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Measure


The terms "measure," "measurable," etc. have very precise technical definitions (usually involving sigma-algebras) that can make them appear difficult to understand. However, the technical nature of the definitions is extremely important, since it gives a firm footing to concepts that are the basis for much of analysis (including some of the slippery underpinnings of calculus).

For example, every definition of an integral is based on a particular measure: the Riemann integral is based on Jordan measure, and the Lebesgue integral is based on Lebesgue measure. The study of measures and their application to integration is known as measure theory.

A measure is defined as a nonnegative real function from a delta-ring πŸ‘ F
such that

where πŸ‘ emptyset
is the empty set, and

for any finite or countable collection of pairwise disjoint sets πŸ‘ (A_n)
in πŸ‘ F
such that πŸ‘ A= union A_n
is also in πŸ‘ F
.

If πŸ‘ F
is πŸ‘ sigma
-finite and πŸ‘ m
is bounded, then πŸ‘ m
can be extended uniquely to a measure defined on the πŸ‘ sigma
-algebra generated by πŸ‘ F
.

πŸ‘ m
is said to be a probability measure on a set πŸ‘ X
if πŸ‘ m(X)=1
and πŸ‘ F
is a πŸ‘ sigma
-algebra.

In the usual definition of a probability measure (or, more precisely a nontrivial πŸ‘ sigma
-additive measure), a measure is a real-valued function πŸ‘ mu
on the Power Set πŸ‘ P(S)
of an infinite set πŸ‘ S
that satisfies the following properties:

1. πŸ‘ mu(emptyset)=0
and πŸ‘ mu(S)=1
,

2. If πŸ‘ X subset= Y
then πŸ‘ mu(x)<=mu(Y)
,

3. πŸ‘ mu({a})=0
for all πŸ‘ a in S
(nontriviality),

4. If πŸ‘ X_n,n=0,1,2,...
, are pairwise disjoint, then

(Jech 1997).

A measure πŸ‘ m
may be extended by completion. The subsets of sets with measure zero form a πŸ‘ delta
-ring πŸ‘ G
. By "changing" sets in πŸ‘ F
on a set from πŸ‘ G
, a πŸ‘ delta
-ring πŸ‘ F_c
which is the completion of πŸ‘ F
with respect to πŸ‘ m
is obtained.

The measure πŸ‘ m
is called complete if πŸ‘ F=F_c
. If πŸ‘ m
is not complete, it may be extended to πŸ‘ F_c
by setting πŸ‘ m((A\B) union (B\A))=m(A)
, where πŸ‘ A in F
and πŸ‘ B in G
.


See also

Almost Everywhere, Borel Measure, Ergodic Measure, Euler Measure, Gauss Measure, Haar Measure, Hausdorff Measure, Helson-SzegΓΆ Measure, Integral, Jordan Measure, Lebesgue Measure, Liouville Measure, Mahler Measure, Measurable Space, Measure Algebra, Measure Space, Minkowski Measure, Natural Measure, Probability Measure, Radon Measure, Wiener Measure Explore this topic in the MathWorld classroom

Portions of this entry contributed by Allan Cortzen

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References

Czyz, J. Paradoxes of Measures and Dimensions Originating in Felix Hausdorff's Ideas. Singapore: World Scientific, 1994.Jech, T. J. Set Theory, 2nd ed. Berlin: Springer-Verlag, p. 295, 1997.

Referenced on Wolfram|Alpha

Measure

Cite this as:

Cortzen, Allan and Weisstein, Eric W. "Measure." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/Measure.html

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