Concept:
For a DSB-full carrier wave, the transmitted power is given by:
\({P_t} = {P_c}\left( {1 + \frac{{{\mu ^2}}}{2}} \right)\)
μ = Modulation index.
pc = Carrier power.
The above expression can be written as:
\({P_t} = {P_c} + \frac{{{P_c}{\mu ^2}}}{2}\)
\(\frac{{{P_c}{\mu ^2}}}{2}\)= Sideband power.
Analysis:
For modulation index ‘μ1’, the ratio of sideband to carrier power will be:
\(\frac{{{P_s}}}{{{P_c}}} = \frac{{{P_c}\mu _1^2}}{{2 \times {P_c}}} = \frac{{\mu _2^2}}{2}\) ---(1)
For μ2 = 2μ1, the ratio will be:
\(\frac{{{P_s}}}{{{P_c}}} = \frac{{{P_c}\mu _2^2}}{{2 \times {P_c}}} = \frac{{\mu _2^2}}{2} = \frac{{4\mu _1^2}}{2}\)
\(\frac{{{P_s}}}{{{P_c}}} = 2\mu _1^2\) ---(2)
Comparing Equations (1) and (2), we conclude that the ratio has increased by a factor of 4.