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moment, in physics and engineering, term designating the product of a quantity and a distance (or some power of the distance) to some point associated with that quantity. The most theoretically useful moments are moments of masses, areas, lines, and forces, including magnetic force. The concept of torque (propensity to turn about a point) is the moment of force. If a force tends to rotate a body about some point, then the moment, or turning effect, is the product of the force and the distance from the point to the direction of the force. The application of this concept is illustrated by pushing open a door: the farther from the hinge the push is applied, the less force is required. The principle of the moment of a force is perhaps best seen in the use of a lever. Extensions of this concept are important in mechanics, in topics such as inertia, center of gravity, equilibrium, and stability of structures, and in architectural problems. The moment of inertia of a body about a point is the sum, for each particle in the body, of the mass of the particle and the square of its distance from the point. The angular momentum of a body about a fixed axis is equal to the product of the momentum and the length of the moment arm (distance from the body to the axis). A torque acting on a rigid body acts to change its angular momentum by producing an angular acceleration.

The Columbia Electronic Encyclopedia Copyright © 2004.

Licensed from Columbia University Press

Licensed from Columbia University Press

In probability theory and statistics, the moment-generating function of a random variable X is## Calculation

## Significance

## See also

- $M\_X(t)=operatorname\{E\}left(e^\{tX\}right),\; quad\; t\; in\; mathbb\{R\},$

wherever this expectation exists. The moment-generating function generates the moments of the probability distribution.

If X has a continuous probability density function f(x) then the moment generating function is given by

- $M\_X(t)\; =\; int\_\{-infty\}^infty\; e^\{tx\}\; f(x),mathrm\{d\}x$

- $=\; int\_\{-infty\}^infty\; left(1+\; tx\; +\; frac\{t^2x^2\}\{2!\}\; +\; cdotsright)\; f(x),mathrm\{d\}x$

- $=\; 1\; +\; tm\_1\; +\; frac\{t^2m\_2\}\{2!\}\; +cdots,$

where $m\_i$ is the ith moment. $M\_X(-t)$ is just the two-sided Laplace transform of f(x).

Regardless of whether the probability distribution is continuous or not, the moment-generating function is given by the Riemann-Stieltjes integral

- $M\_X(t)\; =\; int\_\{-infty\}^infty\; e^\{tx\},dF(x)$

where F is the cumulative distribution function.

If X_{1}, X_{2}, ..., X_{n} is a sequence of independent (and not necessarily identically distributed) random variables, and

- $S\_n\; =\; sum\_\{i=1\}^n\; a\_i\; X\_i,$

where the a_{i} are constants, then the probability density function for S_{n} is the convolution of the probability density functions of each of the X_{i} and the moment-generating function for S_{n} is given by

- $$

For vector-valued random variables X with real components, the moment-generating function is given by

- $M\_X(mathbf\{t\})\; =\; operatorname\{E\}left(e^\{langle\; mathbf\{t\},\; mathbf\{X\}rangle\}right)$

where t is a vector and $langle\; mathbf\{t\}\; ,\; mathbf\{X\}rangle$ is the dot product.

Provided the moment-generating function exists in an open interval around t = 0, the nth moment is given by

- $operatorname\{E\}left(X^nright)=M\_X^\{(n)\}(0)=left.frac\{mathrm\{d\}^n\; M\_X(t)\}\{mathrm\{d\}t^n\}right|\_\{t=0\}.$

If the moment generating function is finite in such an interval, then it uniquely determines a probability distribution.

Related to the moment-generating function are a number of other transforms that are common in probability theory, including the characteristic function and the probability-generating function.

The cumulant-generating function is the logarithm of the moment-generating function.

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Last updated on Tuesday October 07, 2008 at 16:28:04 PDT (GMT -0700)

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Last updated on Tuesday October 07, 2008 at 16:28:04 PDT (GMT -0700)

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