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Frequency Modulation

Switch on an FM radio, pick up a walkie-talkie, or use a wireless microphone, and you are using FM — frequency modulation. The carrier frequency swings up when the audio is positive, swings down when it is negative, and returns to center during silence. FM's defining characteristic — information carried in the carrier's frequency variations rather than its amplitude — gives it properties that make it ideal for high-quality broadcasting and for clear local voice communication: excellent noise immunity, the capture effect, and the ability to use efficient non-linear amplifiers.

What you will learn: How FM encodes information in carrier frequency variations, what frequency deviation means, how to calculate the FM modulation index (deviation ratio), how to use Carson's rule to find FM bandwidth, the difference between NBFM and WBFM, what pre-emphasis and de-emphasis do, the capture effect and why it matters, and how FM discriminators demodulate the signal.

How FM Encodes Information

In frequency modulation, the instantaneous frequency of the carrier is made to deviate from its center frequency in proportion to the instantaneous amplitude (voltage) of the modulating audio signal. The amplitude of the carrier remains constant throughout — it is only the frequency that varies. This is the opposite of AM, where the frequency stays constant and the amplitude varies.

The mathematical description of an FM signal is:

FM signal equation:
v(t) = Vc · sin[2πfct + β·sin(2πfmt)]

Where:
Vc = carrier amplitude (constant — does not change with modulation)
fc = center (carrier) frequency
fm = frequency of the modulating audio signal
β (beta) = modulation index = Δf / fm
Δf = peak frequency deviation from center frequency

To make this concrete: imagine a transmitter set to 146.520 MHz. Without modulation, it transmits exactly 146.520 MHz continuously. When you speak into the microphone and generate a 1,000 Hz audio tone at 2 V peak, the carrier frequency swings from 146.520 MHz upward to 146.5225 MHz (a deviation of +2.5 kHz) and then downward to 146.5175 MHz (a deviation of −2.5 kHz), oscillating between these extremes 1,000 times per second. The center frequency always returns to 146.520 MHz between deviations.

Notice what determines the frequency deviation: it is the amplitude of the audio signal. A louder audio tone causes a larger frequency swing. A quieter tone causes a smaller swing. The rate at which the carrier swings back and forth — the speed of the modulation — is determined by the audio frequency. A 1,000 Hz tone causes the carrier to sweep back and forth 1,000 times per second. A 2,000 Hz tone sweeps the carrier back and forth 2,000 times per second.

Three-panel diagram showing FM modulation. Top panel shows the modulating audio signal — a sine wave with positive peaks labeled loud audio and troughs labeled quiet audio, with an intermediate level labeled normal audio. Middle panel shows the instantaneous frequency of the carrier over time: frequency rises above center when audio is positive (labeled high frequency = compressed cycles), drops below center when audio is negative (labeled low frequency = expanded cycles), and returns to center when audio is zero. Bottom panel shows the actual FM waveform as a time-domain signal with visibly compressed cycles when audio is positive and visibly expanded cycles when audio is negative. Frequency deviation arrows labeled +Δf and -Δf are shown relative to the center frequency line. All three panels share a common time axis.

FM modulation: the audio amplitude (top) controls the instantaneous carrier frequency (middle). The resulting FM waveform (bottom) shows compressed cycles when audio is positive (carrier above center frequency) and expanded cycles when audio is negative (carrier below center frequency). The carrier amplitude remains constant throughout.

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Frequency Deviation

Frequency deviation (symbol Δf, spoken "delta f") is the peak shift of the carrier frequency away from its center frequency, caused by the maximum amplitude of the modulating signal. Deviation is always specified as a peak value (plus or minus), not a peak-to-peak value.

