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Weighted arithmetic mean

From Wikipedia, the free encyclopedia
Statistical amount
For broader coverage of this topic, seeWeighted average.

Theweighted arithmetic mean is similar to an ordinaryarithmetic mean (the most common type ofaverage), except that instead of each of the data points contributing equally to the final average, some data points contribute more than others. The notion of weighted mean plays a role indescriptive statistics and also occurs in a more general form in several other areas ofmathematics.

If all the weights are equal, then the weighted mean is the same as thearithmetic mean. While weighted means generally behave in a similar fashion to arithmetic means, they do have a few counterintuitive properties, as captured for instance inSimpson's paradox.

Examples

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Basic example

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Given two schoolclassesone with 20 students, one with 30studentsand test grades in each class as follows:

Morning class = {62, 67, 71, 74, 76, 77, 78, 79, 79, 80, 80, 81, 81, 82, 83, 84, 86, 89, 93, 98}

Afternoon class = {81, 82, 83, 84, 85, 86, 87, 87, 88, 88, 89, 89, 89, 90, 90, 90, 90, 91, 91, 91, 92, 92, 93, 93, 94, 95, 96, 97, 98, 99}

The mean for the morning class is 80 and the mean of the afternoon class is 90. The unweighted mean of the two means is 85. However, this does not account for the difference in number of students in each class (20 versus 30); hence the value of 85 does not reflect the average student grade (independent of class). The average student grade can be obtained by averaging all the grades, without regard to classes (add all the grades up and divide by the total number of students):x¯=430050=86.{\displaystyle {\bar {x}}={\frac {4300}{50}}=86.}

Or, this can be accomplished by weighting the class means by the number of students in each class. The larger class is given more "weight":

x¯=(20×80)+(30×90)20+30=86.{\displaystyle {\bar {x}}={\frac {(20\times 80)+(30\times 90)}{20+30}}=86.}

Thus, the weighted mean makes it possible to find the mean average student grade without knowing each student's score. Only the class means and the number of students in each class are needed.

Convex combination example

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Since only therelative weights are relevant, any weighted mean can be expressed using coefficients that sum to one. Such a linear combination is called aconvex combination.

Using the previous example, we would get the following weights:

2020+30=0.4{\displaystyle {\frac {20}{20+30}}=0.4}
3020+30=0.6{\displaystyle {\frac {30}{20+30}}=0.6}

Then, apply the weights like this:

x¯=(0.4×80)+(0.6×90)=86.{\displaystyle {\bar {x}}=(0.4\times 80)+(0.6\times 90)=86.}

Mathematical definition

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Formally, the weighted mean of a non-empty finitetuple of data(x1,x2,,xn){\displaystyle \left(x_{1},x_{2},\dots ,x_{n}\right)},with corresponding non-negativeweights(w1,w2,,wn){\displaystyle \left(w_{1},w_{2},\dots ,w_{n}\right)} is

x¯=i=1nwixii=1nwi,{\displaystyle {\bar {x}}={\frac {\sum \limits _{i=1}^{n}w_{i}x_{i}}{\sum \limits _{i=1}^{n}w_{i}}},}

which expands to:

x¯=w1x1+w2x2++wnxnw1+w2++wn.{\displaystyle {\bar {x}}={\frac {w_{1}x_{1}+w_{2}x_{2}+\cdots +w_{n}x_{n}}{w_{1}+w_{2}+\cdots +w_{n}}}.}

Therefore, data elements with a high weight contribute more to the weighted mean than do elements with a low weight. The weights may not be negative in order for the equation to work[a]. Some may be zero, but not all of them (since division by zero is not allowed).

The formulas are simplified when the weights are normalized such that they sum up to 1, i.e.,i=1nwi=1{\textstyle \sum \limits _{i=1}^{n}{w_{i}'}=1}.For such normalized weights, the weighted mean is equivalently:

x¯=i=1nwixi{\displaystyle {\bar {x}}=\sum \limits _{i=1}^{n}{w_{i}'x_{i}}}.

