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Frequency modulation

From Wikipedia, the free encyclopedia
(Redirected fromFrequency Modulation)
Electronic method of transmitting information with a carrier wave
For the application of frequency modulation to radio broadcasting, seeFM broadcasting.
"NFM" redirects here. For other uses, seeNFM (disambiguation).
Passbandmodulation
Analog modulation
Digital modulation
Hierarchical modulation
Spread spectrum
See also
Animation of audio, AM and FM signals
A signal may be carried by anAM or FM radio wave.
FM has better noise (RFI) rejection than AM, as shown in this dramatic New York publicity demonstration byGeneral Electric in 1940. The radio has both AM and FM receivers. With a million-voltelectric arc as a source of interference behind it, the AM receiver produced only a roar ofstatic, while the FM receiver clearly reproduced a music program from Armstrong's experimental FM transmitterW2XMN in New Jersey.

Frequency modulation (FM) is asignal modulation technique used in electronic communication, originally for transmitting messages with aradio wave. In frequency modulation acarrier wave is varied in itsinstantaneous frequency in proportion to a property, primarily the instantaneous amplitude, of a message signal, such as anaudio signal.[1] The technology is used intelecommunications,radio broadcasting,signal processing, andcomputing.

Inanalog frequency modulation, such as radio broadcasting of voice and music, the instantaneousfrequency deviation, i.e. the difference between the frequency of the carrier and its center frequency, has a functional relation to the modulating signal amplitude.

Digital data can be encoded and transmitted with a type of frequency modulation known asfrequency-shift keying (FSK), in which the instantaneous frequency of the carrier is shifted among a set of frequencies. The frequencies may represent digits, such as0 and1. FSK is widely used in computermodems such asfax modems, telephonecaller ID systems, garage door openers, and other low-frequency transmissions.[2]Radioteletype also uses FSK.[3]

Frequency modulation is widely used forFM radiobroadcasting. It is also used intelemetry,radar, seismic prospecting, and monitoringnewborns for seizures viaEEG,[4]two-way radio systems,sound synthesis, magnetic tape-recording systems and some video-transmission systems. In radio transmission, an advantage of frequency modulation is that it has a largersignal-to-noise ratio and therefore rejectsradio frequency interference better than an equal poweramplitude modulation (AM) signal. For this reason, most music is broadcast over FM radio.

Frequency modulation andphase modulation are the two complementary principal methods ofangle modulation; phase modulation is often used as an intermediate step to achieve frequency modulation. These methods contrast withamplitude modulation, in which theamplitude of the carrier wave varies, while the frequency and phase remain constant.

Theory

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If the information to be transmitted (i.e., thebaseband signal) isxm(t){\displaystyle x_{m}(t)} and thesinusoidal carrier isxc(t)=Accos(2πfct){\displaystyle x_{c}(t)=A_{c}\cos(2\pi f_{c}t)\,}, wherefc is the carrier's base frequency, andAc is the carrier's amplitude, the modulator combines the carrier with the baseband data signal to get the transmitted signal:[5][citation needed]

y(t)=Accos(2π0tf(τ)dτ)=Accos(2π0t[fc+fΔxm(τ)]dτ)=Accos(2πfct+2πfΔ0txm(τ)dτ){\displaystyle {\begin{aligned}y(t)&=A_{c}\cos \left(2\pi \int _{0}^{t}f(\tau )d\tau \right)\\&=A_{c}\cos \left(2\pi \int _{0}^{t}\left[f_{c}+f_{\Delta }x_{m}(\tau )\right]d\tau \right)\\&=A_{c}\cos \left(2\pi f_{c}t+2\pi f_{\Delta }\int _{0}^{t}x_{m}(\tau )d\tau \right)\\\end{aligned}}}

wherefΔ=KfAm{\displaystyle f_{\Delta }=K_{f}A_{m}},Kf{\displaystyle K_{f}} being the sensitivity of the frequency modulator andAm{\displaystyle A_{m}} being the amplitude of the modulating signal or baseband signal.

In this equation,f(τ){\displaystyle f(\tau )\,} is theinstantaneous frequency of the oscillator andfΔ{\displaystyle f_{\Delta }\,} is thefrequency deviation, which represents the maximum shift away fromfc in one direction, assumingxm(t) is limited to the range ±1.