Frequency deviation:
Δf = peak carrier frequency shift from center
Total carrier swing = 2 × Δf (peak-to-peak frequency swing)

At maximum modulation (loudest permissible audio):
fmax = fc + Δf (carrier at its highest frequency)
fmin = fc − Δf (carrier at its lowest frequency)

The deviation is set by the transmitter design and the audio levels. Different FM services use different standard deviation values:

  • Narrow-band FM (NBFM) — two-way and business radio, walkie-talkies: maximum deviation ±2.5 kHz or ±5 kHz depending on channel spacing (±2.5 kHz for 12.5 kHz channels, ±5 kHz for 25 kHz channels), audio bandwidth about 300–3,000 Hz
  • Wireless microphones and in-ear monitors: typically ±40–75 kHz deviation for full-bandwidth audio
  • Commercial narrowband FM (NBFM): ±2.5 kHz or ±5 kHz depending on service and country
  • Wideband FM (WBFM) — broadcast: Maximum deviation ±75 kHz (USA), 75 kHz time constant pre-emphasis

Over-deviation — modulating the transmitter more than the specified maximum deviation — causes the FM signal to exceed its channel allocation. On a 12.5 kHz-spaced radio system, an over-deviated signal spreads into adjacent channels and interferes with other users. The transmitter's deviation is measured by service technicians using a deviation meter or a communications test set, or by looking at the signal on a spectrum analyzer. Broadcast transmitters use audio processors with precise limiters so that deviation never exceeds ±75 kHz.

The FM Modulation Index (Deviation Ratio)

The FM modulation index β (also called the deviation ratio when Δf is the maximum rated deviation and fm is the maximum rated audio frequency) is the ratio of the peak frequency deviation to the modulating audio frequency:

FM modulation index:
β = Δf / fm

Where:
β (beta) = FM modulation index (dimensionless)
Δf = peak frequency deviation (Hz)
fm = frequency of the modulating audio tone (Hz)

Deviation ratio (DR) = Δfmax / fm(max)
(When using maximum rated deviation and maximum audio frequency)

β is not a fixed property of the FM system — it changes depending on both the audio frequency and the audio amplitude (which sets the deviation). For a transmitter with maximum deviation of ±5 kHz:

  • At a 1,000 Hz audio tone at maximum amplitude: β = 5,000 / 1,000 = 5
  • At a 3,000 Hz audio tone at maximum amplitude: β = 5,000 / 3,000 = 1.67
  • At a 1,000 Hz audio tone at half amplitude (2.5 kHz deviation): β = 2,500 / 1,000 = 2.5

The significance of β becomes clear when you examine how FM bandwidth depends on it. Small β (called narrowband FM, or NBFM) produces a signal that is not very different from AM in bandwidth. Large β (called wideband FM, or WBFM) produces a much wider signal but with greatly improved noise performance — a fundamental tradeoff in FM system design called the FM improvement threshold or FM quieting.

Calculator: FM Deviation Ratio

FM Deviation Ratio Calculator

Enter the peak frequency deviation and the audio frequency to calculate the FM modulation index β = Δf / fm.

Result will appear here.

FM Bandwidth and Carson's Rule

Calculating the exact bandwidth of an FM signal requires Bessel functions (discussed briefly in the next section), which give the precise power levels of each sideband pair. For practical engineering purposes, however, an approximation rule developed by John R. Carson in 1922 gives a result accurate enough for most calculations:

Carson's rule for FM bandwidth:
BW = 2 × (Δf + fm)

Or equivalently:
BW = 2 × fm × (β + 1)

Where:
BW = signal bandwidth (Hz) — contains approximately 98% of the signal power
Δf = peak frequency deviation (Hz)
fm = highest audio frequency in the modulating signal (Hz)
β = modulation index = Δf / fm

Carson's rule captures both contributions to FM bandwidth: the frequency deviation (how far the carrier swings) and the audio frequency (how fast it swings). If either increases, the bandwidth increases. A signal with very high deviation but very low audio frequency is still wide (swept far, though slowly). A signal with very high audio frequency but very little deviation is also wide (swept fast, though not far). The bandwidth is dominated by whichever term is larger.

