In 1975 Nyquist received together with Hendrik Bode the Rufus Oldenburger Medal from the American Society of Mechanical Engineers.[3]

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

His early theoretical work on determining the bandwidth requirements for transmitting information laid the foundations for later advances by Claude Shannon, which led to the development of information theory. In particular, Nyquist determined that the number of independent pulses that could be put through a telegraph channel per unit time is limited to twice the bandwidth of the channel, and published his results in the papers Certain factors affecting telegraph speed (1924)[6] and Certain topics in Telegraph Transmission Theory (1928).[7] This rule is essentially a dual of what is now known as the Nyquist–Shannon sampling theorem.

The Nyquist frequency should not be confused with the Nyquist rate, which is the minimum sampling rate that satisfies the Nyquist sampling criterion for a given signal or family of signals. The Nyquist rate is twice the maximum component frequency of the function being sampled. For example, the Nyquist rate for the sinusoid at 0.6 fs is 1.2 fs, which means that at the fs rate, it is being undersampled. Thus, Nyquist rate is a property of a continuous-time signal, whereas Nyquist frequency is a property of a discrete-time system.

When the function domain is time, sample rates are usually expressed in samples/second, and the unit of Nyquist frequency is cycles/second (hertz). When the function domain is distance, as in an image sampling system, the sample rate might be dots per inch and the corresponding Nyquist frequency would be in cycles/inch.

http://www.wescottdesign.com/articles/Sampling/sampling.pdf

Fig 12.

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