Introduction to Communication Prepared By Dr. Hany Taher Modified by: Dr. Mouaaz Nahas
Text Book 2
Contents 3
Contents (Cont.) 4
5
6
7
Comm. System (Cont.) ) that converted by input transducer 8
Comm. System (Cont.) 9
10
Can be eliminated Comm. System (Cont.) 11
Cannot be eliminated Comm. System (Cont.) 12
.. .. .. Comm. System (Cont.) 13
.. Analog & Digital Messages 14
Analog & Digital Messages (Cont.) 15
.. .. Noise immunity of Digital Signals 16
Distorted signal Distorted noisy signal .. Due to channel Noise immunity of Digital Signals (Cont.) 17
Noise immunity of Digital Signals (Cont.) .. 18
.. .. .. Viability of Regenerative Repeaters in Digital Communication 19
Viability of Regenerative Repeaters in Digital Communication (Cont.) .. .. .. 20
Signal to noise ratio Signal Bandwidth & SNR A measure of the width of a range of frequencies, measured in hertz (Hz). 21
Sinusoidal Waveform 22
Modulation 23
24
25
Demodulation 26
... 27
AM (Cont.) 28
AM (Cont.) .. .. LetA=1 .. 29
AM (Cont.) .. .. .. 30
AM (Cont.) .. .. .. .. 31
AM Demodulation 32
AM Demodulation (Cont.) 33
Example on AM Solution.. 34
Example on AM (Cont.) 35
Example on AM (Cont.) 36
37
Modulators (Cont.) 38
Modulators (Cont.) .. 39
Modulators (Cont.) .. .. .. 40
Modulators (Cont.) .. .. 41
Modulators (Cont.) .. 42
Modulators (Cont.) .. 43
Modulators (Cont.) .. .. .. 44
Modulators (Cont.) 45
Modulators (Cont.) .. .. .. 46
Modulators (Cont.) .. 47
.. .. 48
Modulators (Cont.) .. .. .. .. .. 49
Modulators (Cont.) 50
Modulators (Cont.) .. 51
.. .. .. 52
DSB-SC Demodulation (Cont.) .. .. 53
Solution 54
Example (Cont.) LPF 55
Solution Example: Frequency Mixer 56
Example: Frequency Mixer (Cont.) 57
Exercises
Exercises (Cont.) Solution 59
Exercises (Cont.) 60
Exercises (Cont.) 61
Exercises (Cont.) 62
Exercises (Cont.) 63
Exercises (Cont.) 64
Exercises (Cont.)
Exercises (Cont.) 66
Exercises (Cont.) Wanted Unwanted Solution 67
Exercises (Cont.) Band pass Filter at w c 68
Exercises (Cont.) 69
Exercises (Cont.) Solution
Exercises (Cont.) k 71
.. Transmitter may be very far, i.e, thousands of Kms Expensive .. Solution is to use Amplitude modulation: 72
AM (Cont.) ..Disadvantage .... More power is needed .... 1. Point to point communications : One transmitter for every receiver. One transmitter for every receiver. Complexity in the receiver is justified. Complexity in the receiver is justified. 2. Broadcast communications: Single transmitter and multi receivers. Single transmitter and multi receivers. Better economically to have one expensive high-power transmitter and simpler less expensive multiple receivers. Better economically to have one expensive high-power transmitter and simpler less expensive multiple receivers. 73
AM (Cont.) .. .. .. Remember Compare 74
AM (Cont.) 75
AM (Cont.) 76
AM (Cont.) Two conditions for the envelop detection of an AM signal are: 1) f c > bandwidth of m(t) 2)A + m(t) ≥ 0 for all t 77 If A + m(t) is not positive for all t, m(t) cannot be recovered from the envelop \ A + m(t)\. If m(t) ≥ 0 for all t, A=0 already satisfies the condition A + m(t) ≥ 0. No need to add any carrier because the envelop of the DSB-SC signal m(t) cosω c t is m(t). This signal can be detected by envelop detection.
AM (Cont.) Let, m p the peak amplitude The modulation index A< m p µ > 1 (overmodulation) 78
Solution 79
Example (Cont.) 80
Sidebands and AM efficiencies .. .. Time mean square value .. .. 81
Sidebands and AM efficiencies (Cont.) .. 82
Solution 83 Sidebands and AM efficiencies (Cont.)
.. .. 84
85 Generation of AM Signals (Cont.)
86
Rectifier Detector (Cont.) 87
88 Rectifier Detector (Cont.)
89 Rectifier Detector (Cont.)
90 Rectifier Detector (Cont.)
Envelope Detector 1. First AM positive cycle Capacitor is charged until the peak value 2. The AM signal falls below the peak Diode On Diode is Off Capacitor is discharged into the resistance with time constant ‘RC’ and its voltage starts to decrease from the peak value 91
3. The AM signal now is in its negative cycle Diode is still off Capacitor is still discharged into the resistance and its voltage continues in decreasing from the peak value 4. The AM signal now is going into 2 nd positive cycle Diode is still off until the value of AM signal becomes larger than voltage on the capacitor, at this moment, Diode is on Capacitor is charged until the peak value, and so on. The above steps are repeated again 92 Envelope Detector (Cont.)
