(i) Let the two modulating signals Am1sinωm1t and Am2sinωm2t be superimposed on carrier signal
Acsimωct. The signal produced is x(t)=Am1sinωm1t+Am2sinωm2t+Acsinωct
To produce amplitude modulated wave the signal x(t) is passed through a square law device which produces
an output given by
$$y(t)=B[A_{m_1}sinω_{m_1}+A_{m_2}sinω_{m_2}t+A_csinω_ct]+C[A_{m_1}sinω_{m_1}t+A_{m_2}sinω_{m_2}t+A_csimω_ct]^2$$
$$B=[A_{m_1}sinω_{m_1}t+A_{m_2}sinω_{m_2}t+A_csinω_ct]+C[(A_{m_1}sinω_{m_1}t+A_{m_2}sinω_{m_2}t)2+A^2_csin^2ω_ct$$
$$+2A_csinω_ct(A_{m_1}sinω_{m_1}t+A_{m_2}sinω_{m_2}t)]$$
$$=B[A_{m_1}sinω_{m_1}t+A_{m_2}sinω_{m_2}t+A_csinω_ct]$$
$$+C[A^2_{m_1}sin^2ω_{m_1}t+A^2_{m_2}sin^2ω_{m_2}t+2A_{m_1}A_{m_2}sinω_{m_1}tsinω_{m_2}t$$
$$+A^2_csin^2ω_ct+2A_c(A_{m_1}sinω_{m_1}tsinω_ct+Am^2sinω_{m_2}tsinω_ct)]$$
$$=B[A{m_1}sinω_{m_1}t+A_{m_2}sinω_{m_2}t+A_csinω_ct]$$
$$+C[A^2_{m_1}sin^2ω_{m_1}t+A^2_{m_2}sin^2ω_{m_2}t+A_{m_1}A_{m_2}{cos(ω_{m_2}−ω_{m_1})t−cos(ω_{m_2}+ω_{m_1})}+A^2_csin^2ω_ct$$
$$+A_cA_{m_1}{cos(ω_c−ω_{m_1})t−cos(ω_c+ω_{m_1})t}+A_cA_{m_2}{cos(ω_c−ω_{m_2})t−cos(ω_c+ω_{m_2})t}]$$
In the above amplitude modulated waves, the frequencies present are
$$ω_{m_1},ω_{m_2},ω_c,(ω_{m_2}−ω_{m_1}),(ω_{m_2}+ω_{m_1}),(ω_c−ω_{m_1}),(ω_c+ω_{m_1}),(ω_c−ω_{m_2}) and (ω_c+ω_{m_2})$$
The plot of amplitude versus ω is shown in
figure
(ii) From figure , we note that frequency
spectrum is not symmetrical about $$ω_c$$.
Crowding of spectrum is present for $$ω<ω_c.$$
(iii) if more waves are to be modulated then
there will be more crowding in the modulating
signal in the region $$ω<ω_c.$$ That will result
more chances of mixing of signals.
(iv) To accommodate more signals, we should increase band width and frequency of carrier waves $$ω_c$$. This
shows that large carrier frequency enables to carry more information (i.e., more $$ω_m$$) and the same will
inturn increase band width.
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