17-Phys-B4 Signals and Communications · December 2016
Question 6 of 6: VCO-Based FM Modulator — Output Expression, Demodulation, Carson Bandwidth
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. 98-Phys-B4 Communications, National
Examination December 2016 — a three-hour closed-book examination (a standard
non-programmable, no-text-storage calculator is the only aid permitted). The cover
page states any five of the six questions constitute a complete
paper, with only the first five as they appear in the answer book marked; every
question is nonetheless answered in full below so the paper remains a complete
study resource. All six questions carry equal value.
Reference texts. A. V. Oppenheim and A. S. Willsky, Signals
and Systems, 2nd ed. (Fourier series, sampling, z-transform); S. Haykin and
M. Moher, Communication Systems, 5th ed. (AM/DSB/FM modulation, PCM,
mixers and frequency conversion); B. P. Lathi and Z. Ding, Modern Digital and
Analog Communication Systems, 4th ed. (envelope detection, Carson's rule);
J. G. Proakis and D. G. Manolakis, Digital Signal Processing, 4th ed.
(z-transform stability, partial-fraction inversion).
Question 6: VCO-Based FM Modulator — Output Expression, Demodulation, Carson Bandwidth (1/6 of paper)
Given. VCO characteristic: a straight line through
$(f,V)=(f_c,0)$ with slope $dV/df=10^{-4}\text{ V/Hz}$. Modulator output power
$=10$ (part a). Message bandwidth $W=10\text{ kHz}$, peak value $m_p=2\text{ V}$
(part c).
VCO characteristic: V is
linear in f near f_c, slope dV/df = 10⁻⁴ V/Hz.
Find. (a) FM modulator output $s(t)$ in terms of $m(t)$; (b) a
demodulator block diagram; (c) approximate FM bandwidth.
Approach. Invert the VCO's given $V$-vs-$f$ slope to obtain
its frequency sensitivity $K_v$ (in Hz/V, the quantity that actually drives
instantaneous frequency); write the standard FM instantaneous-phase expression
using $K_v\,m(t)$ as the frequency-deviation term, with amplitude set by the
given output power; choose a standard FM discriminator for the demodulator; and
apply Carson's rule with the peak deviation $K_v\times$(peak of $m$).
Part (a) — FM modulator output. The given slope is
$dV/df=10^{-4}\text{ V/Hz}$ (volts needed per hertz of shift); the VCO's
frequency SENSITIVITY is its reciprocal,
$$K_v=\frac{df}{dV}=\frac{1}{10^{-4}}=\boxed{10^4\text{ Hz/V}}$$
so driving the VCO with $m(t)$ volts produces an instantaneous frequency
$f_i(t)=f_c+K_vm(t)$ and phase $\theta(t)=2\pi f_ct+2\pi K_v\int_0^tm(\lambda)\,d\lambda$.
The output power is $A_c^2/2=10$, so $A_c=\sqrt{20}=2\sqrt5$:
$$s(t)=\boxed{2\sqrt5\,\cos\!\Big[2\pi f_ct+2\pi\!\cdot\!10^4\!\int_0^tm(\lambda)\,d\lambda\Big]}$$
Part (b) — FM demodulator. A standard non-coherent FM
discriminator recovers $m(t)$ without needing a phase-locked local oscillator:
limit the signal to remove amplitude noise/variation, differentiate (which
converts instantaneous-frequency variation into amplitude variation, since
$d\theta/dt=2\pi f_c+2\pi K_vm(t)$), envelope-detect, then low-pass filter to
strip the DC term left by $f_c$:
$$s_{FM}(t)\ \xrightarrow{\text{limiter}}\ \xrightarrow{d/dt}\
\xrightarrow{\text{envelope det.}}\ \xrightarrow{\text{LPF, no dc}}\ \propto m(t)$$
(a PLL-based demodulator, using a second VCO of the same $K_v$ locked to
$s_{FM}(t)$, would be an equally standard alternative.)
Part (c) — approximate FM bandwidth (Carson's rule).
The peak frequency deviation is the VCO sensitivity times the message's peak
value:
$$\Delta f=K_v\times m_p=10^4\text{ Hz/V}\times2\text{ V}=\boxed{20\text{ kHz}}$$
Carson's rule then bounds the FM bandwidth using the message bandwidth
$W=10\text{ kHz}$:
$$BW_{FM}\approx2(\Delta f+W)=2(20+10)\text{ kHz}=\boxed{60\text{ kHz}}$$