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Harry Nyquist

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Harry Nyquist
Harry Nyquist
Born(1889-02-07)February 7, 1889
Nilsby, Stora Kil, Värmland, Sweden
DiedApril 4, 1976(1976-04-04) (aged 87)
Harlingen, Texas, U.S.
CitizenshipSwedish / American
Alma materYale University
University of North Dakota
Known forNyquist–Shannon sampling theorem
Nyquist rate
Johnson–Nyquist noise
Nyquist stability criterion
Nyquist ISI criterion
Nyquist plot
AwardsIEEE Medal of Honor (1960)
Stuart Ballantine Medal (1960)
Rufus Oldenburger Medal (1975)
Scientific career
FieldsElectronic engineer
InstitutionsBell Laboratories
Henry Andrews Bumstead

Harry Theodor Nyquist (/ˈnaɪkwɪst/, Swedish: [ˈnŷːkvɪst]; February 7, 1889 – April 4, 1976) was a Swedish-American physicist and electronic engineer who made important contributions to communication theory.[1]

Personal life

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Harry Theodor Nykvist was born on 7 February 1889 in the village of Nilsby, in the Stora Kil parish [sv], Värmland, Sweden. He was the fourth of eight children born to Lars Jonsson Nyqvist (1847–1930) and Catarina (or Katrina) Eriksdotter (1857–1920).[2][3] He immigrated to the United States in 1907.[4] At Southern Minnesota Normal College he met Antonia Wachlin, whom he would later marry and have four children with.[3][5] Nyquist lived in Pharr, Texas after his retirement, and died in Harlingen, Texas on April 4, 1976.[4][5]

Education

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He entered the University of North Dakota in 1912 and received B.S. and M.S. degrees in electrical engineering in 1914 and 1915, respectively. He received a Ph.D. in physics at Yale University in 1917.[3]

Career

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After receiving his doctorate, Nyquist joined AT&T in 1917. He worked in its transmission research organization, studying telegraph, picture, and voice transmission. In 1934 he moved to Bell Telephone Laboratories, where his work broadened from transmission engineering to communications systems. In 1954 he retired, having served as Assistant Director of Systems Studies.[6]

During his time at the Bell system he received 138 patents and published twelve technical papers.[3][6]

Nyquist formally retired in 1954 but continued for several years as a part-time consultant on communications problems for the Bell System and federal agencies.[7]

Technical contributions

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Memorial to Harry Nyquist at the University of North Dakota's College of Engineering and Mines

Nyquist's work at the Bell System addressed practical problems in telegraphy, long-distance telephony, carrier telephony, facsimile, and television. Market growth required more efficient use of wire circuits and the available bandwidth. Stable repeaters, accurate carrier generation, and control of noise and distortion were required. His work on those problems led to advances in communication theory, the understanding of thermal noise, feedback stability, and phase and frequency control.[3]

Telegraph transmission and communication theory

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Telegraph service growth was an issue for the Bell System. More messages had to be sent over the lines, and those lines were also needed for telephone service. Increasing the signaling rate made pulses smear into adjacent time intervals, while sharp pulses occupied a wide frequency range and interfered with other circuits. The problem was therefore not simply how fast a telegraph key could operate, but how much information could be carried through a limited frequency band.[8]

Wozencraft and Jacobs placed the beginnings of communication theory in Nyquist’s 1924 publication, where he showed that the number of independently resolvable pulses that could be transmitted through a band-limited channel was proportional to the product of that bandwidth and of transmission time. They described Ralph Hartley’s 1928 work as extending this result by considering the accuracy with which received signal levels could be distinguished.[9]

In “Certain Factors Affecting Telegraph Speed” (1924), Nyquist examined both the shape of the transmitted signal and the choice of the code. He showed that rectangular pulses and half-cycle sine waves were (generally) not the most efficient waveforms, and that shaping pulses before transmission increased signaling speed and limited interference with other signals. He compared binary with multilevel codes, showing that the information conveyed increased logarithmically with the number of available signal values. Noise and distortion limited how many levels could be distinguished reliably.[8]

