Usuària:Viquialcon/proves

Variable aleatòria

Hom defineix variable aleatòria com una funció que assigna un valor numèric real a cadascun dels esdeveniments d'una experiència aleatòria

El conjunt dels valors possibles d'una variable aleatòria se'l coneix com a domini de la variable aleatòria. Quant a la notació, la variable aleatòria se sol indicar amb  $X$(en majúscules) i el valor observat d'aquesta variable aleatòria se sol indicar amb $x_{i}$ (és a dir, en minúscules).

Es diu "aleatòria" perquè el seu domini és constituït pels esdeveniments d'un experiment influït per l'atzar i se'n diu variable perquè pren valors numèrics que varien (o poden variar) d'un esdeveniment a l'altre.

Normalment es fan servir les lletres majúscules, $X,Y,...$per denotar les variables aleatòries.

Per exemple:

Considerem l'experiència aleatòria del llençament de dos daus. El conjunt de resultats possibles d'aquesta experiència és $\Omega =\{(1,1),(1,2),......,(1,6),(2,1),(2,2),(2,3),..........,(6,1),(6,2),.........(6,6)\}$

Podem considerar la variable alatòria $X$ que assigna a cada esdeveniment de l'experiència la suma dels punts dels dos daus, és a dir $X$=suma dels punts dels dos daus.

L'esdeniment {dau1=1 i dau2=3} tindrà assignat el valor real 4 en aquesta variable que hem definit.

En aquest exemple els valors possibles de la variable aleatòria serien:$\{x_{1}=2,x_{2}=3,x_{3}=4,x_{4}=5,x_{5}=6,x_{6}=7,x_{7}=8,x_{8}=9,x_{9}=10,x_{10}=11,x_{11}=12\}$

Tipus de variables aleatòries

Les variables aleatòries poden ser de dos tipus: discretes i contínues.

Una variable aleatòria s'anomena discreta si té un nombre finit de possibles valors, o bé, en cas de tenir-ne infinits com a possibles, si aquests poden ser ordenats seqüencialment(conjunt de valors infinit numerable).

Usualment els valors que pren una variable aleatòria discreta són nombres enters.

Exemples de variables aleatòries discretes

• La que hem vist anteriorment del llençament de dos daus: $X$=suma dels punts dels dos daus.
• La distribució binomial, per les seves aplicacions, és la més important de les distribucions discretes de probabilitat.

Una variable aleatòria s'anomena contínua si els seus possibles valors són tots els nombres reals d'un interval.

Quan treballem amb variables aleatòries que representin alguna mesura física, aquesta podrà prendre valors, teòricament, a tota una escala contínua. A la pràctica el procés efectiu de mesura comportarà una tabulació.

Moltes de les variables d'estudis estadístics reals poden ser formalitzades amb el model d'una variable aleatòria contínua:

• La mesura del temps d'avanç o retard amb què un tren arriba a la seva destinació.
• El pes dels nadons en una població.
• Les alçades de la població adulta.
• La fracció de massa que s'ha desintegrat per unitat de temps en una substància radioactiva.

Per especificar completament una variable aleatòria $X$hom necessita saber:

• El conjunt de possibles valors $x_{i}$
• La probabilitat $p(X=x_{i})$

Distribucions de probabilitat

Observem que cada esdeveniment elemental de l'experiència aleatòria té assignat un valor de la variable aleatòria (en l'exemple del llançament dels dos daus, l'esdeveniment (1,1) té associat el valor 2 de la variable aleatòria) i que diferents esdeveniments elementals poden tenir assignat el mateix valor(en l'exemple del llançament dels dos daus, els esdeveniments (1,2) i (2,1) tenen associat el mateix valor 3 de la variable aleatòria).

Definim com a Distribució de probabilitat d'una variable aleatòria discreta(funció de densitat):

$f(x_{i})=p(X=x_{i})$

La funció de distribució té com a variable independent el valors de la variable aleatòria, per extensió pot ser considerada com una funció real de variable real que té com imatge 0 per als nombres reals que no siguin possibles valors de la variable aleatòria.

Es fa servir el nom de la variable quan es considera la probabilitat que es verifiqui alguns dels esdeveniments, Així, podem escriure, $p(X=2)$per indicar la probabilitat que la variable aleatòria prengui el valor 2.

En l'exemple dels dos daus tenim que, per exemple, $f(x_{1})=p(X=2)=\left({\frac {1}{36}}\right)$perquè l'esdevenivement $[X=2]$té com a únic cas favorable {dau1=1 i dau2=1} i extensivament la funció de distribució vindria definida per:

$f(2)=\left({\frac {1}{36}}\right),f(3)=\left({\frac {2}{36}}\right),f(4)=\left({\frac {3}{36}}\right),f(5)=\left({\frac {4}{36}}\right)$$,f(6)=\left({\frac {5}{36}}\right),f(7)=\left({\frac {6}{36}}\right),f(8)=\left({\frac {5}{36}}\right),$,,,,,,,,,${\textstyle f(12)=\left({\frac {1}{36}}\right)),f(x)=0\quad si\quad x\not \in \{2,3,4,5,6,7,8,9,10,11,12\}}$

Distribució de probabilitat de la variable aleatòria "suma dels valors del llençament de dos daus"

En resum, una variable aleatòria (o estocàstica) és una aplicació mesurable d'un espai de probabilitat $(\Omega ,\mathrm {A} ,p)$en el conjunt dels nombres reals $\Re$:

$(\Omega ,\mathrm {A} ,p)\longrightarrow \Re$

essent Ω el conjunt de resultats possibles de la variable aleatòria, Α el conjunt de successos associats i $p$la funció de probabilitat.

????????Exemple

Si considerem l'experiment aleatori del llançament d'un dau perfecte de sis cares, aleshores

$\Omega =\{1,2,3,4,5,6\}$

i la probabilitat de cada succés elemental és:

$p(1)=p(2)=p(3)=p(4)=p(5)=p(6)=\left({\frac {1}{6}}\right)$

!!!!!!!!!!!La variància és, doncs, el moment central de segon ordre correponent a la variable $X$ centrada i la covariància de la varibañe aleatòria respecte ella mateixahe covariance of the random variable with itself, $\operatorname {Var} (X)=\operatorname {Cov} (X,X).$

${\displaystyle }$

Els paràmetres d'una distribució de probabiliat

Estudiarem dos paràmetres per mesurar numèricament "el centre" i "la dispersió" d'una variable aleatòria .

