivity (Q limited).
-
Image frequency problem: \(f_{\text{image}} = f_{\text{signal}} + 2 f_{\text{IF}}\) (if IF used) or direct tuning issues.
B. Superheterodyne Receiver
Block Diagram & Function:
-
RF Amplifier: Selects desired channel, amplifies, provides initial image rejection.
-
Mixer: Heterodynes with LO \(f_{\text{LO}}\) to produce IF \(f_{\text{IF}} = |f_{\text{signal}} - f_{\text{LO}}|\).
-
Local Oscillator: \(f_{\text{LO}} = f_{\text{signal}} \pm f_{\text{IF}}\).
-
IF Amplifier: Fixed frequency (e.g., 455 kHz AM, 10.7 MHz FM), high gain, excellent selectivity.
-
Detector: Demodulates IF signal.
-
Audio Amplifier: Drives speaker.
Intermediate Frequency (IF):
-
Choice Trade-off:
-
Higher IF → better image rejection (since \(f_{\text{image}} - f_{\text{signal}} = 2 f_{\text{IF}}\)).
-
Lower IF → better selectivity (since \(Q = f_{\text{IF}} / BW_{\text{IF}}\)).
-
-
Typical: AM → 455 kHz; FM → 10.7 MHz.
Image Frequency:
\[ f_{\text{image}} = f_{\text{signal}} + 2 f_{\text{IF}} \quad (\text{if } f_{\text{LO}} = f_{\text{signal}} + f_{\text{IF}}) \]
Arises because mixer responds to both \(f_{\text{signal}}\) and \(f_{\text{image}}\) producing same IF.
Image Rejection Ratio (IMRR):
\[ \text{IMRR} = \frac{V_{\text{signal}}}{V_{\text{image}}} \approx Q \cdot \frac{f_{\text{signal}}}{f_{\text{IF}}} \]
where \(Q\) = Q-factor of RF tuned circuit.
Selectivity: Ability to separate adjacent channels (determined by IF filter shape).
Fidelity: Accuracy of audio reproduction.
Automatic Volume Control (AVC): DC from detector controls RF/IF gain to maintain constant output level.
C. Automatic Gain Control (AGC) & Automatic Frequency Control (AFC)
-
AGC:
-
Uses rectified detector output to generate bias voltage controlling RF/IF amplifier gain.
-
Maintains constant output despite signal strength variations.
-
-
AFC:
-
Uses discriminator output (proportional to frequency error) to control LO frequency (via varactor).
-
Stabilizes receiver against drift.
-
VI. Additional Key Topics
A. Gate Function
Definition:
\[ \text{rect}\left(\frac{t}{\tau}\right) = \begin{cases} 1, & |t| \leq \tau/2 \\ 0, & \text{otherwise} \end{cases} \]
Fourier Transform:
\[ \mathcal{F}\left\{\text{rect}\left(\frac{t}{\tau}\right)\right\} = \tau \cdot \text{sinc}(f\tau), \quad \text{sinc}(x) = \frac{\sin(\pi x)}{\pi x} \]
B. Carson's Rule Applications
-
Quick bandwidth estimation for FM signals.
-
Example: \(f_m = 15 \text{ kHz}\), \(\Delta f = 75 \text{ kHz}\) (FM broadcast) → \(BW = 2(75+15) = 180 \text{ kHz}\) (actual FM channel = 200 kHz).
C. FM Transmitter
Block Diagram:
Modulator (direct/indirect) → Power Amplifier → Antenna.
-
Direct: Varactor in oscillator.
-
Indirect: Phase modulator + frequency multipliers.
D. Applications of Modulation Schemes
| Scheme | Applications |
|---|---|
| AM (DSB-TC) | Broadcast radio (medium wave) |
| DSB-SC | Television (audio), telemetry |
| SSB-SC | Long-distance point-to-point, military, amateur radio |
| VSB-SC | Television video transmission (NTSC/PAL) |
| FM | Broadcast radio (VHF), two-way radio (police, taxi), satellite |
Final Exam Strategy:
-
Fourier Transform: Practice transforms of basic signals and property applications.
-
AM Power Saving: Derive formulas for DSB-SC and SSB-SC.
-
SSB Generation: Phase discrimination (phasing method) diagram is frequent.
-
FM: Carson’s rule, NBFM vs WBFM spectrum, PLL demodulation.
-
Noise: Figure of merit derivations (AM vs DSB-SC), FM threshold effect.
-
Receivers: Superheterodyne image frequency calculation, IF choice reasons.
-
VSB & AGC: Short notes common (4m).