Note that Carson's rule gives the bandwidth containing approximately 98% of the signal's total power. The actual spectrum of an FM signal extends to infinity in theory (the Bessel function series never completely terminates), but the outer sidebands become negligible for practical purposes. For receiver filter design and channel planning, the 98% bandwidth from Carson's rule is the standard specification.

Calculator: FM Bandwidth (Carson's Rule)

FM Bandwidth Calculator (Carson's Rule)

Enter the peak frequency deviation and the highest audio frequency. The bandwidth using Carson's rule is BW = 2 × (Δf + fm).

Result will appear here.
Worked Example 1: A narrow-band FM two-way radio (±5 kHz deviation)

Given: Δf = 5,000 Hz (±5 kHz deviation), fm = 3,000 Hz (3 kHz audio)

β = Δf / fm = 5,000 / 3,000 = 1.67
BW = 2 × (5,000 + 3,000) = 2 × 8,000 = 16,000 Hz = 16 kHz

This 16 kHz signal fits comfortably in a 25 kHz channel (the traditional two-way radio channel spacing). With the newer 12.5 kHz channel spacing, deviation is reduced to ±2.5 kHz:
BW = 2 × (2,500 + 3,000) = 2 × 5,500 = 11,000 Hz = 11 kHz — fits in 12.5 kHz.

Worked Example 2: FM broadcast station (88–108 MHz)

Given: Δf = 75,000 Hz (±75 kHz deviation), fm = 15,000 Hz (15 kHz audio for music)

β = 75,000 / 15,000 = 5
BW = 2 × (75,000 + 15,000) = 2 × 90,000 = 180,000 Hz = 180 kHz

FM broadcast stations are spaced 200 kHz apart in the US (100 kHz in some other countries) to accommodate this 180 kHz signal width.
Two-panel spectrum diagram comparing NBFM and WBFM. Left panel labeled NBFM two-way radio (Δf=5 kHz, fm=3 kHz): shows FM signal centered on fc with total bandwidth labeled 16 kHz by Carson's rule arrow spanning the signal; multiple sideband pairs visible close to the carrier. Right panel labeled WBFM broadcast (Δf=75 kHz, fm=15 kHz): shows much wider FM signal with bandwidth labeled 180 kHz by Carson's rule arrow; many more sideband pairs visible extending far from carrier. Both panels show the signal power envelope curving from center outward. Frequency axis has markers at fc, fc±Δf (peak deviation), and fc±BW/2 (Carson rule edge). White background, © Ham Radio Base lower right.

FM spectrum comparison using Carson's rule. Left: NBFM two-way radio with ±5 kHz deviation and 3 kHz audio gives 16 kHz total bandwidth. Right: WBFM broadcast with ±75 kHz deviation and 15 kHz audio gives 180 kHz total bandwidth. The multiple spectral lines are Bessel function sideband pairs; Carson's rule gives the bandwidth envelope containing ~98% of total signal power.

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NBFM vs WBFM

FM systems are broadly categorized as narrowband (NBFM) or wideband (WBFM) based on their modulation index and resulting bandwidth:

Parameter NBFM (two-way radio) WBFM (Broadcast)
Peak deviation Δf ±2.5 kHz to ±5 kHz ±75 kHz
Audio bandwidth 300–3,000 Hz (voice) 50–15,000 Hz (music)
Modulation index β 0.5–5 (typically ~1.7 for ±5/3k) 5 (75k/15k)
Carson's rule bandwidth 11–16 kHz 180 kHz
Channel spacing 12.5–25 kHz 200 kHz (US)
Audio quality Intelligible voice High-fidelity music
FM improvement Moderate noise reduction Large noise reduction (higher β)
Spectrum efficiency Higher (narrow channels) Lower (wide channels)

The trade-off between NBFM and WBFM illustrates a fundamental principle of FM: wider deviation provides better noise performance (the FM improvement factor), but at the cost of more bandwidth. FM broadcast stations accept 200 kHz of channel spacing (and about 180 kHz of signal bandwidth) because the resulting audio quality and noise performance are excellent for music. Two-way radios accept the narrower audio quality of NBFM because the goal is intelligible speech and fitting as many channels as possible into a limited band.