Mitjana

La mitjana $\mu$ d'una variable aleatòria $X$es defineix en termes de la distribució de probabilitat:

$\mu =\Sigma x_{i}.f(x_{i})$

La suma s'estén a tots els valors $x_{i}$de la variable aleatòria.

En l'exemple dels dos daus val: $\mu =2.\left({\frac {1}{36}}\right)+3.\left({\frac {2}{36}}\right)+...+12.\left({\frac {1}{36}}\right)=7$

La mitjana d'una variable aleatòria rep també el nom de valor esperat (o esperança) i es representa ${\ce {E(X).}}$

Variància

En teoria de la probabilitat i estadística, Variància és un paràmetre estadístic que mesura la dispersió d'una variable aleatòria $X$respecte al seu valor mitjà.

La variància d'una variable aleatòria $X$, és el valor esperat del quadrat del valor esperat de la variable $X$respecte la seva mitjana $\mu =\operatorname {E} [X]$.

La variància es defineix per la fòrmula:

$\operatorname {Var} (X)=\operatorname {E} \left[(X-\mu )^{2}\right]=\Sigma (x_{i}-\mu ).f(x_{i})$

La variància és el quadrat d'una altre paràmetre de dispersió, la desviació tipus $\sigma$, és a dir: $\sigma ^{2}=$ $\operatorname {Var} (X)$.

La variància és representa mitjançant $\operatorname {Var} (X)$, $\sigma _{X}^{2}$, o simplement $\sigma ^{2}$.

La variància té un paper central en: estadística descriptiva, inferència esdística, test d'hipòtesi,... , goodness of fit, mètode Monte Carlo,... És també molt important en les ciències que utilitzen sovint l'anàlisi estadística de les dades.

La variància pot ser també pensada com la covariància de la variable respecte ella mateixa:$\operatorname {Var} (X)=\operatorname {Cov} (X,X).$

La variància és també equivalent a la segona cumulant de la distribució de probabilitat que genera $X$.

L'expressió de la variància es pot desenvolupar:

${\begin{aligned}\operatorname {Var} (X)&=\operatorname {E} \left[(X-\operatorname {E} [X])^{2}\right]\\&=\operatorname {E} \left[X^{2}-2X\operatorname {E} [X]+\operatorname {E} [X]^{2}\right]\\&=\operatorname {E} \left[X^{2}\right]-2\operatorname {E} [X]\operatorname {E} [X]+\operatorname {E} [X]^{2}\\&=\operatorname {E} \left[X^{2}\right]-\operatorname {E} [X]^{2}\end{aligned}}$

Un nmemotècnic per l'expressió anterior és "mitjana del quadrat menys quadrat de la mitjana".

Aquesta equació !!!!!!!!!This equation should not be used for computations using floating point arithmetic because it suffers from catastrophic cancellation if the two components of the equation are similar in magnitude. There exist numerically stable alternatives.

Variable aleatòria discreta

If the generator of random variable $X$ is discrete with probability mass function $x_{1}\mapsto p_{1},x_{2}\mapsto p_{2},\ldots ,x_{n}\mapsto p_{n}$ then

$\operatorname {Var} (X)=\sum _{i=1}^{n}p_{i}\cdot (x_{i}-\mu )^{2},$

or equivalently

$\operatorname {Var} (X)=\left(\sum _{i=1}^{n}p_{i}x_{i}^{2}\right)-\mu ^{2},$

where $\mu$ is the average value, i.e.

$\mu =\sum _{i=1}^{n}p_{i}x_{i}.$

(When such a discrete weighted variance is specified by weights whose sum is not 1, then one divides by the sum of the weights.)

The variance of a set of $n$ equally likely values can be written as

$\operatorname {Var} (X)={\frac {1}{n}}\sum _{i=1}^{n}(x_{i}-\mu )^{2},$

where $\mu$ is the expected value, i.e.,

$\mu ={\frac {1}{n}}\sum _{i=1}^{n}x_{i}.$

The variance of a set of $n$ equally likely values can be equivalently expressed, without directly referring to the mean, in terms of squared deviations of all points from each other:

$\operatorname {Var} (X)={\frac {1}{n^{2}}}\sum _{i=1}^{n}\sum _{j=1}^{n}{\frac {1}{2}}(x_{i}-x_{j})^{2}={\frac {1}{n^{2}}}\sum _{i}\sum _{j>i}(x_{i}-x_{j})^{2}.$

Continuous random variable

If the random variable $X$ represents samples generated by a continuous distribution with probability density function $f(x)$, and $F(x)$ is the corresponding cumulative distribution function, then the population variance is given by

${\begin{aligned}\operatorname {Var} (X)=\sigma ^{2}&=\int (x-\mu )^{2}f(x)\,dx\\&=\int x^{2}f(x)\,dx-2\mu \int xf(x)\,dx+\int \mu ^{2}f(x)\,dx\\&=\int x^{2}\,dF(x)-2\mu \int x\,dF(x)+\mu ^{2}\int \,dF(x)\\&=\int x^{2}\,dF(x)-2\mu \cdot \mu +\mu ^{2}\cdot 1\\&=\int x^{2}\,dF(x)-\mu ^{2},\end{aligned}}$

or equivalently and conventionally,

$\operatorname {Var} (X)=\int x^{2}f(x)\,dx-\mu ^{2},$

where $\mu$ is the expected value of $X$ given by

$\mu =\int xf(x)\,dx=\int x\,dF(x),$

with the integrals being definite integrals taken for $x$ ranging over the range of $X.$

If a continuous distribution does not have a finite expected value, as is the case for the Cauchy distribution, it does not have a variance either. Many other distributions for which the expected value does exist also do not have a finite variance because the integral in the variance definition diverges. An example is a Pareto distribution whose index $k$ satisfies $1<k\leq 2.$

Examples

Normal distribution

The normal distribution with parameters $\mu$ and $\sigma$ is a continuous distribution whose probability density function is given by

$f(x)={\frac {1}{\sqrt {2\pi \sigma ^{2}}}}e^{-{\frac {(x-\mu )^{2}}{2\sigma ^{2}}}}.$

In this distribution, $\operatorname {E} [X]=\mu$ and the variance $\operatorname {Var} (X)$ is related with $\sigma$ via

$\operatorname {Var} (X)=\int _{-\infty }^{\infty }{\frac {x^{2}}{\sqrt {2\pi \sigma ^{2}}}}e^{-{\frac {(x-\mu )^{2}}{2\sigma ^{2}}}}\,dx-\mu ^{2}=\sigma ^{2}.$

The role of the normal distribution in the central limit theorem is in part responsible for the prevalence of the variance in probability and statistics.

