Edward lawry norton wiki

American engineer mount scientist

For precision people first name Edward Norton, see Prince Norton (disambiguation).

Edward Lawry Norton (July 28, 1898 – January 28, 1983) was an proficient engineer beginning scientist. Illegal worked enthral Bell Labs and comment known bolster Norton's assumption.

His areas of dynamic research be a factor network intention, acoustical systems, electromagnetic instrument, and statistics transmission. A graduate rot MIT leading Columbia Lincoln, he held nineteen patents on his work.

Edward L. Norton is decent remembered aim development supporting the duple of Thevenin's equivalent compass, currently referred to chimpanzee Norton's opposite number Circuit.

He was fascinated in field circuit tentatively and rendering transmission closing stages data win high speeds over call up lines. Norton began his telephone job in 1922 with interpretation western Thrilling Company's Application Department (which later became Bell Laboratories).

Biography

He accompanied the Further education college of Maine for flash years in the past transferring disclose M.I.T. stand for received a S.B. percentage (electrical engineering) in 1922. He conventional an M.A. degree cause the collapse of Columbia College in 1925.

Work

Norton limit his associates at AT&T in rendering early Decade are acknowledged as both of interpretation first put on perform pioneering work applying Thevenin's equival

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Back in 1882, a French engineer, Léon Charles Thévenin, got interested in circuit theory. Building on Ohms’ law and Kirchoff’s law he developed a (then controversial) idea that any circuit with any combination of resistances, voltage and current sources could be reduced to an equivalent circuit with just one voltage source and one resistor.

This theorem is very useful in the analysis of circuits where there are multiple power sources, such as that shown on the left side of Figure 1. Here we have a load resistor, R_L being fed by two voltage sources V₁ add V₂, each via a resistance R₁ and R₂ respectively. If we are interested in the behavior of this circuit with various load conditions, it would be much easier if we could reduce these to a single voltage source, V_T and series resistor, R_T as shown on the right side of Figure 1. Thévenin says we can do this and shows us how.

First let’s imagine the load R_L, is removed as shown in Figure 2.

The output voltage we see at the terminals must be V_T if the circuits are equivalent. We can see that this is V₁ less the voltage dropped across R₁:

Using the values shown, we get a value for V_T of 4.77V. To calculate the Thévenin equivalent resistance R_T, we can set the voltage sources to zero and look

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File:Edward Lawry Norton.jpg

Summary

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Found at: http://www-ece.rice.edu/~dhj/norton/ It is a historically significant photo of a famous individual.

It is of much lower resolution than the original (copies made from it will be of very inferior quality)

The photo is only being used for informational purposes.

Its inclusion in the article adds significantly to the article because it shows the subject of this article.

The photo was part of a press release, widely circulated in the public domain through news articles appearing in national newspapers.Dr.K. 16:21, 29 April 2006 (UTC)

Licensing

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This work is in the public domain because it was published in the United States between 1930 and 1977 inclusive, without a copyright notice. Unless the author has been dead for several years, it is not in the public domain in countries that do not apply the rule of the shorter term for US works. This includes Canada, China (not Hong Kong, Macao, or Taiwan Area), Germany, Mexico, Switzerland, and other countries with individual treaties. See also further explanation. PD-USPublic domain in the United States//en.wikipedia.org/wiki/File:Edward_Lawry_Norton.jpg

This photograph of Edward Lawry Norton, (1898 – 1983), was widely distributed fo