The Bessel Functions: FM Sidebands in Detail

Unlike AM, which produces exactly three spectral components (carrier, USB, LSB) for a single audio tone, FM produces theoretically infinite sideband pairs for any non-zero modulation index. The amplitude of each sideband pair is determined by Bessel functions of the first kind, denoted Jn(β), where n is the sideband order and β is the modulation index.

The FM sideband structure consists of:

  • A component at the carrier frequency fc with amplitude J0(β)
  • First-order sidebands at fc ± fm with amplitude J1(β)
  • Second-order sidebands at fc ± 2fm with amplitude J2(β)
  • Third-order sidebands at fc ± 3fm with amplitude J3(β)
  • And so on to infinity...

Several important things to note about the Bessel function behavior:

The carrier power changes with modulation index. Unlike AM, where the carrier power is always Pc regardless of modulation depth, the FM carrier component's amplitude is J0(β), which actually goes to zero at certain values of β (approximately β = 2.40, 5.52, 8.65...). At these special values of β, all of the signal's power is in the sidebands — the carrier disappears. This is useful in laboratory tests and in certain communications systems, but is worth knowing because it means FM's spectral structure is fundamentally different from AM's.

Total power is constant. Unlike AM, where the total transmitted power increases with modulation depth, FM modulation does not change the total transmitted power. The carrier amplitude is constant. What FM does is redistribute the constant total power among the carrier and an increasing number of sidebands as β increases. This is why FM transmitters can use more efficient (Class C or Class D) output amplifiers — the output amplitude never changes, so there is no need for the linear amplifiers required by AM or SSB.

For practical purposes you do not need to memorize the Bessel function values. Carson's rule gives a good approximation to the signal bandwidth, and the key understanding is simply that FM produces multiple sideband pairs, unlike AM's single pair. The Bessel functions do explain one useful trick: at a modulation index of 2.405 the carrier component disappears completely, which lets technicians set deviation precisely by watching the carrier vanish on a spectrum analyzer.

The Capture Effect

One of FM's most distinctive and useful properties is the capture effect (also called the FM capture effect): when two FM signals on the same frequency arrive at a receiver simultaneously, the receiver tends to lock onto only the stronger signal and almost completely ignore the weaker one. This is fundamentally different from AM behavior, where two AM signals add linearly at the receiver and both are heard simultaneously (with a mixture of the two audio contents).

The capture effect arises from the way FM limiters work. The FM receiver contains a limiter stage that strips away all amplitude variations from the received signal, passing only the frequency variations to the discriminator. When two signals of different amplitudes are present, they combine to produce a complex signal that appears to the limiter approximately as the stronger signal with some frequency variations imposed by the weaker signal. The limiter, by stripping amplitude variations, also strips most of the weaker signal's contribution — effectively "capturing" the receiver for the stronger station.

The capture effect is approximately 6 dB: if one FM signal is 6 dB stronger than a co-channel interferer, the receiver will capture the stronger signal and provide a nearly interference-free output. Below 6 dB difference, capture is not complete and both signals degrade. Above 10–12 dB difference, capture is essentially perfect and the weaker signal is virtually inaudible.

Block diagram and graph showing the FM capture effect. Left side shows two FM transmitters TX1 (strong signal) and TX2 (weak signal) with their signals combining at a receiver antenna. Right side shows a graph with x-axis labeled Signal ratio (dB) from minus 20 to plus 20 dB and y-axis labeled Audio output quality (0 to 100%). Three curves plotted: Captured signal quality rises from 0 at minus 6 dB to 95% at plus 6 dB; Interfering signal quality falls from 95% at minus 6 dB to near zero at plus 6 dB. A vertical dashed line at 0 dB marks equal signal strength. The region between minus 6 and plus 6 dB is shaded and labeled Capture region — degraded reception. Above plus 6 dB is labeled Clean capture of strong signal. Below minus 6 dB is labeled Captured by interferer. White background, © Ham Radio Base lower right.