Nyquist also worked on making telegraph performance measurable in working telegraph systems. With R. B. Shanck and S. I. Cory, he developed methods for separating distortion into bias, characteristic distortion caused by the transmission path, and random or “fortuitous” distortion. Their paper described instruments and test signals that could be used to measure the lengthening and shortening of marks and spaces and to identify likely faults in lines, repeaters, batteries, and relays.[10]

Nyquist analyzed the underlying theory in the paper “Certain Topics in Telegraph Transmission Theory” (1928). He showed that an ideal channel of bandwidth B could transmit up to 2 B independent signal elements per second. He showed that pulses were not constrained to remain separate or to retain their original shape: they could overlap, provided that the contributions from neighboring pulses were zero at the instants when each signal was sampled. This became the basis of the Nyquist ISI criterion and of later pulse-shaping methods. Nyquist further analyzed transmit shaping and equalization, multilevel signaling in the presence of interference, coherent transmission using in-phase and quadrature carriers, and the bandwidth advantages and limitations of single-sideband and vestigial-sideband transmission.[11]

The 2 B result concerned the rate at which independent elements could be transmitted through the channel. In his 1948 introduction to information theory, Claude Shannon cited Nyquist’s 1924 and 1928 papers, together with work by Ralph Hartley, as important foundations for a general theory of communication.[12]

Long-distance transmission and frequency control

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As communication traffic grew, the Bell System needed to carry more circuits over each individual line. Demand also increased for longer distances without loss of quality. Carrier telephony and carrier telegraphy did this by shifting each conversation or telegraph channel to a different frequency band, and then sending the bands together over the same wires. That solved the capacity problem, but created others. The signal loss on the line varied with frequency and temperature. Repeaters were needed to amplify traffic in both directions, and do so without oscillating. As the distortion accumulated on the line, the contribution of each section of line needed to be small.[13]

Nyquist worked on several parts of this problem. His patents from the 1920s covered an automatic gain regulator in which a motor and relays changed an artificial-line attenuator as line loss varied, a bidirectional repeater intended to cope with unequal lines and reflections, and lattice networks for correcting phase-delay distortion.[14][15][16] These were practical parts of keeping signal level, timing, and waveform under control over a long route.[14]

Carrier systems also had to reproduce their carrier frequencies accurately at distant terminals. In a single-sideband system, the carrier was suppressed at the transmitting end and generated again at the receiver. Any error in the locally generated carrier shifted the recovered speech or telegraph signal. As more channels were packed into the system, the allowable frequency error became smaller.[17]

Phase-locked loop frequency control

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In a patent application filed in 1923, Nyquist compared a standard controlling frequency with the output of a motor-driven generator. A balanced vacuum-tube modulator produced a control current determined by the phase difference between them. That current changed the magnetic drag on the generator shaft, adjusting its speed. A separate coarse-frequency mechanism first brought the generator close enough for the phase-control loop to take over.[18] In modern block-diagram terms, the patent shows a reference, phase detector, control path, controlled generator, and feedback- all the elements of a phase-locked loop.[19]

Histories of the phase-locked loop usually begin instead with Henri de Bellescize’s 1932 paper on synchronous radio reception.[19][20] His circuit, like Nyquist’s, combined electronic and electromechanical control. Nyquist returned to the same problem in a 1931 patent application for synchronizing radio transmitters, using a phase-sensitive system to lock a higher-frequency oscillator to a lower-frequency reference.[21]

A related phase-locking arrangement was used in the Bell System Type L coaxial carrier system. A reference received from the transmitting terminal and a quadrature signal derived from the local oscillator drove the two windings of a synchronous motor. Through a reduction gearbox, the motor adjusted a variable capacitor in the tuned circuit of a crystal oscillator. The gearbox integrated the phase error and retained its position if the reference was interrupted, providing frequency holdover.[22]

Thermal noise

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John Bertrand Johnson and Nyquist had known each other since their student days at the University of North Dakota and later became colleagues in the Bell System.[23] In 1928 Johnson measured random voltage fluctuations in resistances and showed that they increased with temperature and resistance.[24] Johnson later recalled that, after discussions with Nyquist, Nyquist developed the formula explaining the effect within “a month or so”.[25]