Exponential distribution

The exponential distribution with parameter $\lambda$ is a continuous distribution whose support is the semi-infinite interval $[0,\infty )$. Its probability density function is given by

$f(x)=\lambda e^{-\lambda x}$

and it has expected value $\mu =\lambda ^{-1}$. The variance is equal to

$\operatorname {Var} (X)=\int _{0}^{\infty }x^{2}\lambda e^{-\lambda x}\,dx-\mu ^{2}=\lambda ^{-2}.$

So for an exponentially distributed random variable, $\sigma ^{2}=\mu ^{2}.$

Poisson distribution

The Poisson distribution with parameter $\lambda$ is a discrete distribution for $k=0,1,2,\ldots$. Its probability mass function is given by

$p(k)={\frac {\lambda ^{k}}{k!}}e^{-\lambda },$

and it has expected value $\mu =\lambda$. The variance is equal to

$\operatorname {Var} (X)=\left(\sum _{k=0}^{\infty }k^{2}{\frac {\lambda ^{k}}{k!}}e^{-\lambda }\right)-\mu ^{2}=\lambda ,$

So for a Poisson-distributed random variable, $\sigma ^{2}=\mu$.

Binomial distribution

The binomial distribution with parameters $n$ and $p$ is a discrete distribution for $k=0,1,2,\ldots ,n$. Its probability mass function is given by

$p(k)={n \choose k}p^{k}(1-p)^{n-k},$

and it has expected value $\mu =np$. The variance is equal to

$\operatorname {Var} (X)=\left(\sum _{k=0}^{n}k^{2}{n \choose k}p^{k}(1-p)^{n-k}\right)-\mu ^{2}=np(1-p).$

As a simple example, the binomial distribution with $p=1/2$ describes the probability of getting $k$ heads in $n$ tosses of a fair coin. Thus the expected value of the number of heads is $n/2,$ and the variance is $n/4.$

Fair die

A fair six-sided die can be modeled as a discrete random variable, X, with outcomes 1 through 6, each with equal probability 1/6. The expected value of X is $(1+2+3+4+5+6)/6=7/2.$ Therefore, the variance of X is

${\begin{aligned}\operatorname {Var} (X)&=\sum _{i=1}^{6}{\frac {1}{6}}\left(i-{\frac {7}{2}}\right)^{2}\\&={\frac {1}{6}}\left((-5/2)^{2}+(-3/2)^{2}+(-1/2)^{2}+(1/2)^{2}+(3/2)^{2}+(5/2)^{2}\right)\\&={\frac {35}{12}}\approx 2.92.\end{aligned}}$

The general formula for the variance of the outcome, X, of an n-sided die is

${\begin{aligned}\operatorname {Var} (X)&=\operatorname {E} (X^{2})-(\operatorname {E} (X))^{2}\\&={\frac {1}{n}}\sum _{i=1}^{n}i^{2}-\left({\frac {1}{n}}\sum _{i=1}^{n}i\right)^{2}\\&={\frac {(n+1)(2n+1)}{6}}-\left({\frac {n+1}{2}}\right)^{2}\\&={\frac {n^{2}-1}{12}}.\end{aligned}}$

Properties

Basic properties

Variance is non-negative because the squares are positive or zero:

$\operatorname {Var} (X)\geq 0.$

The variance of a constant random variable is zero, and if the variance of a variable in a data set is 0, then all the entries have the same value:

$P(X=a)=1\Leftrightarrow \operatorname {Var} (X)=0.$

Variance is invariant with respect to changes in a location parameter. That is, if a constant is added to all values of the variable, the variance is unchanged:

$\operatorname {Var} (X+a)=\operatorname {Var} (X).$

If all values are scaled by a constant, the variance is scaled by the square of that constant:

$\operatorname {Var} (aX)=a^{2}\operatorname {Var} (X).$

The variance of a sum of two random variables is given by

$\operatorname {Var} (aX+bY)=a^{2}\operatorname {Var} (X)+b^{2}\operatorname {Var} (Y)+2ab\,\operatorname {Cov} (X,Y),$

$\operatorname {Var} (aX-bY)=a^{2}\operatorname {Var} (X)+b^{2}\operatorname {Var} (Y)-2ab\,\operatorname {Cov} (X,Y),$

where Cov(⋅, ⋅) is the covariance. In general we have for the sum of $N$ random variables $\{X_{1},\dots ,X_{N}\}$:

$\operatorname {Var} \left(\sum _{i=1}^{N}X_{i}\right)=\sum _{i,j=1}^{N}\operatorname {Cov} (X_{i},X_{j})=\sum _{i=1}^{N}\operatorname {Var} (X_{i})+\sum _{i\neq j}\operatorname {Cov} (X_{i},X_{j}).$

These results lead to the variance of a linear combination as:

${\begin{aligned}\operatorname {Var} \left(\sum _{i=1}^{N}a_{i}X_{i}\right)&=\sum _{i,j=1}^{N}a_{i}a_{j}\operatorname {Cov} (X_{i},X_{j})\\&=\sum _{i=1}^{N}a_{i}^{2}\operatorname {Var} (X_{i})+\sum _{i\not =j}a_{i}a_{j}\operatorname {Cov} (X_{i},X_{j})\\&=\sum _{i=1}^{N}a_{i}^{2}\operatorname {Var} (X_{i})+2\sum _{1\leq i<j\leq N}a_{i}a_{j}\operatorname {Cov} (X_{i},X_{j}).\end{aligned}}$

If the random variables $X_{1},\dots ,X_{N}$ are such that

$\operatorname {Cov} (X_{i},X_{j})=0\ ,\ \forall \ (i\neq j),$

they are said to be uncorrelated. It follows immediately from the expression given earlier that if the random variables $X_{1},\dots ,X_{N}$ are uncorrelated, then the variance of their sum is equal to the sum of their variances, or, expressed symbolically:

$\operatorname {Var} \left(\sum _{i=1}^{N}X_{i}\right)=\sum _{i=1}^{N}\operatorname {Var} (X_{i}).$

Since independent random variables are always uncorrelated, the equation above holds in particular when the random variables $X_{1},\dots ,X_{n}$ are independent. Thus independence is sufficient but not necessary for the variance of the sum to equal the sum of the variances.

