MAYURBHANJ SCHOOL OF ENGINEERING � LAXMIPOSI ,BARIPADA,757107
SEMISTAR- 5TH
Pulse Modulation
Analog Pulse Modulation
Digital Pulse Modulation
Pulse Amplitude Modulation (PAM)
Pulse Width Modulation (PWM)
Pulse Code Modulation (PCM)
Delta Modulation (DM)
Pulse Position Modulation (PPM)
Advantage of Pulse modulation: (i) Transmitted power is no longer continuous as in CW
Modulation, but pulsed in nature
(ii) Vacant time between pulse occurrence filled by interleaving/multiplexing pulse waveforms of some other Message (TDM)
Sampling Theorem
This provides a mechanism for representing a continuous time signal by a discrete time signal , taking sufficient number of samples of signal so that original signal is represented in its samples completely. It can be stated as:
𝟏
(i) A band-limited signal of finite energy with no frequency component higher than fm Hz, is completely described by its sample values which are at uniform intervals less than or equal to 1/2fm
seconds apart. [Ts=𝟐𝒇𝒎 ]where Ts is sampling time.
(ii) Sampling frequency must be equal to or higher than 2fm Hz. [fs ≥ 2fm]
A continuous time signal may be completely represented in samples and recovered back, if fs≥2fm, where fs is sampling frequency and fm is maximum frequency component of message signal
Proof of sampling theorem
The Fourier series representation of δ(t) :
n=1
0
𝑠
where a = 1 ∫ δ(t) dt =
1
δ(0) = 1
𝑇𝑠 𝑇
𝑠
𝑇
n s
a =2 ∫δ(t)cosnω dt =
𝑇
𝑠
s
2 δ(0)cosnω 0= 2
𝑇
𝑆
2
bn= ∫δ(t)sinnωst dt
𝑇 -T/2
=2 δ(0)sinnω 0=0
s
T/2
𝑠 -T/2
δ(t)= 1 +Σ ( 2 cosnω t+0)
𝑆
𝑇 𝑇
𝑆
s
1
𝑇
2
𝑇
𝑆 𝑆
s
∴δ(t) = +Σ ( cosnω t+0)
Substitute δ(t) in equation 1.
→y(t)=x(t).δ(t)
𝑇𝑠
1 2
𝑇𝑠
= x(t)[ +Σ ( cosnωst+0)]
1
𝑇𝑆
= [x(t)+2Σ(cosnωst)x(t)]
𝑻
𝑺
s s s
y(t)= 𝟏 [x(t)+2cosω t.x(t)+2cos2ω t.x(t)+2cos3ω t.x(t)......]
Take Fourier transform on both sides.
𝑇
𝑆
s s s s s
Y(ω) = 1 [X(ω)+ X(ω-ω ) +X(ω+ω )+X(ω-2ω )+X(ω+2ω )+ X(ω+3ω )+………..]
n=1
n=∞
n=1
n=∞
n=1
n=∞
n=∞
Y(ω)=𝟏 +∞ 𝑿(𝝎 − 𝒏𝝎 )
𝑻
𝑺
−∞
𝒔
To reconstruct x(t), one has to recover input signal spectrum X(ω) from sampled signal spectrum Y(ω), which is possible when there is no overlapping between the cycles of Y(ω) which is possible if
fs≥2fm
For fs=2fm, is known as Nyquist rate.
s
T =
𝟏
𝟐𝒇𝒎
is known as Nyquist interval
Aliasing Effect
The overlapped region in case of under sampling
represents Aliasing effect. It can be termed as “the phenomenon of a high-frequency component in the spectrum of a signal, taking on the identity of a lower-frequency component in the spectrum of its sampled version.
This effect can be removed by considering
Three types of sampling techniques:
Also called ideal sampling. Practically not used because pulse width cannot be zero and the generation of impulse train not possible.