Nyquist's theoretical explanation appeared immediately after Johnson's paper in the same issue of Physical Review. Using the thermodynamics of a transmission line, he derived the relationship between noise, absolute temperature, resistance, and bandwidth.[26] The effect, now known as Johnson–Nyquist noise, established a fundamental noise floor for amplifiers, receivers, and electrical measuring systems rather than a defect that could be removed through better components or construction.[27]

Feedback and stability

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Carrier telephony depended on chains of repeater amplifiers. As more channels were placed on a circuit and routes became longer, small amounts of distortion and gain variation in each vacuum-tube amplifier accumulated from one repeater to the next. Harold Stephen Black, another Bell Laboratories engineer, spent much of the 1920s looking for a way to make amplifiers sufficiently linear. In 1927, he conceived the negative-feedback amplifier. The attendant reduction in gain produced a much larger reduction in distortion and made the amplifier less sensitive to changes in its components and operating conditions, such as temperature and voltage.[28][29]

Negative feedback introduced a different problem. The gain and phase shift of an amplifier and its feedback path changed with frequency. At some frequency, a signal intended to oppose the input could instead reinforce it, causing the amplifier to oscillate. Black built and field-tested working amplifiers, but wider use of large amounts of feedback required a mathematical analysis to determine whether a proposed circuit would remain stable.[13]: 61–71 

Nyquist addressed this problem in his 1932 paper “Regeneration Theory”. He represented the gain and phase around the feedback loop as a curve in the complex plane and showed how the curve indicated whether the closed-loop system would be stable.[30] The result became known as the Nyquist stability criterion. Black used Nyquist's analysis in his 1934 presentation of the theory and measured performance of stabilized feedback amplifiers.[31] Black supplied the amplifier principle; Nyquist supplied a general test that allowed engineers to apply it reliably.[13]: 61–71 

Facsimile and television transmission

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AT&T also wanted to use telephone lines to carry pictures. Herbert E. Ives led its early work on telephotography, which was publicly demonstrated in 1924 and offered commercially the following year.[32] Picture transmission was less tolerant of faults than ordinary speech. A change in line loss that was heard only as a modest change in volume could appear as bands of incorrect shading in a photograph, while unequal delay at different frequencies blurred edges and fine detail. Nyquist worked on both problems. A picture-transmission patent filed with Alva B. Clark and Danforth K. Gannett described nonlinear conversion of picture brightness into line current, reducing the visible effect of changes in line attenuation. It also included phase equalization to prevent blurring caused by different frequency components arriving at different times.[33]

In 1930, Nyquist and S. Brand described methods for measuring group delay, using the derivative of phase shift with frequency, which they called envelope delay. They applied the measurements to actual telephone circuits and noted that lines adequate for speech could require phase correction for telephotography, broadcast programs, and especially television.[34] Nyquist later patented a television receiver that used feedback to correct the nonlinear response of its light source and amplifier as the required image bandwidth increased.[35]

Nyquist later returned to a problem he had first studied in telegraphy: how much of a modulated signal could be removed without losing useful information. In 1940, he and K. W. Pfleger compared picture transmission using one and two sidebands. With the same overall bandwidth, the single-sideband system carried finer picture detail. Its quadrature component made the detected electrical waveform appear badly distorted, but the photographs were affected much less than the waveform suggested. They also found that maintaining a small transmitted current for the darkest parts of the picture reduced the visible error.[36]

Awards and legacy

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Nyquist received the IRE Medal of Honor in 1960 for his contributions to the understanding of thermal noise, data transmission, and negative feedback. The same year, the Franklin Institute awarded him the Stuart Ballantine Medal for his theoretical and practical work in communications. He received the National Academy of Engineering Founders Award in 1969 and shared the 1975 Rufus Oldenburger Medal with Hendrik Wade Bode.[37][3]

Nyquist was also remembered for encouraging the work of other Bell Laboratories researchers. In ''The Idea Factory'', Jon Gertner reported that Bell patent lawyers found that many of the laboratory's most productive inventors regularly ate with Nyquist. One colleague recalled that “he drew people out, got them thinking”.[38] In Sweden, his contributions to telecommunications have been highlighted alongside those of inventor Lars Magnus Ericsson.[39] Nyquist was profiled on a Sveriges Radio P1 program called "Ett bortglömt geni" (transl. A forgotten genius).[40]