One can always normalize the weights by making the following transformation on the original weights:

wi=wij=1nwj{\displaystyle w_{i}'={\frac {w_{i}}{\sum \limits _{j=1}^{n}{w_{j}}}}}.

Theordinary mean1ni=1nxi{\textstyle {\frac {1}{n}}\sum \limits _{i=1}^{n}{x_{i}}} is a special case of the weighted mean where all data have equal weights.

If the data elements areindependent and identically distributed random variables with varianceσ2{\displaystyle \sigma ^{2}}, thestandard error of the weighted mean,σx¯{\displaystyle \sigma _{\bar {x}}}, can be shown viauncertainty propagation to be:

σx¯=σi=1nwi2{\textstyle \sigma _{\bar {x}}=\sigma {\sqrt {\sum \limits _{i=1}^{n}w_{i}'^{2}}}}

Variance-defined weights

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Main article:Inverse-variance weighting
See also:Weighted least squares

For the weighted mean of a list of data for which each elementxi{\displaystyle x_{i}} potentially comes from a differentprobability distribution with knownvarianceσi2{\displaystyle \sigma _{i}^{2}}, all having the same mean, one possible choice for the weights is given by the reciprocal of variance:

wi=1σi2.{\displaystyle w_{i}={\frac {1}{\sigma _{i}^{2}}}.}

The weighted mean in this case is:

x¯=i=1n(xiσi2)i=1n1σi2=i=1n(xiwi)i=1nwi,{\displaystyle {\bar {x}}={\frac {\sum _{i=1}^{n}\left({\dfrac {x_{i}}{\sigma _{i}^{2}}}\right)}{\sum _{i=1}^{n}{\dfrac {1}{\sigma _{i}^{2}}}}}={\frac {\sum _{i=1}^{n}\left(x_{i}\cdot w_{i}\right)}{\sum _{i=1}^{n}w_{i}}},}

and thestandard error of the weighted mean (with inverse-variance weights) is:

σx¯=1i=1nσi2=1i=1nwi,{\displaystyle \sigma _{\bar {x}}={\sqrt {\frac {1}{\sum _{i=1}^{n}\sigma _{i}^{-2}}}}={\sqrt {\frac {1}{\sum _{i=1}^{n}w_{i}}}},}

Note this reduces toσx¯2=σ02/n{\displaystyle \sigma _{\bar {x}}^{2}=\sigma _{0}^{2}/n} when allσi=σ0{\displaystyle \sigma _{i}=\sigma _{0}}.It is a special case of the general formula in previous section,

σx¯2=i=1nwi2σi2=i=1nσi4σi2(i=1nσi2)2.{\displaystyle \sigma _{\bar {x}}^{2}=\sum _{i=1}^{n}{w_{i}'^{2}\sigma _{i}^{2}}={\frac {\sum _{i=1}^{n}{\sigma _{i}^{-4}\sigma _{i}^{2}}}{\left(\sum _{i=1}^{n}\sigma _{i}^{-2}\right)^{2}}}.}

The equations above can be combined to obtain:

x¯=σx¯2i=1nxiσi2.{\displaystyle {\bar {x}}=\sigma _{\bar {x}}^{2}\sum _{i=1}^{n}{\frac {x_{i}}{\sigma _{i}^{2}}}.}

The significance of this choice is that this weighted mean is themaximum likelihood estimator of the mean of the probability distributions under the assumption that they are independent andnormally distributed with the same mean.

Statistical properties

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Expectancy

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The weighted sample mean,x¯{\displaystyle {\bar {x}}}, is itself a random variable. Its expected value and standard deviation are related to the expected values and standard deviations of the observations, as follows. For simplicity, we assume normalized weights (weights summing to one).