The FM capture effect: when two signals share a frequency, FM receivers lock onto the stronger one. With approximately 6 dB difference, capture is essentially complete — the weaker signal is almost inaudible. Within 6 dB of equal strength, both signals degrade each other. This behavior differs fundamentally from AM, where both signals are always heard simultaneously.

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In practice, the capture effect is both beneficial and occasionally problematic:

  • Beneficial: If two transmitters are on the same frequency — two walkie-talkie users talking at once, or a distant FM station on the same channel as a local one — the receiver captures the stronger signal. Listeners hear clean audio from one station rather than a garbled mix of two.
  • Problematic: A stronger unwanted signal captures the receiver completely, so a weaker wanted signal can disappear without warning. This is why aviation radio still uses AM, where two simultaneous transmissions are both heard.
  • Critical for safety: This is why aviation VHF uses AM rather than FM — in an emergency, multiple aircraft and ground stations may transmit simultaneously on the same frequency with safety-critical information. With FM, only the strongest would be heard. With AM, all transmissions add at the receiver and all are audible.

Pre-Emphasis and De-Emphasis

FM has a characteristic noise spectrum that creates a practical problem: the noise at the FM discriminator output increases linearly with audio frequency. High audio frequencies suffer more from FM noise than low audio frequencies. This is an inherent property of the FM discriminator — the noise floor after demodulation rises at 6 dB per octave as you go from low to high audio frequencies.

The standard engineering solution is pre-emphasis at the transmitter and de-emphasis at the receiver:

Pre-emphasis: Before the audio reaches the FM modulator, it passes through a high-pass filter (technically an RC network that boosts high frequencies). This intentionally over-emphasizes (amplifies) the high audio frequencies before transmission, boosting them relative to the low frequencies. The standard pre-emphasis time constant in the United States is 75 microseconds (abbreviated 75 μs), which is defined as the RC time constant of the pre-emphasis network. (Europe and most of the rest of the world uses 50 μs for mono broadcast, but US broadcast uses 75 μs.) The pre-emphasis begins rising at 1/(2π × 75×10−6) ≈ 2,120 Hz.

De-emphasis: At the receiver, after FM demodulation, the audio passes through a complementary low-pass filter with the same 75 μs time constant, which rolls off the high frequencies back to their natural levels. Because the FM noise spectrum also rises at high frequencies, and the de-emphasis filter rolls off at exactly the same rate, the de-emphasis filter cuts the noise as well as cutting the boosted high frequencies — resulting in a flat audio response with significantly reduced high-frequency noise compared to a system without pre-emphasis/de-emphasis.

Graph showing pre-emphasis and de-emphasis frequency response curves. Horizontal axis labeled Frequency (Hz) from 20 Hz to 20 kHz logarithmic scale. Vertical axis labeled Relative level (dB) from minus 20 dB to plus 20 dB. Three curves plotted: red curve labeled Pre-emphasis (75 μs) shows flat response below 2,120 Hz and rising response above (+6 dB/octave slope), reaching about +17 dB at 15 kHz; blue curve labeled De-emphasis (75 μs) shows flat response below 2,120 Hz and falling response above (minus 6 dB/octave), reaching about minus 17 dB at 15 kHz; green flat line labeled Recovered audio after de-emphasis shows flat 0 dB response across the full audio band. Vertical dashed line at 2,120 Hz labeled f = 1/(2π × 75 μs). Note: combined pre-emphasis plus de-emphasis gives flat response.

Pre-emphasis (75 μs) boosts high audio frequencies at the transmitter by up to 17 dB at 15 kHz. De-emphasis at the receiver applies the complementary roll-off, restoring a flat audio response while also reducing high-frequency FM noise. The combined effect of pre-emphasis + de-emphasis provides a flat audio response from 20 Hz to 20 kHz.