This process of integrating the instantaneous frequency to create an instantaneous phase is different from adding the modulating signal to the carrier frequency

y(t)=Accos(2π[fc+fΔxm(t)]t){\displaystyle {\begin{aligned}y(t)&=A_{c}\cos \left(2\pi \left[f_{c}+f_{\Delta }x_{m}(t)\right]t\right)\end{aligned}}}

which would result in a modulated signal that has spurious local minima and maxima that do not correspond to those of the carrier.

While most of the energy of the signal is contained withinfc ±fΔ, it can be shown byFourier analysis that a wider range of frequencies is required to precisely represent an FM signal. Thefrequency spectrum of an actual FM signal has components extending infinitely, although their amplitude decreases and higher-order components are often neglected in practical design problems.[6]

Sinusoidal baseband signal

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Mathematically, a baseband modulating signal may be approximated by asinusoidalcontinuous wave signal with a frequencyfm. This method is also named as single-tone modulation. The integral of such a signalxm(t)=cos(2πfmt){\displaystyle x_{m}(t)=cos(2\pi f_{m}t)} is:

0txm(τ)dτ=sin(2πfmt)2πfm{\displaystyle \int _{0}^{t}x_{m}(\tau )d\tau ={\frac {\sin \left(2\pi f_{m}t\right)}{2\pi f_{m}}}\,}

In this case, the expression for y(t) above simplifies to:

y(t)=Accos(2πfct+fΔfmsin(2πfmt)){\displaystyle y(t)=A_{c}\cos \left(2\pi f_{c}t+{\frac {f_{\Delta }}{f_{m}}}\sin \left(2\pi f_{m}t\right)\right)\,}

where the amplitudeAm{\displaystyle A_{m}\,} of the modulatingsinusoid is represented in the peak deviationfΔ=KfAm{\displaystyle f_{\Delta }=K_{f}A_{m}} (seefrequency deviation).

Theharmonic distribution of asine wave carrier modulated by such asinusoidal signal can be represented withBessel functions; this provides the basis for a mathematical understanding of frequency modulation in the frequency domain.

Modulation index

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As in other modulation systems, the modulation index indicates by how much the modulated variable varies around its unmodulated level. It relates to variations in thecarrier frequency:

h=Δffm=fΔ|xm(t)|fm{\displaystyle h={\frac {\Delta {}f}{f_{m}}}={\frac {f_{\Delta }\left|x_{m}(t)\right|}{f_{m}}}}

wherefm{\displaystyle f_{m}\,} is the highest frequency component present in the modulating signalxm(t), andΔf{\displaystyle \Delta {}f\,} is the peak frequency-deviation – i.e. the maximum deviation of theinstantaneous frequency from the carrier frequency. For a sine wave modulation, the modulation index is seen to be the ratio of the peak frequency deviation of the carrier wave to the frequency of the modulating sine wave.

Ifh1{\displaystyle h\ll 1}, the modulation is callednarrowband FM (NFM), and its bandwidth is approximately2fm{\displaystyle 2f_{m}\,}. Sometimes modulation indexh<0.3{\displaystyle h<0.3} is considered NFM and other modulation indices are considered wideband FM (WFM or FM).

For digital modulation systems, for example, binary frequency shift keying (BFSK), where a binary signal modulates the carrier, the modulation index is given by:

h=Δffm=Δf12Ts=2ΔfTs {\displaystyle h={\frac {\Delta {}f}{f_{m}}}={\frac {\Delta {}f}{\frac {1}{2T_{s}}}}=2\Delta {}fT_{s}\ }

whereTs{\displaystyle T_{s}\,} is the symbol period, andfm=12Ts{\displaystyle f_{m}={\frac {1}{2T_{s}}}\,} is used as the highest frequency of the modulating binary waveform by convention, even though it would be more accurate to say it is the highestfundamental of the modulating binary waveform. In the case of digital modulation, the carrierfc{\displaystyle f_{c}\,} is never transmitted. Rather, one of two frequencies is transmitted, eitherfc+Δf{\displaystyle f_{c}+\Delta f} orfcΔf{\displaystyle f_{c}-\Delta f}, depending on the binary state 0 or 1 of the modulation signal.