Natural sampling
Using Fourier series, we can rewrite the signal S(t) as:
0 𝑛=1 𝑠
S(t)= C + ∞ 2𝐶𝑛𝑐𝑜𝑠(𝑛ω 𝑡)
𝑻
𝒔
0 n s
s
Where the Fourier coefficients C = 𝝉 and C =f τsinc(nf τ)
Therefore: x (t)=x(t)[C + ∞ 2𝐶𝑛(𝑐𝑜𝑠𝑛𝜔 𝑡)]
s 0 𝑛=1 𝑠
xs(t)=C0x(t)+2C1x(t) cos(ωst)+2C2x(t) cos(2ωst)+……
Applying Fourier Transform for the above equation
Using x(t)↔X(f)
𝟐
0 0
0
x(t) cos(2πf t)↔ 𝟏[X(f-f )+X(f+f )]
Xs(f)=C0X(f)+C1[X(f-f0)+X(f+f0)]+C2[X(f-f0)+X(f+f0)]+…………
s 0
𝒏=−∞
𝒏
X (f)= C X(f)+ ∞ 𝑪 𝑿(𝒇 − 𝒏𝒇𝒔)
Xs(f) = Aτ/ Ts .[ Σ sin c(n fs.τ) X(f-n fs)]
The signal Xs(t) has the spectrum which consists of message spectrum and repetition of message spectrum periodically in the frequency domain with a period of fs. But the message term is scaled by ‘Co”( sinc function) which is not the case in instantaneous sampling.
ideally sampled signal ,sδ(t) g(t)= s(t) ⊗ h(t)
δ(t)
t
h(t)
⊗
=
0 τ
f(t) ⊗ δ(t) = f(t); property of delta function Applying a modified form; s(t) in place of δ(t)
On convolution of s(t) and h(t), we get a pulse whose duration is equal to h(t) only but amplitude
defined by s(t).
Train of impulses given by:
Ts
𝒏=−∞
δ (t) = ∞ 𝜹(𝒕 − 𝒏𝑻𝒔)
Signal s(t) obtained by multiplication of message signal x(t) and δTs(t)
Thus, s(t) = x(t). δTs(t)
𝒏=−∞
𝒔
s(t)= ∞ 𝒙(𝒏𝑻𝒔)𝜹(𝒕−𝒏𝑻 )
Now sampled signal g(t) given as:
g(t)=s(t) ⊗ h(t)
=
−∞
∞
𝑠 τ ℎ 𝑡 − τ 𝑑τ
G(f)=S(f) H(f)
S(f)=fs 𝑋(𝑓 − 𝑛𝑓𝑠)
g(t) =
−∞
∞
𝑛=−∞
∞
s
𝑥(𝑛𝑇𝑠)δ(τ-nT ) h(t-τ)dτ
−∞
g(t)= ∞
𝒙(𝒏𝑻𝒔)
−∞
∞
𝒔
𝜹(𝝉 − 𝒏𝑻 ) 𝒉(𝒕 − 𝝉)𝒅𝝉
Using shifting property of delta function:
−∞
∞
0
𝑓(𝑡)δ(𝑡 − 𝑡𝑜)=f(t )
−∞
g(t)= ∞
𝒙 𝒏𝑻
𝒔
𝒉(𝒕 − 𝒏𝑻𝒔)
s
−∞
G(f)=f ∞
𝑿 𝒇 − 𝒏𝒇𝒔 𝑯(𝒇) Spectrum of flat top samples
Aperture Effect: Spectrum of flat topped sample is given by;
G(f)=fs ∑〖𝑿(𝒇−𝒏𝒇𝒔)𝑯(𝒇)〗 , where H(f)= τ.sin c(fs.t)𝒆^(−𝒋𝝅𝒇𝝉)
This equation shows that signal g(t) is obtained by passing the signal s(t) through a filter having transfer function H(f).
Figure(a) shows one pulse of rectangular pulse train and each sample of x(t) i.e. s(t) is
convolved with this pulse
Figure (b) shows the spectrum of this pulse. Thus, flat top sampling introduces an amplitude distortion in reconstructed signal x(t) from g(t). There is a high frequency roll off making H(f) act like a LPF, thus attenuating the upper portion of message signal spectrum. This is known as aperture effect
How to minimize aperture effect?? An equalizer at the receiver end is needed to compensate aperture effect. The receiver contains low pass reconstruction Filter with cut off slightly higher than fm Hz.
