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Normal Distribution

The normal distribution is a hypothetical symmetrical distribution used to make comparisons among scores or to make other kinds of statistical decisions. The shape of this distribution is often referred to as “bell shaped” or colloquially called the “bell curve.” This shape implies that the majority of scores lie close to the center of the distribution, and as scores drift from the center, their frequency decreases.

Normal distributions belong to the family of continuous probability distributions or probability density functions. A probability density function is a function meant to communicate the likelihood of a random variable to assume a given value. This function is graphed by plotting the variable, x, by the probability of that variable occurring, y. These normal probability distributions are characterized by the aforementioned symmetric bell shape but can have any real mean, labeled µ, and any positive real standard deviation, labeled σ. Specifically, the normal distribution is characterized by continuous data, meaning the data can occupy any range of values. In special cases, the normal distribution can be standardized in which the mean becomes 0 and the standard deviation becomes 1. All normal distributions can be transformed or standardized to the standard normal distribution.

The normal distribution is commonly named the “Gaussian distribution,” after Carl Friedrich Gauss, a German mathematician who made significant advancements of statistical concepts. Less frequently, the normal distribution may be called the “Laplace distribution,” after Pierre-Simon Laplace. The remainder of this entry reviews the history of normal distribution, explains the defining function of normal distribution, explores its properties, highlights the differences between normal distribution and standard normal distribution, and reviews assumptions and tests of normality.

History

The first affiliation with normal distribution stemmed from errors of measurement. Galileo Galilei looked specifically within astronomy to notice that the errors in observations were not random. Small errors far outweighed the larger errors, and these errors had a tendency to be symmetrically distributed around a peak value.

In 1895, Karl Pearson is credited with the first appearance of the term normal distribution from his seminal paper. However, the term also appeared in work by Charles Peirce in 1783, Francis Galton in 1889, and Henri Poincaré in 1893. The first mathematical derivation of the normal distribution is attributed to Abraham DeMoivre in his Approximatio ad summam terminorum binomii (a + b)n in seriem expansi. DeMoivre used integral calculus to estimate a continuous distribution, resulting in a bell-shaped distribution.

In 1808, Robert Adrain, an American mathematician, debated the validity of the normal distribution, expounding on distributions of measurement errors. His discoveries led to further work in proving Adrien-Marie Legendre’s method of least squares. In 1809, without knowledge of Adrain’s work, Gauss published his Theory of Celestial Movement. This work presented substantial contributions to the statistics field, including the method of least squares, the maximum likelihood parameter estimation, and the normal distribution. The significance of these contributions is possibly why Gauss is given credit over Adrain in regard to the normal distribution. In use from 1991 to 2001, the German 10 DM banknote displayed a portrait of Gauss and a graphical display of the normal density function.

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