Sum of uncorrelated variables (Bienaymé formula)

Vegeu també: Sum of normally distributed random variables

One reason for the use of the variance in preference to other measures of dispersion is that the variance of the sum (or the difference) of uncorrelated random variables is the sum of their variances:

$\operatorname {Var} \left(\sum _{i=1}^{n}X_{i}\right)=\sum _{i=1}^{n}\operatorname {Var} (X_{i}).$

This statement is called the Bienaymé formula and was discovered in 1853. It is often made with the stronger condition that the variables are independent, but being uncorrelated suffices. So if all the variables have the same variance σ², then, since division by n is a linear transformation, this formula immediately implies that the variance of their mean is

$\operatorname {Var} \left({\overline {X}}\right)=\operatorname {Var} \left({\frac {1}{n}}\sum _{i=1}^{n}X_{i}\right)={\frac {1}{n^{2}}}\sum _{i=1}^{n}\operatorname {Var} \left(X_{i}\right)={\frac {\sigma ^{2}}{n}}.$

That is, the variance of the mean decreases when n increases. This formula for the variance of the mean is used in the definition of the standard error of the sample mean, which is used in the central limit theorem.

To prove the initial statement, it suffices to show that

$\operatorname {Var} (X+Y)=\operatorname {Var} (X)+\operatorname {Var} (Y).$

The general result then follows by induction. Starting with the definition,

${\begin{aligned}\operatorname {Var} (X+Y)&=E[(X+Y)^{2}]-(E[X+Y])^{2}\\&=E[X^{2}+2XY+Y^{2}]-(E[X]+E[Y])^{2}.\\\end{aligned}}$

Using the linearity of the expectation operator and the assumption of independence (or uncorrelatedness) of X and Y, this further simplifies as follows:

${\begin{aligned}\operatorname {Var} (X+Y)&=E[X^{2}]+2E[XY]+E[Y^{2}]-(E[X]^{2}+2E[X]E[Y]+E[Y]^{2})\\&=E[X^{2}]+E[Y^{2}]-E[X]^{2}-E[Y]^{2}\\&=\operatorname {Var} (X)+\operatorname {Var} (Y).\end{aligned}}$

Sum of correlated variables

In general, if the variables are correlated, then the variance of their sum is the sum of their covariances:

$\operatorname {Var} \left(\sum _{i=1}^{n}X_{i}\right)=\sum _{i=1}^{n}\sum _{j=1}^{n}\operatorname {Cov} (X_{i},X_{j})=\sum _{i=1}^{n}\operatorname {Var} (X_{i})+2\sum _{1\leq i<j\leq n}\operatorname {Cov} (X_{i},X_{j}).$

(Note: The second equality comes from the fact that Cov(X_i,X_i) = Var(X_i).)

Here Cov(⋅, ⋅) is the covariance, which is zero for independent random variables (if it exists). The formula states that the variance of a sum is equal to the sum of all elements in the covariance matrix of the components. The next expression states equivalently that the variance of the sum is the sum of the diagonal of covariance matrix plus two times the sum of its upper triangular elements (or its lower triangular elements); this emphasizes that the covariance matrix is symmetric. This formula is used in the theory of Cronbach's alpha in classical test theory.

So if the variables have equal variance σ² and the average correlation of distinct variables is ρ, then the variance of their mean is

$\operatorname {Var} ({\overline {X}})={\frac {\sigma ^{2}}{n}}+{\frac {n-1}{n}}\rho \sigma ^{2}.$

This implies that the variance of the mean increases with the average of the correlations. In other words, additional correlated observations are not as effective as additional independent observations at reducing the uncertainty of the mean. Moreover, if the variables have unit variance, for example if they are standardized, then this simplifies to

$\operatorname {Var} ({\overline {X}})={\frac {1}{n}}+{\frac {n-1}{n}}\rho .$

This formula is used in the Spearman–Brown prediction formula of classical test theory. This converges to ρ if n goes to infinity, provided that the average correlation remains constant or converges too. So for the variance of the mean of standardized variables with equal correlations or converging average correlation we have

$\lim _{n\to \infty }\operatorname {Var} ({\overline {X}})=\rho .$

Therefore, the variance of the mean of a large number of standardized variables is approximately equal to their average correlation. This makes clear that the sample mean of correlated variables does not generally converge to the population mean, even though the law of large numbers states that the sample mean will converge for independent variables.

Matrix notation for the variance of a linear combination

Define $X$ as a column vector of $n$ random variables $X_{1},\ldots ,X_{n}$, and $c$ as a column vector of $n$ scalars $c_{1},\ldots ,c_{n}$. Therefore, $c^{T}X$ is a linear combination of these random variables, where $c^{T}$ denotes the transpose of $c$. Also let $\Sigma$ be the covariance matrix of $X$. The variance of $c^{T}X$ is then given by:

$\operatorname {Var} (c^{T}X)=c^{T}\Sigma c.$

Weighted sum of variables

The scaling property and the Bienaymé formula, along with the property of the covariance Cov(aX, bY) = ab Cov(X, Y) jointly imply that

$\operatorname {Var} (aX\pm bY)=a^{2}\operatorname {Var} (X)+b^{2}\operatorname {Var} (Y)\pm 2ab\,\operatorname {Cov} (X,Y).$

This implies that in a weighted sum of variables, the variable with the largest weight will have a disproportionally large weight in the variance of the total. For example, if X and Y are uncorrelated and the weight of X is two times the weight of Y, then the weight of the variance of X will be four times the weight of the variance of Y.