Ifh1{\displaystyle h\gg 1}, the modulation is calledwideband FM and its bandwidth is approximately2fΔ{\displaystyle 2f_{\Delta }\,}. While wideband FM uses more bandwidth, it can improve thesignal-to-noise ratio significantly; for example, doubling the value ofΔf{\displaystyle \Delta {}f\,}, while keepingfm{\displaystyle f_{m}} constant, results in an eight-fold improvement in the signal-to-noise ratio.[7] (Compare this withchirp spread spectrum, which uses extremely wide frequency deviations to achieve processing gains comparable to traditional, better-known spread-spectrum modes).

With a tone-modulated FM wave, if the modulation frequency is held constant and the modulation index is increased, the (non-negligible) bandwidth of the FM signal increases but the spacing between spectra remains the same; some spectral components decrease in strength as others increase. If the frequency deviation is held constant and the modulation frequency increased, the spacing between spectra increases.

Frequency modulation can be classified as narrowband if the change in the carrier frequency is about the same as the signal frequency, or as wideband if the change in the carrier frequency is much higher (modulation index > 1) than the signal frequency.[8] For example, narrowband FM (NFM) is used fortwo-way radio systems such asFamily Radio Service, in which the carrier is allowed to deviate only 2.5 kHz above and below the center frequency with speech signals of no more than 3.5 kHz bandwidth. Wideband FM is used forFM broadcasting, in which music and speech are transmitted with up to 75 kHz deviation from the center frequency and carry audio with up to a 20 kHz bandwidth and subcarriers up to 92 kHz.

Bessel functions

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Frequency spectrum andwaterfall plot of a 146.52 MHz carrier, frequency modulated by a 1,000 Hz sinusoid. The modulation index has been adjusted to around 2.4, so the carrier frequency has small amplitude. Several strong sidebands are apparent; in principle an infinite number are produced in FM but the higher-order sidebands are of negligible magnitude.

For the case of a carrier modulated by a single sine wave, the resulting frequency spectrum can be calculated usingBessel functions of the first kind, as a function of thesideband number and the modulation index. The carrier and sideband amplitudes are illustrated for different modulation indices of FM signals. For particular values of the modulation index, the carrier amplitude becomes zero and all the signal power is in the sidebands.[6]

Since the sidebands are on both sides of the carrier, their count is doubled, and then multiplied by the modulating frequency to find the bandwidth. For example, 3 kHz deviation modulated by a 2.2 kHz audio tone produces a modulation index of 1.36. Suppose that we limit ourselves to only those sidebands that have a relative amplitude of at least 0.01. Then, examining the chart shows this modulation index will produce three sidebands. These three sidebands, when doubled, gives us (6 × 2.2 kHz) or a 13.2 kHz required bandwidth.

Modulation
index
Sideband amplitude
Carrier12345678910111213141516
0.001.00
0.250.980.12
0.50.940.240.03
1.00.770.440.110.02
1.50.510.560.230.060.01
2.00.220.580.350.130.03
2.404830.000.520.430.200.060.02
2.5−0.050.500.450.220.070.020.01
3.0−0.260.340.490.310.130.040.01
4.0−0.40−0.070.360.430.280.130.050.02
5.0−0.18−0.330.050.360.390.260.130.050.02
5.520080.00−0.34−0.130.250.400.320.190.090.030.01
6.00.15−0.28−0.240.110.360.360.250.130.060.02
7.00.300.00−0.30−0.170.160.350.340.230.130.060.02
8.00.170.23−0.11−0.29−0.100.190.340.320.220.130.060.03
8.653730.000.270.06−0.24−0.230.030.260.340.280.180.100.050.02
9.0−0.090.250.14−0.18−0.27−0.060.200.330.310.210.120.060.030.01
10.0−0.250.040.250.06−0.22−0.23−0.010.220.320.290.210.120.060.030.01
12.00.05−0.22−0.080.200.18−0.07−0.24−0.170.050.230.300.270.200.120.070.030.01

Carson's rule

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Main article:Carson bandwidth rule

Arule of thumb,Carson's rule states that nearly all (≈98 percent) of the power of a frequency-modulated signal lies within abandwidthBT{\displaystyle B_{T}\,} of:

BT=2(Δf+fm)=2fm(h+1){\displaystyle B_{T}=2\left(\Delta f+f_{m}\right)=2f_{m}(h+1)}

whereΔf{\displaystyle \Delta f\,}, as defined above, is the peak deviation of the instantaneous frequencyf(t){\displaystyle f(t)\,} from the center carrier frequencyfc{\displaystyle f_{c}},h{\displaystyle h} is the modulation index which is the ratio of frequency deviation to highest frequency in the modulating signal, andfm{\displaystyle f_{m}\,}is the highest frequency in the modulating signal.Carson's rule can only be applied to sinusoidal signals. For non-sinusoidal signals:

BT=2(Δf+W)=2W(D+1){\displaystyle B_{T}=2(\Delta f+W)=2W(D+1)}

where W is the highest frequency in the modulating signal but non-sinusoidal in nature and D is the Deviation ratio which is the ratio of frequency deviation to highest frequency of modulating non-sinusoidal signal.