If the observations have expected valuesE(xi)=μi,{\displaystyle E(x_{i})={\mu _{i}},}then the weighted sample mean has expectationE(x¯)=i=1nwiμi.{\displaystyle E({\bar {x}})=\sum _{i=1}^{n}{w_{i}'\mu _{i}}.}In particular, if the means are equal,μi=μ{\displaystyle \mu _{i}=\mu }, then the expectation of the weighted sample mean will be that value,E(x¯)=μ.{\displaystyle E({\bar {x}})=\mu .}

Variance

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Simple i.i.d. case

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When treating the weights as constants, and having a sample ofn observations fromuncorrelatedrandom variables, all with the samevariance andexpectation (as is the case fori.i.d random variables), then the variance of the weighted mean can be estimated as the multiplication of the unweighted variance byKish's design effect (seeproof):

Var(y¯w)=σ^y2w2¯w¯2{\displaystyle \operatorname {Var} ({\bar {y}}_{w})={\hat {\sigma }}_{y}^{2}{\frac {\overline {w^{2}}}{{\bar {w}}^{2}}}}

Withσ^y2=i=1n(yiy¯)2n1{\displaystyle {\hat {\sigma }}_{y}^{2}={\frac {\sum _{i=1}^{n}(y_{i}-{\bar {y}})^{2}}{n-1}}},w¯=i=1nwin{\displaystyle {\bar {w}}={\frac {\sum _{i=1}^{n}w_{i}}{n}}}, andw2¯=i=1nwi2n{\displaystyle {\overline {w^{2}}}={\frac {\sum _{i=1}^{n}w_{i}^{2}}{n}}}

However, this estimation is rather limited due to the strong assumption about they observations. This has led to the development of alternative, more general, estimators.

Survey sampling perspective

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From amodel based perspective, we are interested in estimating the variance of the weighted mean when the differentyi{\displaystyle y_{i}} are noti.i.d random variables. An alternative perspective for this problem is that of some arbitrarysampling design of the data in which units areselected with unequal probabilities (with replacement).[1]: 306 

InSurvey methodology, the population mean, of some quantity of interesty, is calculated by taking an estimation of the total ofy over all elements in the population (Y or sometimesT) and dividing it by the population size – either known (N{\displaystyle N}) or estimated (N^{\displaystyle {\hat {N}}}). In this context, each value ofy is considered constant, and the variability comes from the selection procedure. This in contrast to "model based" approaches in which the randomness is often described in the y values. Thesurvey sampling procedure yields a series ofBernoulli indicator values (Ii{\displaystyle I_{i}}) that get 1 if some observationi is in the sample and 0 if it was not selected. This can occur with fixed sample size, or varied sample size sampling (e.g.:Poisson sampling). The probability of some element to be chosen, given a sample, is denoted asP(Ii=1Some sample of size n)=πi{\displaystyle P(I_{i}=1\mid {\text{Some sample of size }}n)=\pi _{i}}, and the one-draw probability of selection isP(Ii=1|one sample draw)=piπin{\displaystyle P(I_{i}=1|{\text{one sample draw}})=p_{i}\approx {\frac {\pi _{i}}{n}}} (If N is very large and eachpi{\displaystyle p_{i}} is very small). For the following derivation we'll assume that the probability of selecting each element is fully represented by these probabilities.[2]: 42, 43, 51  I.e.: selecting some element will not influence the probability of drawing another element (this doesn't apply for things such ascluster sampling design).

Since each element (yi{\displaystyle y_{i}}) is fixed, and the randomness comes from it being included in the sample or not (Ii{\displaystyle I_{i}}), we often talk about the multiplication of the two, which is a random variable. To avoid confusion in the following section, let's call this term:yi=yiIi{\displaystyle y'_{i}=y_{i}I_{i}}. With the following expectancy:E[yi]=yiE[Ii]=yiπi{\displaystyle E[y'_{i}]=y_{i}E[I_{i}]=y_{i}\pi _{i}}; and variance:V[yi]=yi2V[Ii]=yi2πi(1πi){\displaystyle V[y'_{i}]=y_{i}^{2}V[I_{i}]=y_{i}^{2}\pi _{i}(1-\pi _{i})}.