Ripples To decrease the ripples, use high ‘RC’ Take Care Very high RC does not accurately follow the envelope T C << RC << T m (1/B) 93 Envelope Detector (Cont.)
In DSB (SC and AM), each USB and LSB contains complete information about m(t). So DSB modulation requires twice the bandwidth of baseband to transmit (spectral redundancy). To improve the spectral efficiency, we have two schemes: –Single-Sideband (SSB). –Quadrature Amplitude Modulation (QAM). 94 Bandwidth-Efficient AM
As mentioned earlier, DSB occupies twice of bandwidth of baseband (this is a disadvantage). Solution Two baseband signal on the same carrier frequency, how??!!!!! Two baseband signal on the same carrier frequency, how??!!!!! There is π/2 (radian) phase shift between the two carriers, i.e. Cosine and Sine as example. There is π/2 (radian) phase shift between the two carriers, i.e. Cosine and Sine as example. 95 QAM (or Quadrature Multiplexing) transmits two DSB signals using two carriers of the same frequency but in phase quadrature.
QAM (Cont.) Two baseband signals Two baseband signals Carrier signal Carrier signal Phase Shifted Carrier signal Phase Shifted Carrier signal Modulated Signal 96 Phase Shifter
QAM (Cont.) In-phase (I) In-phase (I)channel Quadrature (Q) Quadrature (Q)channel 97
QAM (Cont.) The last two terms in x 1 (t) form a QAM signal with 2ω c as the carrier frequency. They are suppressed by the low-pass filter yielding m 1 (t). 98 Obtain an expression for x 2 (t)???? Obtain an expression for x 2 (t)????
99 QAM (Cont.) Note that QAM must be totally synchronous. The problem is that any error in phase or frequency of the carrier at the demodulation results in loss or interference between the two signals. Both baseband signals will appear at the filter output instead of m 1 (t) Cochannel interference
DSB has two sidebands, USB and LSB SSB has one half of the bandwidth of DSB 100
SSB (Cont.) 101 SSB signal can be coherently (synchronously) demodulated by multiplying it by cos ω c t (exactly like DSB-SC). Example of USB demodulation is: SSB-SC
102 SSB (Cont.)
F
SSB (Cont.) 104
SSB (Cont.) Substitute with 105
SSB (Cont.) Φ LSB (ω) = M + ( ω + ω c ) + M - ( ω - ω c ) Φ LSB (t) = m + (t) e -jωct + m - (t) e jωct Substitute with 106
SSB (Cont.) 107
Determination of m h (t) 108
SSB (Cont.) Hilbert transform 109
SSB (Cont.) 110
SSB (Cont.) .. .. 111
Solution 112
Example (Cont.) 113
Example (Cont.) 114
DSB is passed through BPF to eliminate undesired band Most commonly used To obtain USB, the filter should pass all components above ω c and attenuate all components below ω c Difficult to design sharp cutoff filter Voice spectrum 300 Hz 115
Generation of SSB signals (Cont.) Difficult to build 116
Envelope detection of SSB with carrier (SSB+C) If ‘A’ is large enough m(t) can be recovered by envelop detection envelop detection 117
Envelope detection of SSB with carrier (SSB+C) (Cont.) 118
119
Example (Cont.) 120
Solution Diodes conducting The diode resistance is ‘ r’ off state off state The diode resistance is ‘ ∞’ A carrier in positive cycle A carrier in negative cycle The output voltage is ‘ zero’ The diode acts as a gate with gain ‘2R/(R+r)’ (R/(r+R))φ (t) appears across each resistance ‘R’ 121
Solution (Cont.) The output is, e 0 (t) = (2R/(R+r)) ω (t) m (t) If e 0 is passed through B.P.F centered at ω C and has 2B band width, the output is ( 4R/ ( π ( R + r ) ) m ( t ) Cos (ω C t ) 122
Solution (Cont.) This circuit can work as a demodulator as follows: The input is m (t) cos ω C t LPF is used at the output The output ( 2R/ ( π ( R + r ) ) m ( t ) 123
Solution e 0 (t) = ( 4R/ ( π ( R + r )) m ( t ) cos ω C t e 0 (t) = ( 4R/ ( π ( R + r )) m ( t ) cos ω C t = k m ( t ) cos ω C t = k m ( t ) cos ω C t m ( t ) = sin (ω C t + θ ) e 0 (t)= k sin ( ω C t + θ ) cos ω C t 124
Solution (Cont.) e 0 (t) = k/2 (sin ( 2 ω C t + θ ) + sin θ ) The LPF suppresses the sinusoid and transmits only the DC component only the DC component e o / (t) = k/2 sin θ 125 Phase difference between the two sinusoids
Solution Attenuated by LPF Removed by DC blocker 126 ab cd
127
Solution 128
Solution 129
Solution (Cont.) 130