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Pre-emphasis time constants are standardized: 75 μs in the Americas and South Korea, and 50 μs in Europe and most other regions, for FM broadcasting. Two-way radios use a similar 6 dB/octave pre-emphasis over the speech band. If the transmitter and receiver use different time constants, the system still works but the audio sounds slightly dull or slightly bright. FM receiver chips apply the correct de-emphasis automatically, and it is rarely something the user needs to adjust.

FM Demodulation

FM demodulation — recovering the audio from the frequency-modulated signal — requires a circuit that converts frequency variations into voltage variations. Several circuit types accomplish this:

The FM Limiter

Before the detector, an FM receiver passes the signal through one or more limiter stages. A limiter is a high-gain amplifier that clips its output at a fixed amplitude regardless of the input amplitude — it acts like a hard clipper. Because FM encodes information only in frequency (not amplitude), clipping the amplitude does no harm to the information content but dramatically reduces amplitude noise, especially impulse noise from lightning and electrical equipment. After limiting, the signal has constant amplitude with only frequency variations — the pure FM signal the detector was designed for.

The Slope Detector

The simplest FM detector tunes an LC circuit slightly off the FM center frequency, on the slope of the resonance curve. As the FM signal's frequency varies above and below center, the signal moves up and down the slope of the resonance, converting frequency variations into amplitude variations. An envelope detector then recovers the audio from the resulting AM-like signal. The slope detector has poor linearity and low efficiency, but illustrates the basic principle of FM-to-AM conversion.

The Foster-Seeley Discriminator

The Foster-Seeley discriminator uses a special transformer arrangement to produce two voltages whose difference is proportional to the frequency offset from the center frequency. At center frequency, the two voltages are equal and their difference is zero (no audio output). Above center, one voltage rises and the other falls; below center, the reverse occurs. The differential output, after rectification and filtering, gives the recovered audio. The Foster-Seeley discriminator requires a limiter stage before it.

The Ratio Detector

The ratio detector is similar to the Foster-Seeley but includes a large storage capacitor that suppresses amplitude variations — it provides some of its own AM rejection without requiring a separate limiter stage. Ratio detectors were common in high-quality FM broadcast receivers from the 1950s through the 1980s because they combined amplitude rejection and FM detection in one stage. They have slightly higher harmonic distortion than the Foster-Seeley discriminator.

The Phase-Locked Loop (PLL) FM Detector

Modern FM receivers, including the single-chip FM radios in phones and the receivers in two-way radios, use either a phase-locked loop or a digital demodulator after an analog-to-digital converter. In a PLL detector, the VCO tracks the incoming FM signal's frequency. As the FM signal's frequency swings above and below center, the error voltage that drives the VCO to track it is proportional to the frequency deviation — this error voltage is the demodulated audio. PLL detectors offer excellent linearity, low distortion and wide bandwidth, and need no tuned coils.

Where FM Is Used

FM is the standard for high-quality analog broadcasting and for local voice communication:

  • FM broadcasting (88–108 MHz): wide-band FM with ±75 kHz deviation, stereo carried on a 38 kHz subcarrier with a 19 kHz pilot tone, and RDS station-name data on a 57 kHz subcarrier.
  • Two-way radio: walkie-talkies, business, public-safety and marine VHF radios use narrow-band FM. Many systems switch between talk groups using sub-audible tones (CTCSS, 67–254 Hz) or digital codes (DCS) added to the audio, so that a receiver only opens its squelch for the right users.
  • Wireless microphones and in-ear monitors: wide-deviation FM with companding gives near-broadcast audio quality.
  • Analog TV sound, baby monitors, cordless phones and FM transmitters for car stereos all used or use FM.
  • Data: frequency-shift keying (FSK) and Gaussian FSK (GFSK) — the digital form of FM — carry Bluetooth, many 433/868/915 MHz sensor links and pagers, as described in the Digital Modulation Overview lesson.
FM key facts summary:
  • FM varies the carrier frequency; carrier amplitude remains constant throughout
  • Frequency deviation Δf = peak shift from center frequency, set by audio amplitude
  • FM modulation index β = Δf / fm
  • Carson's rule: BW = 2 × (Δf + fm) — contains ~98% of total signal power
  • Two-way radio NBFM: Δf = ±5 kHz, BW ≈ 16 kHz; FM broadcast WBFM: Δf = ±75 kHz, BW ≈ 180 kHz
  • Capture effect: FM receivers lock onto the stronger of two co-channel signals
  • Pre-emphasis (75 μs USA) boosts high frequencies at transmitter; de-emphasis restores flat response at receiver and reduces noise
  • FM demodulators include the slope detector, Foster-Seeley discriminator, ratio detector, and PLL detector