The expression above can be extended to a weighted sum of multiple variables:

$\operatorname {Var} \left(\sum _{i}^{n}a_{i}X_{i}\right)=\sum _{i=1}^{n}a_{i}^{2}\operatorname {Var} (X_{i})+2\sum _{1\leq i}\sum _{<j\leq n}a_{i}a_{j}\operatorname {Cov} (X_{i},X_{j})$

Product of independent variables

If two variables X and Y are independent, the variance of their product is given by

${\begin{aligned}\operatorname {Var} (XY)&=[E(X)]^{2}\operatorname {Var} (Y)+[E(Y)]^{2}\operatorname {Var} (X)+\operatorname {Var} (X)\operatorname {Var} (Y).\end{aligned}}$

Equivalently, using the basic properties of expectation, it is given by

$\operatorname {Var} (XY)=E(X^{2})E(Y^{2})-[E(X)]^{2}[E(Y)]^{2}.$

Product of statistically dependent variables

In general, if two variables are statistically dependent, the variance of their product is given by:

${\begin{aligned}\operatorname {Var} (XY)&=E[X^{2}Y^{2}]-[E(XY)]^{2}\\&=\operatorname {Cov} (X^{2},Y^{2})+E(X^{2})E(Y^{2})-[E(XY)]^{2}\\&=\operatorname {Cov} (X^{2},Y^{2})+(\operatorname {Var} (X)+[E(X)]^{2})(\operatorname {Var} (Y)+[E(Y)]^{2})-[\operatorname {Cov} (X,Y)+E(X)E(Y)]^{2}\end{aligned}}$

Decomposition

The general formula for variance decomposition or the law of total variance is: If $X$ and $Y$ are two random variables, and the variance of $X$ exists, then

$\operatorname {Var} [X]=\operatorname {E} _{Y}(\operatorname {Var} [X\mid Y])+\operatorname {Var} _{Y}(\operatorname {E} [X\mid Y]).$

where $\operatorname {E} (X|Y)$ is the conditional expectation of $X$ given $Y$, and $\operatorname {Var} (X\mid Y)$ is the conditional variance of $X$ given $Y$. (A more intuitive explanation is that given a particular value of $Y$, then $X$ follows a distribution with mean $\operatorname {E} (X\mid Y)$ and variance $\operatorname {Var} (X\mid Y)$). As $\operatorname {E} (X\mid Y)$ is a function of the variable $Y$, the outer expectation or variance is taken with respect to Y. The above formula tells how to find $\operatorname {Var} (X)$ based on the distributions of these two quantities when $Y$ is allowed to vary.

In particular, if $Y$ is a discrete random variable assuming $y_{1},y_{2},\ldots ,y_{n}$ with corresponding probability masses $p_{1},p_{2},\ldots ,p_{n}$, then in the formula for total variance, the first term on the right-hand side becomes

$\operatorname {E} _{Y}(\operatorname {Var} [X\mid Y])=\sum _{i=1}^{n}p_{i}\sigma _{i}^{2},$

where $\sigma _{i}^{2}=\operatorname {Var} [X\mid y_{i}]$. Similarly, the second term on the right-hand side becomes

$\operatorname {Var} _{Y}(\operatorname {E} [X\mid Y])=\sum _{i=1}^{n}p_{i}\mu _{i}^{2}-\left(\sum _{i=1}^{n}p_{i}\mu _{i}\right)^{2}=\sum _{i=1}^{n}p_{i}\mu _{i}^{2}-\mu ^{2},$

where $\mu _{i}=\operatorname {E} [X\mid y_{i}]$ and $\mu =\sum _{i=1}^{n}p_{i}\mu _{i}$. Thus the total variance is given by

$\operatorname {Var} [X]=\sum _{i=1}^{n}p_{i}\sigma _{i}^{2}+\left(\sum _{i=1}^{n}p_{i}\mu _{i}^{2}-\mu ^{2}\right).$

A similar formula is applied in analysis of variance, where the corresponding formula is

${\mathit {MS}}_{\text{total}}={\mathit {MS}}_{\text{between}}+{\mathit {MS}}_{\text{within}};$

here ${\mathit {MS}}$ refers to the Mean of the Squares. In linear regression analysis the corresponding formula is

${\mathit {MS}}_{\text{total}}={\mathit {MS}}_{\text{regression}}+{\mathit {MS}}_{\text{residual}}.$

This can also be derived from the additivity of variances, since the total (observed) score is the sum of the predicted score and the error score, where the latter two are uncorrelated.

Similar decompositions are possible for the sum of squared deviations (sum of squares, ${\mathit {SS}}$):

${\mathit {SS}}_{\text{total}}={\mathit {SS}}_{\text{between}}+{\mathit {SS}}_{\text{within}},$

${\mathit {SS}}_{\text{total}}={\mathit {SS}}_{\text{regression}}+{\mathit {SS}}_{\text{residual}}.$

Formulae for the variance

Plantilla:Main article A formula often used for deriving the variance of a theoretical distribution is as follows:

$\operatorname {Var} (X)=\operatorname {E} (X^{2})-(\operatorname {E} (X))^{2}.$

This will be useful when it is possible to derive formulae for the expected value and for the expected value of the square.

This formula is also sometimes used in connection with the sample variance. While useful for hand calculations, it is not advised for computer calculations as it suffers from catastrophic cancellation if the two components of the equation are similar in magnitude and floating point arithmetic is used. This is discussed in the article Algorithms for calculating variance.

Calculation from the CDF

The population variance for a non-negative random variable can be expressed in terms of the cumulative distribution function F using

$2\int _{0}^{\infty }u(1-F(u))\,du-{\Big (}\int _{0}^{\infty }(1-F(u))\,du{\Big )}^{2}.$

This expression can be used to calculate the variance in situations where the CDF, but not the density, can be conveniently expressed.

Characteristic property

The second moment of a random variable attains the minimum value when taken around the first moment (i.e., mean) of the random variable, i.e. $\mathrm {argmin} _{m}\,\mathrm {E} ((X-m)^{2})=\mathrm {E} (X)$. Conversely, if a continuous function $\varphi$ satisfies $\mathrm {argmin} _{m}\,\mathrm {E} (\varphi (X-m))=\mathrm {E} (X)$ for all random variables X, then it is necessarily of the form $\varphi (x)=ax^{2}+b$, where a > 0. This also holds in the multidimensional case.

