This document discusses frequency modulation (FM) generation and demodulation. It describes how FM can be generated by varying the capacitance in an LC oscillator circuit using a varactor diode, causing the oscillator frequency to vary with the modulating signal. It also discusses Armstrong's indirect method of generating FM by combining a DSB-SC signal with a quadrature carrier. Frequency multiplication is described as a way to increase the frequency deviation of an FM signal. Demodulation of FM signals is also briefly mentioned.

1. FM Modulators & Demodulators
FM Generation by Parameter Variation Method:
• The generator which produces the carrier of an
FM waveform is in many instances a tuned circuit
oscillator.
• Such oscillator circuits furnish a sinusoidal
waveform whose frequency is very largely
determined by and is very nearly equal to the
resonant frequency of an inductance-capacitance
combination.
• Thus the frequency of oscillation is f = 1/(2π√LC) in
which L is the inductance and C the capacitance.

2. • Such an LC combination, a parallel combination in
this case, is shown in Fig.
• The capacitor consists here of a fixed capacitor Co,
which is shunted by a voltage-variable capacitor Cv.
• A voltage-variable capacitor, commonly called a
varicap, is one whose capacitance value depends
on the biasing voltage maintained across its
electrodes.
• Semiconductor diodes, when operated with a
reverse bias, have characteristics suitable to permit
their use as voltage-variable capacitors.

4. • In the circuit of above Fig. the modulating signal
varies the voltage across Cv. As a consequence the
capacitance of Cv changes and causes a
corresponding change in the oscillator frequency,
Ordinarily the modulating frequency is very small in
comparison with the oscillator frequency.
• Therefore the fractional change in Cv may be very
small during the course of many cycles of the
oscillator signal. We may consequently expect that
even with this variable capacitance, the
instantaneous oscillator frequency will be given by
f = (2π√LC)-1 .

5. • Then we have the result that the system suggested
in above Fig will generate an oscillator output signal
whose instantaneous frequency depends on the
instantaneous value of the modulating signal.
• Any oscillator whose frequency is controlled by the
modulating-signal voltage is called a voltage-
controlled oscillator or VCO.
• Frequency modulation may be achieved by the
variation of any element or parameter on which
the frequency depends.
• If the frequency variation is to occur in response to
a modulating signal m(t), then a component must
be available, capacitor, resistor, or inductor, whose
value can be varied with an electrical signal.

6. • Let us now look at a mathematical representation of VCO
by considering this as a block to which a variable voltage
V(t) is input and Vosc(t) output. The block level relation can
be written as
• where, B is the amplitude of the output of VCO and ωc,
the angular frequency in absence of any Frequency
controlling voltage;
• Go is the frequency sensitivity in radian/volt, i.e. rate of
change et instantaneous angular frequency w.r.t. frequency
controlling voltage v(t). Thus, instantaneous angular
frequency

7. • Note that, frequency modulation is achieved if v(t)
is the modulating message signal m(t).
• Thus frequency modulation may be achieved by
the, modulating signal to control these biasing
voltages.
• There is a certain measure of inconsistency in
requiring that a device have long-time frequency
stability and yet be able to respond readily to a
modulating signal.

8. FM Generation by Armstrong's Indirect
Method
• A frequency-modulated waveform in which the
modulating waveform is m(t) is written
cos [ωct +m(t)] if the modulation is narrowband
[|m(t)|« 1], then we may use the approximation
• The term m(t) sin ωct is a DSB-SC waveform in
which m(t) is the modulating waveform and sin
ωct the carrier.

9. • We note that the carrier of the FM waveform, that is cosωct,
and the carrier of the DSB-SC waveform are in quadrature.
We may note in passing that if the two carriers are in phase,
the result is an AM signal since
• A technique used in commercial FM systems to generate
NBFM, which is based on our observation in connection with
above Eq. is shown in below Fig.
• Here a balanced modulator is employed to generate the DSB-
SC signal using sin wave as the carrier of the modulator.
• This carrier is then shifted in phase by 90° and, when added
to the balanced modulator output, thereby forms an NBFM
signal.
• However, the signal so generated will be phase-modulated
rather than frequency-modulated.

11. Frequency Multiplication and Application
to FM:
• A frequency multiplier is a combination of a nonlinear element and
a band pass filter.
• We consider the operation, qualitatively in order to see the relevance
of the process to our present interest of increasing the frequency
deviation of an FM signal.
• Assume that the input signal to the transistor in the circuit of below
Fig. is a periodic signal, possibly sinusoidal but not necessarily so.
• The amplitude of the input signal is large enough and the biasing
(not shown) is such that the transistor operates nonlinearly. Collector
current flows, not continuously but rather in spurts, forming pulses,
one pulse for each cycle of the input driving signal.
• The collector-current waveform has the same fundamental period as
has the driving signal but is rich in higher-frequency harmonics.

12. • The LC parallel resonant circuit is tuned to resonance at the
nth harmonic of the frequency f of the input signal. The
sharpness of the resonance is such that the impedance
presented by the resonant circuit is very small at all
harmonic frequencies except the nth.
• All components of collector current except the component
at frequency of pass through the resonant circuit without
developing appreciable voltage.

13. • However, in response to this nth harmonic current
component, there appears across the resonant
circuit a very nearly sinusoidal voltage waveform of
frequency nf. The resonant circuit serves as a
bandpass filter to selectively single out the nth
harmonic of the driving waveform.
• The process of frequency multiplication performed
by the multiplier under consideration is one in
which a periodic signal of frequency f serves to
generate a second periodic signal of frequency nf,
with n an integer. In principle, we may multiply by
an arbitrary integral number n by simply tuning the
resonant circuit to nf.

14. FM Demodulator