Frequently Asked Questions

If FM has constant carrier amplitude, can I use a Class C power amplifier for FM?

Yes, and this is one of FM's important practical advantages. Class C amplifiers are highly efficient (typically 70–80%) but they are non-linear — they distort signals whose amplitude varies. Because FM carries its information only in frequency variations (not amplitude), a Class C amplifier preserves the FM information perfectly while offering much higher efficiency than the Class A or AB amplifiers required for AM or SSB. This is why FM transmitters — and the GFSK transmitters in battery-powered Bluetooth devices — use efficient saturated amplifiers, and why FM handheld radios get long battery life.

What is "deviation" and how is it checked?

Deviation is the amount the carrier frequency shifts from its center frequency at the loudest audio. Narrow-band two-way radios use ±5 kHz for 25 kHz channel spacing or ±2.5 kHz for 12.5 kHz spacing; FM broadcasting uses ±75 kHz. Service technicians check it with a deviation meter or a communications test set, or on a spectrum analyzer using the Bessel-null method. The audio level into the modulator controls deviation — too high causes over-deviation and splatter into adjacent channels, too low makes the signal sound quiet and muffled.

Why does FM sound better than AM for local communication even at lower power?

FM's noise advantage comes from two sources. First, the limiter strips amplitude noise (which is where most man-made interference — vehicle ignition, power lines, light switches — appears). Second, FM's capture effect means that once the signal is a few dB above the noise floor, the receiver locks onto it cleanly. AM signals, by contrast, must compete with amplitude noise at all times because the envelope detector cannot distinguish between amplitude variations from modulation and amplitude variations from noise. Once FM is above the FM improvement threshold (typically 10–15 dB signal-to-noise at the input of the discriminator), its output signal-to-noise ratio jumps dramatically — much better than AM at the same signal level. Below the threshold, FM falls off a cliff and becomes unusable; above the threshold, it sounds excellent.

What does CTCSS actually look like on the air — does it change the FM signal?

CTCSS (Continuous Tone-Coded Squelch System) adds a sub-audible tone — typically 67 Hz to 254 Hz — to the audio being transmitted. This tone appears below the normal voice audio range (which starts at about 300 Hz) and is inaudible to most people even if the receiver's de-emphasis filter does not completely remove it. The tone modulates the FM carrier along with the voice, causing a very small additional frequency deviation (typically ±0.5 kHz or less for the tone). It is not a digital signal but a pure continuous sine wave at a specific frequency. A receiver using CTCSS has a narrow band-pass filter tuned to the CTCSS frequency to detect the tone, and only opens the audio path when the correct tone is continuously present. CTCSS does not significantly affect the FM signal's spectrum or operation; it simply adds a small constant-amplitude tone to the pre-existing audio mix.

Can a narrow-band FM receiver receive FM broadcast stations?

Only poorly. Even if a two-way radio or scanner can tune to 88–108 MHz, its IF filter and demodulator are designed for ±5 kHz deviation in a 12.5 or 25 kHz channel. A broadcast signal with ±75 kHz deviation swings far outside that filter, so the receiver only reproduces the parts of the waveform that happen to fall inside it, and the audio is badly distorted. Receivers that cover both, such as many scanners, switch to a wide IF filter and a wide-band demodulator in their broadcast-FM mode.

Test Your Knowledge

Answer the questions below to check your understanding. Every answer can be found in the lesson above.

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