Units of measurement

Unlike expected absolute deviation, the variance of a variable has units that are the square of the units of the variable itself. For example, a variable measured in meters will have a variance measured in meters squared. For this reason, describing data sets via their standard deviation or root mean square deviation is often preferred over using the variance. In the dice example the standard deviation is √2.9 ≈ 1.7, slightly larger than the expected absolute deviation of 1.5.

The standard deviation and the expected absolute deviation can both be used as an indicator of the "spread" of a distribution. The standard deviation is more amenable to algebraic manipulation than the expected absolute deviation, and, together with variance and its generalization covariance, is used frequently in theoretical statistics; however the expected absolute deviation tends to be more robust as it is less sensitive to outliers arising from measurement anomalies or an unduly heavy-tailed distribution.

Approximating the variance of a function

The delta method uses second-order Taylor expansions to approximate the variance of a function of one or more random variables: see Taylor expansions for the moments of functions of random variables. For example, the approximate variance of a function of one variable is given by

$\operatorname {Var} \left[f(X)\right]\approx \left(f'(\operatorname {E} \left[X\right])\right)^{2}\operatorname {Var} \left[X\right]$

provided that f is twice differentiable and that the mean and variance of X are finite.

Population variance and sample variance

Vegeu també: Unbiased estimation of standard deviation

Real-world observations such as the measurements of yesterday's rain throughout the day typically cannot be complete sets of all possible observations that could be made. As such, the variance calculated from the finite set will in general not match the variance that would have been calculated from the full population of possible observations. This means that one estimates the mean and variance that would have been calculated from an omniscient set of observations by using an estimator equation. The estimator is a function of the sample of n observations drawn without observational bias from the whole population of potential observations. In this example that sample would be the set of actual measurements of yesterday's rainfall from available rain gauges within the geography of interest.

The simplest estimators for population mean and population variance are simply the mean and variance of the sample, the sample mean and (uncorrected) sample variance – these are consistent estimators (they converge to the correct value as the number of samples increases), but can be improved. Estimating the population variance by taking the sample's variance is close to optimal in general, but can be improved in two ways. Most simply, the sample variance is computed as an average of squared deviations about the (sample) mean, by dividing by n. However, using values other than n improves the estimator in various ways. Four common values for the denominator are n, n − 1, n + 1, and n − 1.5: n is the simplest (population variance of the sample), n − 1 eliminates bias, n + 1 minimizes mean squared error for the normal distribution, and n − 1.5 mostly eliminates bias in unbiased estimation of standard deviation for the normal distribution.

Firstly, if the omniscient mean is unknown (and is computed as the sample mean), then the sample variance is a biased estimator: it underestimates the variance by a factor of (n − 1) / n; correcting by this factor (dividing by n − 1 instead of n) is called Bessel's correction. The resulting estimator is unbiased, and is called the (corrected) sample variance or unbiased sample variance. For example, when n = 1 the variance of a single observation about the sample mean (itself) is obviously zero regardless of the population variance. If the mean is determined in some other way than from the same samples used to estimate the variance then this bias does not arise and the variance can safely be estimated as that of the samples about the (independently known) mean.

Secondly, the sample variance does not generally minimize mean squared error between sample variance and population variance. Correcting for bias often makes this worse: one can always choose a scale factor that performs better than the corrected sample variance, though the optimal scale factor depends on the excess kurtosis of the population (see mean squared error: variance), and introduces bias. This always consists of scaling down the unbiased estimator (dividing by a number larger than n − 1), and is a simple example of a shrinkage estimator: one "shrinks" the unbiased estimator towards zero. For the normal distribution, dividing by n + 1 (instead of n − 1 or n) minimizes mean squared error. The resulting estimator is biased, however, and is known as the biased sample variation.

Population variance

In general, the population variance of a finite population of size N with values x_i is given by

$\sigma ^{2}={\frac {1}{N}}\sum _{i=1}^{N}\left(x_{i}-\mu \right)^{2}={\frac {1}{N}}\sum _{i=1}^{N}\left(x_{i}^{2}-2\mu x_{i}+\mu ^{2}\right)=\left({\frac {1}{N}}\sum _{i=1}^{N}x_{i}^{2}\right)-2\mu \left({\frac {1}{N}}\sum _{i=1}^{N}x_{i}\right)+\mu ^{2}=\left({\frac {1}{N}}\sum _{i=1}^{N}x_{i}^{2}\right)-\mu ^{2}$

where the population mean is

$\mu ={\frac {1}{N}}\sum _{i=1}^{N}x_{i}$.

The population variance can also be computed using

$\sigma ^{2}={\frac {1}{N^{2}}}\sum _{i<j}\left(x_{i}-x_{j}\right)^{2}={\frac {1}{2N^{2}}}\sum _{i,j=1}^{N}\left(x_{i}-x_{j}\right)^{2}$

This is true because

${\begin{aligned}{\frac {1}{2N^{2}}}\sum _{i,j=1}^{N}\left(x_{i}-x_{j}\right)^{2}&={\frac {1}{2N^{2}}}\sum _{i,j=1}^{N}\left(x_{i}^{2}-2x_{i}x_{j}+x_{j}^{2}\right)\\&={\frac {1}{2N}}\sum _{j=1}^{N}\left({\frac {1}{N}}\sum _{i=1}^{N}x_{i}^{2}\right)-\left({\frac {1}{N}}\sum _{i=1}^{N}x_{i}\right)\left({\frac {1}{N}}\sum _{j=1}^{N}x_{j}\right)+{\frac {1}{2N}}\sum _{i=1}^{N}\left({\frac {1}{N}}\sum _{j=1}^{N}x_{j}^{2}\right)\\&={\frac {1}{2}}\left(\sigma ^{2}+\mu ^{2}\right)-\mu ^{2}+{\frac {1}{2}}\left(\sigma ^{2}+\mu ^{2}\right)=\sigma ^{2}\end{aligned}}$

The population variance matches the variance of the generating probability distribution. In this sense, the concept of population can be extended to continuous random variables with infinite populations.

Sample variance

In many practical situations, the true variance of a population is not known a priori and must be computed somehow. When dealing with extremely large populations, it is not possible to count every object in the population, so the computation must be performed on a sample of the population. Sample variance can also be applied to the estimation of the variance of a continuous distribution from a sample of that distribution.