Noise reduction

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FM provides improvedsignal-to-noise ratio (SNR), as compared for example withAM. Compared with an optimum AM scheme, FM typically has poorer SNR below a certain signal level called the noise threshold, but above a higher level – the full improvement or full quieting threshold – the SNR is much improved over AM. The improvement depends on modulation level and deviation. For typical voice communications channels, improvements are typically 5–15 dB. FM broadcasting using wider deviation can achieve even greater improvements. Additional techniques, such as pre-emphasis of higher audio frequencies with corresponding de-emphasis in the receiver, are generally used to improve overall SNR in FM circuits. Since FM signals have constant amplitude, FM receivers normally have limiters that remove AM noise, further improving SNR.[9][10]

Implementation

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Modulation

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FM signals can be generated using either direct or indirect frequency modulation:

Demodulation

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See also:Detector (radio) § Frequency and phase modulation detectors
FM modulation

Many FM detector circuits exist. A common method for recovering the information signal is through aFoster–Seeley discriminator orratio detector. Aphase-locked loop can be used as an FM demodulator.Slope detection demodulates an FM signal by using a tuned circuit which has its resonant frequency slightly offset from the carrier. As the frequency rises and falls the tuned circuit provides a changing amplitude of response, converting FM to AM. AM receivers may detect some FM transmissions by this means, although it does not provide an efficient means ofdetection for FM broadcasts.

Insoftware-defined radio implementations, the demodulation may be carried out by using theHilbert transform (implemented as a filter) to recover the instantaneous phase, and thereafter differentiating this phase (using another filter) to recover the instantaneous frequency. Alternatively, a complex mixer followed by a bandpass filter may be used to translate the signal to baseband, and then proceeding as before. For sampled signals, phase detection, and therefore frequency modulation detection, can be approximated by taking the IQ (complex) sample and multiplying it with the complex conjugate of the previous IQ sample,x[n]x[n1]¯{\displaystyle x[n]\cdot {\overline {x[n-1]}}}[12]. If the demodulated signal is sampled at or above Nyquist, this allows for recovery of near-instantaneous phase changes.

Applications

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Doppler effect

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When an echolocatingbat approaches a target, its outgoing sounds return as echoes, which are Doppler-shifted upward in frequency. In certain species of bats, which produce constant frequency (CF)echolocation calls, the bats compensate for theDoppler shift by lowering their call frequency as they approach a target. This keeps the returning echo in the same frequency range of the normal echolocation call. This dynamic frequency modulation is called theDoppler Shift Compensation (DSC), and was discovered byHans Schnitzler in 1968.

Magnetic tape storage

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FM is also used atintermediate frequencies by analogVCR systems (includingVHS) to record theluminance (black and white) portions of the video signal. Commonly, thechrominance component is recorded as a conventional AM signal, using the higher-frequency FM signal asbias. FM is the only feasible method of recording the luminance ("black-and-white") component of video to (and retrieving video from)magnetic tape without distortion; video signals have a large range of frequency components – from a fewhertz to severalmegahertz, too wide forequalizers to work with due to electronic noise below −60 dB. FM also keeps the tape at saturation level, acting as a form ofnoise reduction; alimiter can mask variations in playback output, and theFM capture effect removesprint-through andpre-echo. A continuous pilot-tone, if added to the signal – as was done onV2000 and many Hi-band formats – can keep mechanical jitter under control and assisttimebase correction.

These FM systems are unusual, in that they have a ratio of carrier to maximum modulation frequency of less than two; contrast this with FM audio broadcasting, where the ratio is around 10,000. Consider, for example, a 6-MHz carrier modulated at a 3.5-MHz rate; byBessel analysis, the first sidebands are on 9.5 and 2.5 MHz and the second sidebands are on 13 MHz and −1 MHz. The result is a reversed-phase sideband on +1 MHz; on demodulation, this results in unwanted output at 6 – 1 = 5 MHz. The system must be designed so that this unwanted output is reduced to an acceptable level.[13]

Sound

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FM is also used ataudio frequencies to synthesize sound. This technique, known asFM synthesis, was popularized by early digitalsynthesizers and became a standard feature in several generations ofpersonal computersound cards.

