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| − | + | Nyquist's Theorem, also called the Nyquist-Shannon Sampling Theorem, is a theorem in the field of digital signal processing. Nyquist's Theorem is credited to Harry Nyquist and Claude Shannon, though its fundamental discovery was made by E. T. Whittaker '''(WIKIPEDIA-NYQUIST'S THEOREM)'''. In signal processing, there are discrete-time signals and continuous-time signals. When time is viewed as a discrete variable, then any function of time is thought of as having distinct values at separate points in time. In this view, the variable being measured is measured once in each time period between measurements. In many applications, such as tracking the number of shipments each day, time can be considered a discrete variable. However, the physical world presents a different view: time as a continuous variable. When time is a continuous variable, the variable measured over time only has its value for an infinitely small moment in time. The infinite time values cannot all be exactly measured, because instruments of measurement only can make measurements periodically. Therefore, there has to be a jump from the continuous form of time that is apparent in the real world to the discrete form of time used in measurement. Nyquist's Theorem makes this jump. | |
Revision as of 16:23, 5 December 2020
Introduction to Nyquist’s Theorem
Nyquist's Theorem, also called the Nyquist-Shannon Sampling Theorem, is a theorem in the field of digital signal processing. Nyquist's Theorem is credited to Harry Nyquist and Claude Shannon, though its fundamental discovery was made by E. T. Whittaker (WIKIPEDIA-NYQUIST'S THEOREM). In signal processing, there are discrete-time signals and continuous-time signals. When time is viewed as a discrete variable, then any function of time is thought of as having distinct values at separate points in time. In this view, the variable being measured is measured once in each time period between measurements. In many applications, such as tracking the number of shipments each day, time can be considered a discrete variable. However, the physical world presents a different view: time as a continuous variable. When time is a continuous variable, the variable measured over time only has its value for an infinitely small moment in time. The infinite time values cannot all be exactly measured, because instruments of measurement only can make measurements periodically. Therefore, there has to be a jump from the continuous form of time that is apparent in the real world to the discrete form of time used in measurement. Nyquist's Theorem makes this jump.