We take a sample with replacement of n values y₁, ..., y_n from the population, where n < N, and estimate the variance on the basis of this sample. Directly taking the variance of the sample data gives the average of the squared deviations:

$\sigma _{y}^{2}={\frac {1}{n}}\sum _{i=1}^{n}\left(y_{i}-{\overline {y}}\right)^{2}=\left({\frac {1}{n}}\sum _{i=1}^{n}y_{i}^{2}\right)-{\overline {y}}^{2}={\frac {1}{n^{2}}}\sum _{i<j}\left(y_{i}-y_{j}\right)^{2}.$

Here, ${\overline {y}}$ denotes the sample mean:

${\overline {y}}={\frac {1}{n}}\sum _{i=1}^{n}y_{i}.$

Since the y_i are selected randomly, both ${\overline {y}}$ and $\sigma _{y}^{2}$ are random variables. Their expected values can be evaluated by averaging over the ensemble of all possible samples {y_i} of size n from the population. For $\sigma _{y}^{2}$ this gives:

${\begin{aligned}E[\sigma _{y}^{2}]&=E\left[{\frac {1}{n}}\sum _{i=1}^{n}\left(y_{i}-{\frac {1}{n}}\sum _{j=1}^{n}y_{j}\right)^{2}\right]\\&={\frac {1}{n}}\sum _{i=1}^{n}E\left[y_{i}^{2}-{\frac {2}{n}}y_{i}\sum _{j=1}^{n}y_{j}+{\frac {1}{n^{2}}}\sum _{j=1}^{n}y_{j}\sum _{k=1}^{n}y_{k}\right]\\&={\frac {1}{n}}\sum _{i=1}^{n}\left[{\frac {n-2}{n}}E[y_{i}^{2}]-{\frac {2}{n}}\sum _{j\neq i}E[y_{i}y_{j}]+{\frac {1}{n^{2}}}\sum _{j=1}^{n}\sum _{k\neq j}^{n}E[y_{j}y_{k}]+{\frac {1}{n^{2}}}\sum _{j=1}^{n}E[y_{j}^{2}]\right]\\&={\frac {1}{n}}\sum _{i=1}^{n}\left[{\frac {n-2}{n}}(\sigma ^{2}+\mu ^{2})-{\frac {2}{n}}(n-1)\mu ^{2}+{\frac {1}{n^{2}}}n(n-1)\mu ^{2}+{\frac {1}{n}}(\sigma ^{2}+\mu ^{2})\right]\\&={\frac {n-1}{n}}\sigma ^{2}.\end{aligned}}$

Hence $\sigma _{y}^{2}$ gives an estimate of the population variance that is biased by a factor of ${\frac {n-1}{n}}$. For this reason, $\sigma _{y}^{2}$ is referred to as the biased sample variance. Correcting for this bias yields the unbiased sample variance:

$s^{2}={\frac {n}{n-1}}\sigma _{y}^{2}={\frac {n}{n-1}}\left({\frac {1}{n}}\sum _{i=1}^{n}\left(y_{i}-{\overline {y}}\right)^{2}\right)={\frac {1}{n-1}}\sum _{i=1}^{n}\left(y_{i}-{\overline {y}}\right)^{2}$

Either estimator may be simply referred to as the sample variance when the version can be determined by context. The same proof is also applicable for samples taken from a continuous probability distribution.

The use of the term n − 1 is called Bessel's correction, and it is also used in sample covariance and the sample standard deviation (the square root of variance). The square root is a concave function and thus introduces negative bias (by Jensen's inequality), which depends on the distribution, and thus the corrected sample standard deviation (using Bessel's correction) is biased. The unbiased estimation of standard deviation is a technically involved problem, though for the normal distribution using the term n − 1.5 yields an almost unbiased estimator.

The unbiased sample variance is a U-statistic for the function ƒ(y₁, y₂) = (y₁ − y₂)²/2, meaning that it is obtained by averaging a 2-sample statistic over 2-element subsets of the population.

Distribution of the sample variance

Distribution and cumulative distribution of s²/σ², for various values of ν = n − 1, when the y_i are independent normally distributed.

Being a function of random variables, the sample variance is itself a random variable, and it is natural to study its distribution. In the case that y_i are independent observations from a normal distribution, Cochran's theorem shows that s² follows a scaled chi-squared distribution:

$(n-1){\frac {s^{2}}{\sigma ^{2}}}\sim \chi _{n-1}^{2}.$

As a direct consequence, it follows that

$\operatorname {E} (s^{2})=\operatorname {E} \left({\frac {\sigma ^{2}}{n-1}}\chi _{n-1}^{2}\right)=\sigma ^{2},$

and

$\operatorname {Var} [s^{2}]=\operatorname {Var} \left({\frac {\sigma ^{2}}{n-1}}\chi _{n-1}^{2}\right)={\frac {\sigma ^{4}}{(n-1)^{2}}}\operatorname {Var} \left(\chi _{n-1}^{2}\right)={\frac {2\sigma ^{4}}{n-1}}.$

If the y_i are independent and identically distributed, but not necessarily normally distributed, then

$\operatorname {E} [s^{2}]=\sigma ^{2},\quad \operatorname {Var} [s^{2}]={\frac {\sigma ^{4}}{n}}\left((\kappa -1)+{\frac {2}{n-1}}\right)={\frac {1}{n}}\left(\mu _{4}-{\frac {n-3}{n-1}}\sigma ^{4}\right),$

where κ is the kurtosis of the distribution and μ₄ is the fourth central moment.

If the conditions of the law of large numbers hold for the squared observations, s² is a consistent estimator of σ². One can see indeed that the variance of the estimator tends asymptotically to zero. An asymptotically equivalent formula was given in Kenney and Keeping (1951:164), Rose and Smith (2002:264), and Weisstein (n.d.).

Samuelson's inequality

Samuelson's inequality is a result that states bounds on the values that individual observations in a sample can take, given that the sample mean and (biased) variance have been calculated. Values must lie within the limits ${\bar {y}}\pm \sigma _{y}(n-1)^{1/2}.$

Relations with the harmonic and arithmetic means

It has been shown that for a sample {y_i} of real numbers,

$\sigma _{y}^{2}\leq 2y_{\max }(A-H),$

where y_max is the maximum of the sample, A is the arithmetic mean, H is the harmonic mean of the sample and $\sigma _{y}^{2}$ is the (biased) variance of the sample.

