Showing posts with label Thapathali Campus. Show all posts
Showing posts with label Thapathali Campus. Show all posts

Standard AM, FM and PM Equations

Standard Mathematical Equations for AM, FM and PM

1. Amplitude Modulation (AM)

  • : Carrier amplitude, : Carrier frequency
  • :  Message signal amplitude, : Message signal frequency
  • : Modulation index
  • : Carrier Power, : Sideband Power, : Total Power
  • : Efficiency
  • : Bandwidth of the AM signal

Amplitude Modulation

Q. The equation of amplitude modulated wave is given by s(t) = 40[1+0.8cos(2π ×10^3t)]cos(4π×10^5t). Find the carrier power, the total sideband power and bandwidth of the signal. The value of resistor given is 30Ω.
Solution: Here,

We are given:

s(t)=40[1+0.8cos(2π103t)]cos(4π105t)

And:

  • Load resistance R=30ΩR = 30\, \Omega

Step 1: Identify the standard AM form

Standard AM wave:

s(t)=Ac[1+μcos(2πfmt)]cos(2πfct)

From the given equation:

  • Ac=40A_c = 40

  • μ=0.8

  • fm=103=1kHz

  • fc=4π1052π=2×105=200kHz

a) Carrier Power PcP_c

Pc=Ac22R=402230=160060=26.67W​

Frequency Modulation

Q. A single tone FM is represented by the voltage equation as v(t)=12cos(5x10^8t+5sin1250t). Determine following:

a) Carrier frequency

b) Modulating frequency

c) Modulation index

d) Maximum frequency deviation

Solution: Here,

We are given a single-tone FM signal:

v(t)=12cos(5×108t+5sin(1250t))

This equation is in the general form of an FM signal:

v(t)=Accos(2πfct+βsin(2πfmt))

Where:

  • fcf_c = carrier frequency

  • fmf_m = modulating frequency

  • β\beta = modulation index

  • Δf=βfm\Delta f = \beta f_m = frequency deviation

Step-by-step Extraction from Given Equation

We compare:

v(t)=12cos(5×108t+5sin(1250t))

with:

v(t)=Accos(ωct+βsin(ωmt))

From this, we get:

  • ωc=5×108fc=ωc2π=5×1082π79.58×106=79.58MHz\omega_c = 5 \times 10^8 \Rightarrow f_c = \frac{\omega_c}{2\pi} = \frac{5 \times 10^8}{2\pi} \approx 79.58 \times 10^6 = 79.58 \, \text{MHz}

  • ωm=1250fm=12502π199Hz\omega_m = 1250 \Rightarrow f_m = \frac{1250}{2\pi} \approx 199 \, \text{Hz}

  • β=5\beta = 5

Amplitude Modulation

Q. An audio frequency signal 10sin(1000πt) is used for a single tone amplitude modulation with a carrier of 50sin(2π×10^(5)t). Calculate:
(i) Modulation index
(ii) Bandwidth requirement
(iii) Total power delivered if load = 60Ω.

Solution: Here,

We are given:

  • Message signal: m(t)=10sin(1000πt)

  • Carrier signal: c(t)=50sin(2π×105t)

  • Load Resistance: R=60ΩR = 60\, \Omega

Let’s solve the parts step-by-step.

(i) Modulation Index μ\mu

The modulation index is defined as:

μ=AmAc​​

Where:

  • Am=A_m =Amplitude of message = 10

  • Ac= Amplitude of carrier = 50

μ=1050=0.2

So, Modulation Index = 0.2

Analog vs Digital Communication System

Feature

Analog Communication

Digital Communication

Signal Type

Continuous-time (sine wave, etc.)

Discrete-time (binary 0s and 1s)

Noise Immunity

Low (prone to distortion)

High (noise can be detected/corrected)

Bandwidth Requirement

Usually, lower

Usually, higher

Transmission Quality

Degrades with distance

Maintains quality with regeneration

Security

Less secure

More secure (encryption possible)

Cost

Cheaper hardware

Costlier due to encoding/processing

Multiplexing

Frequency Division Multiplexing (FDM)

Time/Frequency/Code Division Multiplexing

Applications

Analog radio, landline telephony

Internet, mobile phones, satellite links

Signal Processing

Harder to analyze and process

Easier (digital circuits, software tools)




Line Spectrum of Signal

Q. Plot the line spectrums of x(t) =12 + 6sin (140πt +30°) - 9cos(80πt-70°).

Solution:

Let’s Analyze and Plot the Line Spectrum of

x(t) = 12 + 6sin(140πt+300) − 9cos(80πt−700)

Step 1: Convert all terms to cosine form

Use the identity: sin(θ) = cos(θ−900)

So,

6sin(140πt+300) = 6cos(140πt−600)

−9cos(80πt−700) = 9cos(80πt+1100)

Thus, x(t) = 12 + 6cos(140πt−600) + 9cos(80πt+1100)

Step 2: Frequencies, Amplitudes, Phases

Term

Frequency (Hz)

Amplitude

Phase

12 (DC)

0

12

6cos(140πt−600)

f=70

6

-60°

9cos(80πt+1100)

f=40

9

+110°

 We split each cosine into two spectral lines at ±f with half the amplitude.