Amplitude modulation: Vestigial Sideband (VSB) Due to the difficulties in generating SSB signals VSB is used VSB is asymmetric system VSB is a compromise between DSB and SSB VSB is easy to generate and its bandwidth is only % greater than SSB 131
VSB (Cont.) 132
VSB (Cont.) 133
VSB (Cont.) 134
VSB (Cont.) 135
VSB (Cont.) Solution 136
Use of VSB in television broadcast 137
Carrier Acquisition In any technique from amplitude modulation techniques, the local oscillator must be in synchronous with the oscillator that is used in transmitter side. Why? Consider DSB-SC case: .. .. .. 138
Carrier Acquisition (Cont.) .. Filtered by LPF .. 139
Carrier Acquisition (Cont.) 140 Attenuation to the message .. .. Beating effect Solution Quartz Crystal Oscillator? Difficult to built at high frequencies Phase Locked Loop (PLL)
Free running frequency .. .. .. Suppressed by LPF 141
PLL (Cont.) 142
PLL (Cont.) If the frequencies are different Suppose the frequency of the input sinusoidal signal is increased from ω c to ω c + k This means that the incoming signal is Thus the frequency increase in incoming signal causes θ i to increase to θ i + kt Increasing θ e, and vice versa 143
DC component 144
Carrier Acquisition in DSB-SC (Cont.) 145
146
Carrier Acquisition in SSB-SC (Cont.) 147
148
Angle Modulation (Cont.) 149
Angle Modulation (Cont.) Two techniques are possible to transmit m(t) by varying angle θ of a carrier. 150
Angle Modulation (Cont.) 151
Angle Modulation (Cont.) 152
153
154
Solution 155
156 Example (Cont.)
157
Example (Cont.) 158
Example (Cont.) 159
160 Solution
Example (Cont.) 161
Example (Cont.) 162 This scheme is called Frequency Shift Keying (FSK) where information digits are transmitted by keying different frequencies.
Example (Cont.) 163
Example (Cont.) The derivative ṁ (t) is zero except at points of discontinuity of m(t) where impulses of strengths ±2 are present. 164
Example (Cont.) 165
Example (Cont.) 166 This scheme is called Phase Shift Keying (PSK) where information digits are transmitted by shifting the carrier phase. The phase difference (shift) is π.
167
Bandwidth of Angle Modulated Waves (Cont.) .. .. .. 168
Bandwidth of Angle Modulated Waves (Cont.) .. .. .. 169
.. .. 170
Narrowband Angle Modulation (Cont.) Compare with AM modulated signal .. .. 171
Generation of NBFM .. 172
Generation of NBPM 173
Can not be ignored Very complicated analysis 174 In practical FM,
WBFM (Cont.) Simple way to analyze the problem m(t) m(t) is band limited to B Hz m(t) is approximated by pulses of constant amplitudes (cells), FM analysis of constant amplitude is easier 175 (Staircase)
WBFM (Cont.) m(t) ≈ Pulse interval ≤ 1 / 2B Sec The FM signal of one of these cells starting at t = t k 1/2B Sec Sinusoidal 176
WBFM (Cont.) The FM spectrum of consists of the sum consists of the sum of the Fourier transforms of the sinusoidal pulses. of the Fourier transforms of the sinusoidal pulses. 177
WBFM (Cont.) The min. and max. amplitude of modulating signals are -m p and m p the min. frequency the max. frequency the Bandwidth 178
WBFM (Cont.) .. .. Do not forget, this value is calculated for From earlier analysis: For NBFM, 179 The Peak Frequency Deviation:
WBFM (Cont.) 180 For a truly wideband case, A better bandwidth estimate is: The “deviation ratio” plays a role similar to the “modulation index” in AM.
.. 181
182
Solution 183
Example (Cont.) 184
Example (Cont.) 185
Generation of FM Waves 186 Direct FM Method. Indirect FM Method.
NBFM Generation 187 Recall: The output of the this NBFM has some amplitude variations. A nonlinear device designed to limit the amplitude of a bandpass signal can remove most of this distortion.
NBFM Generation (Cont.) Bandpass Limiter: used to remove amplitude variations in FM wave. 188 The input-output characteristics of the hard limiter.
NBFM Generation (Cont.) Hard limiter input and the corresponding output. 189 Hard limiter output with respect to θ
NBFM Generation (Cont.) 190
NBFM Generation (Cont.) 191
NBFM Generation (Cont.) 192
Demodulation of FM Signals The simplest demodulator is an ideal differentiator followed by an envelop detector. 193 envelop
Demodulation of FM Signals (Cont.) 194 envelop detector can be used to recover m (t )
FM Demodulation using PLL 195 Free running frequency