Chapter 1: Introduction EET-223: RF Communication Circuits Walter - - PowerPoint PPT Presentation
Chapter 1: Introduction EET-223: RF Communication Circuits Walter - - PowerPoint PPT Presentation
Chapter 1: Introduction EET-223: RF Communication Circuits Walter Lara Introduction Electronic communication involves transmission over medium from source to destination Information can contain voice, picture, sensor output, or any
Introduction
- Electronic communication involves transmission
- ver medium from source to destination
- Information can contain voice, picture, sensor
- utput, or any data.
- Intelligence signal or simply “intelligence”– contains
information to transmit
- Intelligence is at frequencies too low to transmit
(e.g. voice 20Hz – 3 KHz) - would require huge antennas
Introduction – Cont’d
- Multiple intelligence signals have the same
frequency (e.g. voice) - would result on interference if transmitted simultaneously
- Modulation – process of putting intelligence signal
- nto high-frequency carrier for transmission
- Demodulation – process of extracting the
intelligence from a transmitted signal
Introduction – Cont’d
- Carrier signal is a sinusoid:
– v(t) = Vp sin(wt + Φ) – Vp : peak value – w: angular velocity – Φ: phase angle
- Can modulate by varying:
– Vp : Amplitude Modulation (AM) – w: Frequency Modulation (FM) – Φ: Phase Modulation (PM)
Introduction – Cont’d
- RF Spectrum divided into ranges. Example:
– MF (300 KHz – 3 MHz): AM Radio – VHF (30-300 MHz): FM Radio, some TV, some cellphones – UHF (300MHz – 3 GHz): TV, cellphones, WiFi, microwaves
- See Table 1-1 for complete details
Figure 1-1 A communication system block diagram.
The Decibels (dB) in Communications
- Used to specify measured and calculated values of
voltage, power and gain
- Power Gain: dB = 10 log P2 / P1
- Voltage Gain: dB = 20 log V2 / V1
- dB using a 1W reference:
dBW = 10 log P / 1 W
- dB using a 1mW reference:
dBm = 10 log P / 1 mW
- dB using a 1mW reference with respect to a load:
dBm(RL) = 20 log V / V0dBm
Noise
- Any undesired voltages/currents that appear in a
signal
- Often very small (~uV)
- Can be introduced by the transmitting medium
(external noise):
– human-made (e.g. sparks, lights, electric motors) – atmosphere (e.g. lightning) – space (e.g. sun)
- Can be introduced by the receiver (internal noise):
– physical properties of electronic components
Figure 1-2 Noise effect on a receiver s first and second amplifier stages.
Thermal Noise
- Aka Johnson or White Noise
- Random voltage fluctuations across a
circuit component caused by random movement of electrons due to heat
- Contains “all” frequencies (all colors = white)
- Power from Thermal Noise: Pn = KT ∆f
– K = 1.38 x 10-23 J/K (Boltzman’s Constant) – T: resistor temperature, in Kelvins – ∆f: bandwidth of system
Figure 1-3 Resistance noise generator.
Thermal Noise – Cont’d
- Pn = (en / 2)2 / R = KT ∆f
- Noise Voltage (rms value):
en = 𝟓𝑳𝑼∆𝒈𝑺
- Textbook assumes room temperature is
17C = 290.15 K, so 𝟓𝑳𝑼 = 1.6 x 10-20 J
Other Noise Sources
- Shot Noise – caused by the fact that
electrons are discrete particles and take their own random paths
- Transit-Time Noise – occurs at high
frequencies near the device cutoff frequency
- Excess Noise – occurs at low frequencies
(<1 KHz), caused by crystal surface defects
Figure 1-4 Device noise versus frequency.
Signal-to-Noise Ratio (S/R or SNR)
- Very important & common measure
- The higher, the better
- Formula: SNR = Ps / Pn
– Ps: Signal Power – Pn: NoisePower
- Typically in dB: SNR(dB) = 10 log (Ps / Pn)
Noise Figure (NF)
- Measure of a device degradation to SNR
- The lower, the better
- Formula: NF = 10 log SNRin / SNRout
– SNRin : SNR at device’s input – SNRout : SNR at device’s output
- Noise Ratio: NR = SNRin / SNRout
- Useful Relationship:
SNRout = SNRin – NF (all in dB)
Information & Bandwidth
- Amount of information transmitted in a
given time is limited by noise & bandwidth
- Harley’s Law:
information α bandwidth x time of transmission
- In USA, bandwidth is regulated by FCC
– AM Radio: 30 KHz – FM Radio: 200 KHz – TV: 6 MHz
Fourier Analysis
- Any signal can be expressed as the sum of
pure sinusoids.
- See Table 1-4 for selected waveforms
- For a square wave:
v = 4V/π (sin wt + 1/3 sin 3wt + 1/5 sin 5wt + …) – sin wt : fundamental frequency – 1/3 sin 3wt: 3rd harmonic – 1/5 sin 5wt: 5th harmonic
- The more bandwidth, the better
representation
Figure 1-9 (a) Fundamental frequency (sin t); (b) the addition of the first and third harmonics (sint + 1/3 sin 3t); (c) the addition of the first, third, and fifth harmonics (sin t + 1/3 sin 3t + 1/5 sin 5t).
Figure 1-9 (continued) (a) Fundamental frequency (sin t); (b) the addition of the first and third harmonics (sint + 1/3 sin 3t); (c) the addition of the first, third, and fifth harmonics (sin t + 1/3 sin 3t + 1/5 sin 5t).
Figure 1-9 (continued) (a) Fundamental frequency (sin t); (b) the addition of the first and third harmonics (sint + 1/3 sin 3t); (c) the addition of the first, third, and fifth harmonics (sin t + 1/3 sin 3t + 1/5 sin 5t).
Figure1-10 Square waves containing: (a) 13 harmonics; (b) 51 harmonics.
Figure1-10 (continued) Square waves containing: (a) 13 harmonics; (b) 51 harmonics.
Fast Fourier Transform (FFT)
- Signal processing technique that converts
time-varying signals to frequency components using samples
- Allows Fourier analysis when using
- scilloscopes and spectrum analyzers
Figure 1-11 (a) A 1-kHz sinusoid and its FFT representation; (b) a 2-kHz sinusoid and its FFT representation.
Figure 1-11 (continued) (a) A 1-kHz sinusoid and its FFT representation; (b) a 2-kHz sinusoid and its FFT representation.
Figure 1-12 A 1-kHz square wave and its FFT representation.
Figure 1-13 (a) A low-pass filter simulating a bandwidth-limited communications channel; (b) the resulting time series and FFT waveforms after passing through the low-pass filter.