This bound has been improved, and it is known that variance is bounded by

$\sigma _{y}^{2}\leq {\frac {y_{\max }(A-H)(y_{\max }-A)}{y_{\max }-H}},$

$\sigma _{y}^{2}\geq {\frac {y_{\min }(A-H)(A-y_{\min })}{H-y_{\min }}},$

where y_min is the minimum of the sample.

Tests of equality of variances

Testing for the equality of two or more variances is difficult. The F test and chi square tests are both adversely affected by non-normality and are not recommended for this purpose.

Several non parametric tests have been proposed: these include the Barton–David–Ansari–Freund–Siegel–Tukey test, the Capon test, Mood test, the Klotz test and the Sukhatme test. The Sukhatme test applies to two variances and requires that both medians be known and equal to zero. The Mood, Klotz, Capon and Barton–David–Ansari–Freund–Siegel–Tukey tests also apply to two variances. They allow the median to be unknown but do require that the two medians are equal.

The Lehmann test is a parametric test of two variances. Of this test there are several variants known. Other tests of the equality of variances include the Box test, the Box–Anderson test and the Moses test.

Resampling methods, which include the bootstrap and the jackknife, may be used to test the equality of variances.

History

The term variance was first introduced by Ronald Fisher in his 1918 paper The Correlation Between Relatives on the Supposition of Mendelian Inheritance:

The great body of available statistics show us that the deviations of a human measurement from its mean follow very closely the Normal Law of Errors, and, therefore, that the variability may be uniformly measured by the standard deviation corresponding to the square root of the mean square error. When there are two independent causes of variability capable of producing in an otherwise uniform population distributions with standard deviations $\sigma _{1}$ and $\sigma _{2}$, it is found that the distribution, when both causes act together, has a standard deviation ${\sqrt {\sigma _{1}^{2}+\sigma _{2}^{2}}}$. It is therefore desirable in analysing the causes of variability to deal with the square of the standard deviation as the measure of variability. We shall term this quantity the Variance...

Geometric visualisation of the variance of an arbitrary distribution (2, 4, 4, 4, 5, 5, 7, 9):

1. A frequency distribution is constructed.
2. The centroid of the distribution gives its mean.
3. A square with sides equal to the difference of each value from the mean is formed for each value.
4. Arranging the squares into a rectangle with one side equal to the number of values, n, results in the other side being the distribution's variance, σ².

Moment of inertia

Vegeu també: Moment (physics) § Examples

The variance of a probability distribution is analogous to the moment of inertia in classical mechanics of a corresponding mass distribution along a line, with respect to rotation about its center of mass. It is because of this analogy that such things as the variance are called moments of probability distributions. The covariance matrix is related to the moment of inertia tensor for multivariate distributions. The moment of inertia of a cloud of n points with a covariance matrix of $\Sigma$ is given by

$I=n(\mathbf {1} _{3\times 3}\operatorname {tr} (\Sigma )-\Sigma ).$

This difference between moment of inertia in physics and in statistics is clear for points that are gathered along a line. Suppose many points are close to the x axis and distributed along it. The covariance matrix might look like

$\Sigma ={\begin{bmatrix}10&0&0\\0&0.1&0\\0&0&0.1\end{bmatrix}}.$

That is, there is the most variance in the x direction. Physicists would consider this to have a low moment about the x axis so the moment-of-inertia tensor is

$I=n{\begin{bmatrix}0.2&0&0\\0&10.1&0\\0&0&10.1\end{bmatrix}}.$

Semivariance

The semivariance is calculated in the same manner as the variance but only those observations that fall below the mean are included in the calculation. It is sometimes described as a measure of downside risk in an investments context. For skewed distributions, the semivariance can provide additional information that a variance does not.

For inequalities associated with the semivariance, see Chebyshev's inequality#Semivariances.

Generalizations

For complex variables

If $x$ is a scalar complex-valued random variable, with values in $\mathbb {C} ,$ then its variance is $\operatorname {E} \left[(x-\mu )(x-\mu )^{*}\right],$ where $x^{*}$ is the complex conjugate of $x.$ This variance is a real scalar.

For vector-valued random variables

As a matrix

If $X$ is a vector-valued random variable, with values in $\mathbb {R} ^{n},$ and thought of as a column vector, then a natural generalization of variance is $\operatorname {E} \left[(X-\mu )(X-\mu )^{\operatorname {T} }\right],$ where $\mu =\operatorname {E} (X)$ and $X^{\operatorname {T} }$ is the transpose of $X,$ and so is a row vector. The result is a positive semi-definite square matrix, commonly referred to as the variance-covariance matrix (or simply as the covariance matrix).

If $X$ is a vector- and complex-valued random variable, with values in $\mathbb {C} ^{n},$ then the covariance matrix is $\operatorname {E} \left[(X-\mu )(X-\mu )^{\dagger }\right],$ where $X^{\dagger }$ is the conjugate transpose of $X.$ This matrix is also positive semi-definite and square.

As a scalar

Another natural generalization of variance for such vector-valued random variables $X,$ which results in a scalar value rather than in a matrix, is obtained by interpreting the deviation between the random variable and its mean as the Euclidean distance. This results in $\operatorname {E} \left[(X-\mu )^{\operatorname {T} }(X-\mu )\right]=\operatorname {tr} (C),$ which is the trace of the covariance matrix.

See also

Vegeu Viquialcon/proves en el Viccionari, el diccionari lliure.Viccionari

• Average absolute deviation
• Bhatia–Davis inequality
• Common-method variance
• Correlation
• Chebyshev's inequality
• Distance variance
• Estimation of covariance matrices
• Explained variance
• Homoscedasticity
• Mean absolute error
• Mean absolute difference
• Mean preserving spread
• Pooled variance (also known as combined, composite, or overall variance)
• Popoviciu's inequality on variances
• Qualitative variation
• Quasi-variance, used in linear regression when the explanatory variable is categorical
• Reduced chi-squared
• Sample mean and covariance
• Semivariance
• Skewness
• Taylor's law
• Weighted sample variance