Modulation is the process of translating a message (information) signal to a different frequency band and increasing its suitability for transmission. In practical communication systems modulation increases the frequency and often the power of the message so that it can be transmitted efficiently over the chosen medium.
Amplitude Modulation (AM) is a family of modulation techniques in which the amplitude of a high-frequency carrier wave is varied in proportion to the instantaneous amplitude of the message (modulating) signal while the carrier frequency and phase remain essentially constant.
The process of AM is illustrated below.

Example context: Audio signals (speech, music) typically occupy low-frequency ranges and are difficult to radiate directly with an antenna. By modulating these audio (message) signals onto a high-frequency carrier, the resulting modulated waveform can be radiated effectively using antennas of practical size and sent over long distances.
Other common modulation types are Frequency Modulation (FM), where the carrier frequency varies with the message, and Phase Modulation (PM), where the carrier phase varies with the message.
Analog refers to quantities that vary continuously with time. In communication:

When a message signal is combined with a carrier signal so that the message information is carried by the resulting waveform, the process is called modulation. The message is effectively "superimposed" on the carrier.
Example: A speech signal has significant energy roughly in 0.3-3.4 kHz. Without modulation two such signals would interfere if transmitted on the same channel. By translating (modulating) each speech signal onto different carrier frequencies (for example around several MHz), many users can share the same physical medium without overlap.
Modulation is required in practical communication systems for several reasons:

The International Telecommunication Union (ITU) designates the common forms of amplitude modulation. The main types are:
The original generic name for amplitude modulation was DSB-AM because two sidebands are normally generated around the carrier.
Modulation may be understood in the frequency domain as multiplication of the message signal by a sinusoidal carrier.
Let the message be a single-tone sinusoid
Vm(t) = Am cos ωm t = Am cos 2π fm t
The message has a spectrum consisting of two impulses at ±fm, each of amplitude Am/2.
Let the carrier be
Vc(t) = Ac cos ωc t
Multiplying the signals in time gives
Vm(t) · Vc(t) = Am Ac cos ωm t · cos ωc t
Using the trigonometric identity cos a cos b = 1/2[cos(a + b) + cos(a - b)], the product contains components at frequencies ωc ± ωm (i.e. fc ± fm) in addition to components at the negatives of those frequencies. Thus the original baseband spectral lines are translated to be centred about the carrier frequency. In general, modulation produces two sideband components around the carrier for each spectral component of the message.

The modulation index (often denoted by m or μ) for amplitude modulation quantifies how much the carrier amplitude varies under modulation. For a message amplitude A (or Am) and carrier amplitude Ac it is
Modulation index = Am / Ac (or m = μ = Am / Ac)
For a modulating signal m(t), when m(t) is normalised so that its peak equals Am, the instantaneous AM waveform is commonly written as
s(t) = Ac [1 + μ m(t)] cos ωc t
where μ must normally satisfy μ ≤ 1 to avoid over-modulation (envelope distortion) when m(t) has amplitude up to unity.
Power efficiency for AM is defined as the ratio of power present in the sidebands (which carry the information) to the total transmitted power (carrier + sidebands):
Efficiency = Ps / Pt
Total power Pt = Pc + Ps, where Pc is carrier power and Ps is total sideband power.
For an AM signal written as s(t) = Ac cos ωc t + Ac μ m(t) cos ωc t, the carrier power is
Pc = Ac2 / 2
If Pm denotes the average power of the modulating signal m(t) (when normalised appropriately), the sideband power can be shown to be
Ps = (Ac2 μ2 / 2) Pm
Thus
Efficiency = (μ2 Pm) / (1 + μ2 Pm)
For single-tone modulation (m(t) = cos ωm t), Pm = 1/2 and the sideband power relative to the carrier leads to the familiar expression for total power
Pt = Pc (1 + μ2/2)
and the maximum theoretical efficiency for conventional DSB-AM with carrier present and single-tone modulation is about 33.33% when μ = 1. For DSB-SC (carrier suppressed) efficiency is higher because the carrier power is not transmitted; SSBSC (single sideband suppressed carrier) can approach 100% efficiency in the ideal case because only the information-bearing sideband is sent.
Example 1: Find the total power of the amplitude modulated signal with a carrier power 400 W and modulation index of 0.8.
Sol.
Use the total power expression for single-tone AM:
Pt = Pc (1 + μ2/2)
Substitute values: Pc = 400 W, μ = 0.8
Pt = 400 × (1 + (0.8)2 / 2)
Pt = 400 × (1 + 0.64 / 2)
Pt = 400 × (1 + 0.32)
Pt = 400 × 1.32
Pt = 528 W
Thus, the total power of the AM signal is 528 watts.
Example 2: What is the maximum efficiency of the single-tone modulation signal?
Sol.
For single-tone modulation the efficiency expression in terms of modulation index μ is
Efficiency = μ2 / (2 + μ2)
Maximum permitted linear modulation without over-modulation is μ = 1.
At μ = 1, Efficiency = 12 / (2 + 12)
Efficiency = 1 / 3
Efficiency = 0.3333 → 33.33%
Hence, the maximum efficiency for single-tone conventional AM (with carrier present) is 33.33%.
This chapter has described the principles of amplitude modulation: why modulation is needed, how modulation translates spectra to higher frequencies, definitions of modulation index and power efficiency, the principal types of AM (DSB, SSB, VSB), historical milestones, and simple numerical examples. Understanding these fundamentals is essential before studying AM transmitter and receiver circuits, demodulation methods (envelope detectors, coherent detection), and advanced topics such as SSB generation and demodulation and bandwidth/power trade-offs in communications engineering.
13 videos|51 docs|30 tests |