Reconstruction Filter
Equalizer
PAM
Signal g(t)
Message signal x(t)
Equalizer in cascade with reconstruction filter has the effect of decreasing the in band loss of reconstruction filter, frequency increases in such away so as to compensate aperture effect.
eq
𝑯(𝒇)
−𝒋𝟐𝝅𝒇𝒕𝒅
H (f)=𝑲.𝒆 ,
where td is time delay introduced by LPF being equal to τ/2
Heq(f) =
𝑲
𝝉𝒔𝒊𝒏 𝒄(𝒇𝝉)
Pulse Amplitude Modulation (PAM)
signal.
also allows multiplexing.
BPF characteristics
the input signal during the time that each sample is taken.
known as Natural PAM.
In simplest form PAM can be visualized as o/p of an AND gate whose two inputs are message signal x(t) and pulses at sampling rate
.
the amplitude of each pulse at a constant level during the sampling time,
Transmission Bandwidth in PAM
𝝉 ≪ Ts
f ≥ 𝟐𝒇𝒎 ; 𝑻𝒔 ≤
𝟏
s
𝝉≪ Ts≤
𝟐𝒇𝒎
𝟏
𝟐𝒇𝒎
max
= 𝟏
𝟐𝝉
BW≥ 𝒇𝒎𝒂𝒙; 𝑩𝑾 ≥
If on and off time of PAM pulse is same then f
𝟏
𝟐𝝉
𝟐𝝉
𝑩𝑾 ≥ 𝟏 ≫ fm
Transmission of PAM signals
Drawbacks of PAM
Demodulation of PAM
Holding circuit
Received PAM signal
C
Zero order Holding Circuit
pulses
PAM
signal
Pulse Time modulation
Generation of PTM signals can be either by:
Pulse Width modulation
The pulse width modulation is the modulation of signals by varying the width of pulses. The amplitude and
positions of the pulses are constant in this modulation
Generation of PWM and PPM by Direct Method
and the other input by a saw-tooth signal which operates at carrier frequency.
for all pulses,
Three types of pulse-width modulation (PWM) are possible:
to the message signal (Symmetrical PWM)
Indirect Method:
Modulating signal (A) applied to i/p of PAM circuit [s(t) pulse train] and PAM signal generated(B). S(t) also is i/p to Ramp generator(Integrator circuit), all having equal slopes, amplitude and generation(D). These ramp pulses added to PAM pulses to produce varying height samples. These varying height ramp gates a S.T ckt to generate varying width rectangular pulses of PWM.
PWM
Summer
Schmitt Trigger
Ramp Generator
x(t)
A
PAM
generator
B
C
D
E
F
PWM detector
Schmitt
Trigger
Ramp Generator
Synchronization
Pulse generator
Adder
Level Shifter
Rectifier
LPF
1
2
3
4
5
6
amplitude and width but delayed by specific amount.
Noisy PWM
Pulse position modulation
to the width of the PWM pulses.
Advantage As the amplitude and width are constant
the power handled is constant
Disadvantage: Synchronization between Transmitter and receiver is a necessity
width
Transmission BW of PWM and PPM
T
𝟏
𝟐𝒕𝒓
PAM
PWM
PPM
Difference Between PAM, PWM, and PPM
Parameter
PAM
Train of Pulses
Amplitude
Low
Low
PWM
Train of Pulses Width
High
High
Low Varies
Width Variations Moderate Varies
Not needed
rise time of the pulse
PPM
Train of Pulses Position
High
High
Position Variations High
Remains Constant Necessary
rise time of the pulse
Instantaneous power varies with Constant width of the pulses
with amplitude of pulses
Complex Easy
12 Similarity with other Modulation Systems Similar to AM
Similar to FM
Complex Similar to PM
Q. For a PAM transmission of voice signal with fm=3kHz, calculate the transmission BW. Given that fs=8kHz and the pulse duration τ=0.1Ts
Soln: Ts= 1 = 125µs
𝑓𝑠
τ=0.1Ts=0.1×125=12.5µs
𝟏
𝟐𝝉
BW≥ ≥ 40 kHz
Q. For the above signal if rise time is 1% of pulse width, find minimum Tx BW for PWM and PPM? Soln: tr=τ×0,01= 1.25x 10-7
T
B ≥
1
2𝑡
𝑟
≥ 4MHz
Thus BW of PWM/PPM much higher than PAM
Multiplexing
transmission over a shared medium .