Terms named for Harry Nyquist

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References

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  1. ^ "Harry Nyquist". Physics Today. 29 (6): 64. June 1976. Bibcode:1976PhT....29f..64.. doi:10.1063/1.3023534.
  2. ^ "Sveriges befolkning 1900" [CD-ROM]: Nyqvist, Harry
  3. ^ a b c d e f "Harry Nyquist [Pioneer in CAS]". IEEE Circuits and Systems Magazine. 22 (1): 77–78. 2022. doi:10.1109/MCAS.2022.3142690. ISSN 1558-0830.
  4. ^ a b "Dr. Harry Nyquist, retired scientist". The Item of Millburn and Short Hills. April 8, 1976. p. 9. Retrieved June 18, 2026 – via Newspapers.com.
  5. ^ a b "Mrs. Antonia Louise Nyquist". The Monitor. April 16, 1971. p. 3. Retrieved June 18, 2026 – via Newspapers.com.
  6. ^ a b Brittain, James E. (August 2010). "Electrical Engineering Hall of Fame: Harry Nyquist". Proceedings of the IEEE. 98 (8): 1535–1537. doi:10.1109/JPROC.2010.2053872.
  7. ^ Bode, H. (December 1977). "Obituary statement: Harry Nyquist". IEEE Transactions on Automatic Control. 22 (6): 897–898. doi:10.1109/TAC.1977.1101666. ISSN 0018-9286.
  8. ^ a b Nyquist, H. (April 1924). "Certain Factors Affecting Telegraph Speed 1". Bell System Technical Journal. 3 (2): 324–346. doi:10.1002/j.1538-7305.1924.tb01361.x.
  9. ^ Wozencraft, John M.; Jacobs, Irwin M. (1965). Principles of Communication Engineering. New York: John Wiley & Sons. p. 2. ISBN 0-471-96240-6.
  10. ^ Nyquist, H.; Shanck, R. B.; Cory, S. I. (January 1927). "Measurement of Telegraph Transmission". Transactions of the American Institute of Electrical Engineers. XLVI: 367–376. doi:10.1109/T-AIEE.1927.5061365. ISSN 0096-3860.
  11. ^ Nyquist, H. (April 1928). "Certain Topics in Telegraph Transmission Theory". Transactions of the American Institute of Electrical Engineers. 47 (2): 617–644. doi:10.1109/T-AIEE.1928.5055024. ISSN 0096-3860.
  12. ^ Shannon, C. E. (July 1948). "A mathematical theory of communication". The Bell System Technical Journal. 27 (3): 379–423. doi:10.1002/j.1538-7305.1948.tb01338.x. ISSN 0005-8580.
  13. ^ a b c A History of Engineering and Science in the Bell System: Transmission Technology (1925–1975). Bell Telephone Laboratories. 1985. ISBN 978-0-932764-08-9.
  14. ^ a b US1580624A, Nyquist, Harry; Bouton, Lewis L. & Shoffstall, Hugh F., "Gain-control circuits for repeaters", issued April 13, 1926 
  15. ^ US1592883A, Barton, Henry A. & Nyquist, Harry, "Repeater for transmission lines", issued July 20, 1926 
  16. ^ US1675460A, Nyquist, Harry, "Distortion compensator", issued July 3, 1928 
  17. ^ Crane, R. E.; Dixon, J. T.; Huber, G. H. (January 1947). "Frequency Division Techniques for a Coaxial Cable Network". Transactions of the American Institute of Electrical Engineers. 66 (1): 1451–1459. doi:10.1109/T-AIEE.1947.5059597. ISSN 0096-3860.
  18. ^ US1647192A, Nyquist, Harry, "Apparatus for controlling the frequency of an alternating current", issued November 1, 1927 
  19. ^ a b Gardner, Floyd M. (1979). Phaselock Techniques (2nd ed.). John Wiley & Sons. p. 2. ISBN 978-0-471-04294-5.
  20. ^ Best, Roland E. (2007). Phase-Locked Loops: Design, Simulation, and Applications (6th ed.). McGraw-Hill. p. 5. ISBN 978-0-07-149375-8.