Radio

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Main article:FM broadcasting
An American FM radio transmitter atWEDG in Buffalo, New York

Edwin Howard Armstrong (1890–1954) was an American electrical engineer who invented wideband frequency modulation (FM) radio.[14]He patented the regenerative circuit in 1914, the superheterodyne receiver in 1918 and the super-regenerative circuit in 1922.[15] Armstrong presented his paper, "A Method of Reducing Disturbances in Radio Signaling by a System of Frequency Modulation", (which first described FM radio) before the New York section of theInstitute of Radio Engineers on November 6, 1935. The paper was published in 1936.[16]

As the name implies, wideband FM (WFM) requires a widersignal bandwidth thanamplitude modulation by an equivalent modulating signal; this also makes the signal more robust againstnoise andinterference. Frequency modulation is also more robust against signal-amplitude-fading phenomena. As a result, FM was chosen as the modulation standard for high frequency,high fidelityradio transmission, hence the term "FM radio" (although for many years theBBC called it "VHF radio" because commercial FM broadcasting uses part of theVHF band – theFM broadcast band). FMreceivers employ a specialdetector for FM signals and exhibit a phenomenon known as thecapture effect, in which thetuner "captures" the stronger of two stations on the same frequency while rejecting the other (compare this with a similar situation on an AM receiver, where both stations can be heard simultaneously).Frequency drift or a lack ofselectivity may cause one station to be overtaken by another on anadjacent channel. Frequencydrift was a problem in early (or inexpensive) receivers; inadequate selectivity may affect any tuner.

A wideband FM signal can also be used to carry astereo signal; this is done withmultiplexing and demultiplexing before and after the FM process. The FM modulation and demodulation process is identical in stereo and monaural processes.

FM is commonly used atVHFradio frequencies forhigh-fidelitybroadcasts of music andspeech. In broadcast services, where audio fidelity is important, wideband FM is generally used. Analog TV sound is also broadcast using FM. Narrowband FM is used for voice communications in commercial andamateur radio settings. Intwo-way radio, narrowband FM (NBFM) is used to conserve bandwidth for land mobile, marine mobile and other radio services.

A high-efficiency radio-frequencyswitching amplifier can be used to transmit FM signals (and otherconstant-amplitude signals). For a given signal strength (measured at the receiver antenna), switching amplifiers useless battery power and typically cost less than alinear amplifier. This gives FM another advantage over other modulation methods requiring linear amplifiers, such as AM andQAM.

There are reports that on October 5, 1924, ProfessorMikhail A. Bonch-Bruevich, during a scientific and technical conversation in theNizhny Novgorod Radio Laboratory, reported about his new method of telephony, based on a change in the period of oscillations. Demonstration of frequency modulation was carried out on the laboratory model.[17]

Hearing assistive technology

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Frequency modulated systems are a widespread and commercially availableassistive technology that make speech more understandable by improving the signal-to-noise ratio in the user's ear. They are also calledauditory trainers, a term which refers to any sound amplification system not classified as ahearing aid. They intensify signal levels from the source by 15 to 20 decibels.[18] FM systems are used by hearing-impaired people as well as children whose listening is affected by disorders such asauditory processing disorder orADHD.[19] For people withsensorineural hearing loss, FM systems result in better speech perception than hearing aids. They can be coupled with behind-the-ear hearing aids to allow the user to alternate the setting.[20] FM systems are more convenient and cost-effective than alternatives such ascochlear implants, but many users use FM systems infrequently due to their conspicuousness and need for recharging.[21]

See also

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Wikimedia Commons has media related toFrequency modulation.