Principle used
Four basic types of multiplexing
•Time Division Multiplexing (TDM) • Code Division Multiplexing (CDM)
Frequency Division Multiplex (FDM): Separation of spectrum into smaller frequency.
Example: Multiplexing of telephonic signals from n subscribers
Interference and no useful information.
FDM System
Advantages: No dynamic coordination needed and works also for analog signals
Disadvantages: Waste of bandwidth if traffic distributed uneven; inflexible;
Time Division Multiplexing
Each signal occupies its own distinct time slot, using all frequencies, for the duration of the transmission. Slots may be permanently assigned on demand
Block diagram of TDM and PAM-TDM
rate 1/Ts (ii) To sequentially interleave N samples Inside a sampling interval Ts
Synchronization in TDM system
frame called Markers (highest amplitude)
Marker Pulse
x
1
x2
xN-1
Crosstalk and Guard Times
𝟎.𝟓𝟓
interfere with each other. Thus interference between adjacent TDM channels is crosstalk
practise has a finite BW, known as band limited channels
get mixed with x2(t) and this overlap causes crosstalk.
Transmission Bandwidth for ‘N’ PAM-TDM channels: Nfm Where fm is the maximum frequency of baseband signal Advantages:
Disadvantages
Application of PWM
A very powerful benefit of PWM is that power loss is very minimal. Compared to regulating power levels using an analog potentiometer to limit the power output by essentially choking the electrical pathway, thereby resulting in power loss as heat, PWM actually turns off the power output rather than limits it. Applications range from controlling DC motors and light dimming to heating elements.
This simple circuit based around the familiar NE555 or 7555 timer chip is used to produced the required pulse width modulation signal at a fixed frequency output. The timing capacitor C is charged and discharged by current flowing through the timing networks RA and RB as we looked at in the 555 Timer tutorial.
The output signal at pin 3 of the 555 is equal to the supply voltage switching the transistors fully “ON”. The time taken for C to charge or discharge depends upon the values of RA, RB.
The capacitor charges up through the network RA but is diverted around the resistive network RB and through diode D1. As soon as the capacitor is charged, it is immediately discharged through diode D2 and network RB into pin 7. During the discharging process the output at pin 3 is at 0 V and the transistor is switched “OFF”.
Then the time taken for capacitor, C to go through one complete charge- discharge cycle depends on the values of RA, RB and C with the time T for one complete cycle being given as:
The time, TH, for which the output is “ON” is: TH = 0.693(RA).C
The time, TL, for which the output is “OFF” is: TL = 0.693(RB).C
Total “ON”-“OFF” cycle time given as: T = TH + TL with the output frequency being ƒ = 1/T
With the component values shown, the duty cycle of the waveform can be adjusted from about 8.3% (0.5V) to about 91.7% (5.5V) using a 6.0V power supply. The Astable frequency is constant at about 256 Hz and the motor is switched “ON” and “OFF” at this rate.
Resistor R1 plus the “top” part of the potentiometer, VR1 represent the resistive network of RA. While the “bottom” part of the potentiometer plus R2 represent the resistive network of RB above.
These values can be changed to suite different applications and DC motors but providing that the 555 Astable circuit runs fast enough at a few hundred Hertz minimum, there should be no jerkiness in the rotation of the motor.
Diode D3 is our old favourite the flywheel diode used to protect the electronic circuit from the inductive loading of the motor. Also if the motor load is high put a heatsink on the switching transistor or MOSFET.
Pulse width modulation is a great method of controlling the amount of power delivered to a load without dissipating any wasted power. The above circuit can also be used to control the speed of a fan or to dim the brightness of DC lamps or LED’s. If you need to control it, then use Pulse Width Modulation to do it.