  21. ^ US1926169A, Nyquist, Harry, "Phase and frequency control", issued September 12, 1933 
  22. ^ Crane, R. E.; Dixon, J. T.; Huber, G. H. (January 1947). "Frequency Division Techniques for a Coaxial Cable Network". Transactions of the American Institute of Electrical Engineers. 66 (1): 1451–1459. doi:10.1109/T-AIEE.1947.5059597.
  23. ^ Åström, Karl J. (2022). "Harry Nyquist". IEEE Circuits and Systems Magazine. 22 (1): 77–78. doi:10.1109/MCAS.2022.3142690.
  24. ^ Johnson, J. B. (July 1, 1928). "Thermal Agitation of Electricity in Conductors". Physical Review. 32 (1): 97–109. Bibcode:1928PhRv...32...97J. doi:10.1103/PhysRev.32.97.
  25. ^ Johnson, J. B. (February 1971). "Electronic noise: The first two decades". IEEE Spectrum. 8 (2): 42–46. doi:10.1109/MSPEC.1971.5217957.
  26. ^ Nyquist, H. (July 1, 1928). "Thermal Agitation of Electric Charge in Conductors". Physical Review. 32 (1): 110–113. Bibcode:1928PhRv...32..110N. doi:10.1103/PhysRev.32.110.
  27. ^ Iivanainen, Joonas; Mäkinen, Antti J.; Zetter, Rasmus; Zevenhoven, Koos C. J.; Ilmoniemi, Risto J.; Parkkonen, Lauri (July 22, 2021). "A general method for computing thermal magnetic noise arising from thin conducting objects". Journal of Applied Physics. 130 (4). doi:10.1063/5.0050371. ISSN 0021-8979. Archived from the original on September 8, 2025.
  28. ^ Black, Harold S. (December 1977). "Inventing the negative feedback amplifier". IEEE Spectrum. 14 (12): 54–60.
  29. ^ Kline, Ronald R. (August 1993). "Harold Black and the negative-feedback amplifier". IEEE Control Systems Magazine. 13 (4): 82–85. doi:10.1109/37.229565.
  30. ^ Nyquist, H. (January 1932). "Regeneration Theory". Bell System Technical Journal. 11 (1): 126–147. doi:10.1002/j.1538-7305.1932.tb02344.x.
  31. ^ Black, H. S. (January 1934). "Stabilized Feedback Amplifiers". Bell System Technical Journal. 13 (1): 1–18. doi:10.1002/j.1538-7305.1934.tb00652.x.
  32. ^ "Herbert E. Ives". Optica. Retrieved June 19, 2026.
  33. ^ US1691147A, Clark, Alva B.; Nyquist, Harry & Gannett, Danforth K., "Electrical picture-transmitting system", issued November 13, 1928 
  34. ^ Nyquist, H.; Brand, S. (July 1930). "Measurement of Phase Distortion". Bell System Technical Journal. 9 (3): 522–549. doi:10.1002/j.1538-7305.1930.tb03215.x.
  35. ^ US2031728A, Nyquist, Harry, "Electrooptical system", issued February 25, 1936 
  36. ^ Nyquist, H.; Pfleger, K. W. (January 1940). "Effect of the Quadrature Component in Single Sideband Transmission". Bell System Technical Journal. 19 (1): 63–73. doi:10.1002/j.1538-7305.1940.tb03131.x. ISSN 0005-8580.
  37. ^ "Rufus Oldenburger Medal". American Society of Mechanical Engineers. Retrieved February 21, 2013.
  38. ^ Gertner, Jon (2012). The Idea Factory: Bell Labs and the Great Age of American Innovation. Penguin Press. p. 135. ISBN 978-1-59420-328-2.
  39. ^ "Värmländskt geni fann lyckan i Amerika" [Genius from Värmland found success in America]. Dagens Nyheter. April 1, 2004. p. 41.
  40. ^ "Harry Nyquist - ett bortglömt geni" [Harry Nyquist - a forgotten genius]. Sveriges Radio. April 1, 2004. Retrieved June 20, 2026.
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