A narrowband FM (NBFM) signal, for a single-tone modulation \(m(t) = A_m \cos(\omega_m t)\), can be approximated as:
\( s_{NBFM}(t) \approx A_c \cos(\omega_c t) - A_c \beta \sin(\omega_m t) \sin(\omega_c t) \)
where \(\beta = \frac{k_f A_m}{\omega_m}\) is the modulation index (and \(\beta \ll 1\)).
Using the product-to-sum identity: \(\sin A \sin B = \frac{1}{2}[\cos(A - B) - \cos(A + B)]\).
Let \(A = \omega_c t\) and \(B = \omega_m t\). Using the identity:
\(\sin(\omega_m t) \sin(\omega_c t) = \frac{1}{2}[\cos((\omega_c - \omega_m)t) - \cos((\omega_c + \omega_m)t)]\).
Thus, we get:
\( s_{NBFM}(t) \approx A_c \cos(\omega_c t) - \frac{A_c \beta}{2} [\cos((\omega_c - \omega_m)t) - \cos((\omega_c + \omega_m)t)] \)
Expanding this:
\( s_{NBFM}(t) \approx A_c \cos(\omega_c t) - \frac{A_c \beta}{2} \cos((\omega_c - \omega_m)t) + \frac{A_c \beta}{2} \cos((\omega_c + \omega_m)t) \)
The components of the NBFM signal are:
The LSB is \(+\frac{A_c \beta}{2} \cos((\omega_c - \omega_m)t + \pi)\), which is \(180^\circ\) out of phase with the carrier. The USB is \(+\frac{A_c \beta}{2} \cos((\omega_c + \omega_m)t)\), which is in phase with the carrier (\(0^\circ\)).
The phase differences are \(180^\circ\) for the LSB and \(0^\circ\) for the USB. These phases are not the same, so option (d) is false.
The question asks for the feature that NBFM does *not* have. The correct answer is:
Both sidebands have the same phase difference with respect to the carrier
Final Answer:
Both sidebands have the same phase difference with respect to the carrier