References

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  1. ^Smith, Robert H. (1993).Machines and Inventions. Alexandria, VA: Time Life. p. 85.ISBN 0-8094-9704-2.
  2. ^Gibilisco, Stan (2002).Teach yourself electricity and electronics. McGraw-Hill Professional. p. 477.ISBN 978-0-07-137730-0.morse-code frequency-shift-keying sent-using-fsk.
  3. ^Rutledge, David B. (1999).The Electronics of Radio. Cambridge University Press. p. 310.ISBN 978-0-521-64645-1.
  4. ^B. Boashash, editor,Time-Frequency Signal Analysis and Processing – A Comprehensive Reference, Elsevier Science, Oxford, 2003;ISBN 0-08-044335-4
  5. ^Faruque, Saleh (2017).Radio Frequency Modulation Made Easy(PDF). Springer Cham. pp. 33–37.ISBN 978-3-319-41200-9.
  6. ^abT.G. Thomas, S. C. SekharCommunication Theory, Tata-McGraw Hill 2005,ISBN 0-07-059091-5 p. 136
  7. ^Der, Lawrence."Frequency Modulation (FM) Tutorial"(PDF).Silicon Laboratories.S2CID 48672999. Archived fromthe original(PDF) on 2014-10-21. Retrieved17 October 2019.
  8. ^Lathi, B. P. (1968).Communication Systems, pp. 214–17. New York: John Wiley and Sons,ISBN 0-471-51832-8.
  9. ^H. P. Westman, ed. (1970).Reference Data for Radio Engineers (Fifth ed.). Howard W. Sams & Co. pp. 21–11.
  10. ^Alan Bloom (2010). "Chapter 8. Modulation". In H. Ward Silver; Mark J. Wilson (eds.).The ARRL Handbook for Radio Communications. American Radio Relay League. p. 8.7.ISBN 978-0-87259-146-2.
  11. ^Haykin, Simon [Ed]. (2001).Communication Systems, 4th ed.
  12. ^Shima, James Michael (1995).FM Demodulation Using a Digital Radio and Digital Signal Processing. University of Florida.
  13. ^"FM Systems Of Exceptional Bandwidth" Proc. IEEE vol. 112, no. 9, p. 1664, September 1965
  14. ^A. Michael Noll (2001).Principles of modern communications technology. Artech House. p. 104.ISBN 978-1580532846.
  15. ^US 1342885 
  16. ^Armstrong, E. H. (May 1936). "A Method of Reducing Disturbances in Radio Signaling by a System of Frequency Modulation".Proceedings of the IRE.24 (5). IRE:689–740.doi:10.1109/JRPROC.1936.227383.S2CID 43628076.
  17. ^Ф. Лбов.Новая система радиофона «Радиолюбитель». – 1924. – № 6. – С. 86.
  18. ^ASHA Ad Hoc Committee on FM Systems (2002) [Original March 1994].Guidelines for Fitting and Monitoring FM Systems (Technical report) (Revised ed.).American Speech–Language–Hearing Association.doi:10.1044/policy.GL2002-00010.
  19. ^Schafer, Erin C.; Bryant, Danielle; Sanders, Katie; Baldus, Nicole; Algier, Katherine; Lewis, Audrey; Traber, Jordan; Layden, Paige; Amin, Aneeqa (June 1, 2014). "Fitting and Verification of Frequency Modulation on Children with Normal Hearing".Journal of the American Academy of Audiology.25 (6):529–540.doi:10.3766/jaaa.25.6.3.ISSN 1050-0545.PMID 25313543.EBSCOhost 107832936 – viaEBSCOhost.
  20. ^Lewis, M. Samantha; Crandall, Carl C.; Valente, Michael; Enrietto Horn, Jane (2004)."Speech perception in noise: directional microphones versus frequency modulation (FM) systems".Journal of the American Academy of Audiology.15 (6):426–439.doi:10.3766/jaaa.15.6.4.PMID 15341224.
  21. ^McArdle, Rachel; Abrams, Harvey B.; Hnath Chisholm, Theresa (2005). "When Hearing Aids Go Bad: An FM Success Story".Journal of the American Academy of Audiology.16 (10):809–821.doi:10.3766/jaaa.16.10.5.EBSCOhost 106441304 – viaEBSCOhost.

Further reading

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  • Carlson, A. Bruce (2001).Communication Systems. Science/Engineering/Math (4th ed.). McGraw-Hill.ISBN 978-0-07-011127-1.
  • Frost, Gary L. (2010).Early FM Radio: Incremental technology in twentieth-century America. Baltimore, MD: Johns Hopkins University Press.ISBN 978-0-8018-9440-4.
  • Seymour, Ken (2005) [1996]. "Frequency Modulation".The Electronics Handbook (2nd ed.). CRC Press. pp. 1188–1200.ISBN 0-8493-8345-5.

External links

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