When each element of the sample is inflated by the inverse of its selection probability, it is termed theπ{\displaystyle \pi }-expandedy values, i.e.:yˇi=yiπi{\displaystyle {\check {y}}_{i}={\frac {y_{i}}{\pi _{i}}}}. A related quantity isp{\displaystyle p}-expandedy values:yipi=nyˇi{\displaystyle {\frac {y_{i}}{p_{i}}}=n{\check {y}}_{i}}.[2]: 42, 43, 51, 52  As above, we can add a tick mark if multiplying by the indicator function. I.e.:yˇi=Iiyˇi=Iiyiπi{\displaystyle {\check {y}}'_{i}=I_{i}{\check {y}}_{i}={\frac {I_{i}y_{i}}{\pi _{i}}}}

In thisdesign based perspective, the weights, used in the numerator of the weighted mean, are obtained from taking the inverse of the selection probability (i.e.: the inflation factor). I.e.:wi=1πi1n×pi{\displaystyle w_{i}={\frac {1}{\pi _{i}}}\approx {\frac {1}{n\times p_{i}}}}.

Variance of the weighted sum (pwr-estimator for totals)

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If the population sizeN is known we can estimate the population mean usingY¯^known N=Y^pwrNi=1nwiyiN{\displaystyle {\hat {\bar {Y}}}_{{\text{known }}N}={\frac {{\hat {Y}}_{pwr}}{N}}\approx {\frac {\sum _{i=1}^{n}w_{i}y'_{i}}{N}}}.

If thesampling design is one that results in a fixed sample sizen (such as inpps sampling), then the variance of this estimator is:

Var(Y¯^known N)=1N2nn1i=1n(wiyiwy¯)2{\displaystyle \operatorname {Var} \left({\hat {\bar {Y}}}_{{\text{known }}N}\right)={\frac {1}{N^{2}}}{\frac {n}{n-1}}\sum _{i=1}^{n}\left(w_{i}y_{i}-{\overline {wy}}\right)^{2}}
Proof

The general formula can be developed like this:

Y¯^known N=Y^pwrN=1ni=1nyipiNi=1nyiπiN=i=1nwiyiN.{\displaystyle {\hat {\bar {Y}}}_{{\text{known }}N}={\frac {{\hat {Y}}_{pwr}}{N}}={\frac {{\frac {1}{n}}\sum _{i=1}^{n}{\frac {y'_{i}}{p_{i}}}}{N}}\approx {\frac {\sum _{i=1}^{n}{\frac {y'_{i}}{\pi _{i}}}}{N}}={\frac {\sum _{i=1}^{n}w_{i}y'_{i}}{N}}.}

The population total is denoted asY=i=1Nyi{\displaystyle Y=\sum _{i=1}^{N}y_{i}} and it may be estimated by the (unbiased)Horvitz–Thompson estimator, also called theπ{\displaystyle \pi }-estimator. This estimator can be itself estimated using thepwr-estimator (i.e.:p{\displaystyle p}-expanded with replacement estimator, or "probability with replacement" estimator). With the above notation, it is:Y^pwr=1ni=1nyipi=i=1nyinpii=1nyiπi=i=1nwiyi{\displaystyle {\hat {Y}}_{pwr}={\frac {1}{n}}\sum _{i=1}^{n}{\frac {y'_{i}}{p_{i}}}=\sum _{i=1}^{n}{\frac {y'_{i}}{np_{i}}}\approx \sum _{i=1}^{n}{\frac {y'_{i}}{\pi _{i}}}=\sum _{i=1}^{n}w_{i}y'_{i}}.[2]: 51 

The estimated variance of thepwr-estimator is given by:[2]: 52 Var(Y^pwr)=nn1i=1n(wiyiwy¯)2{\displaystyle \operatorname {Var} ({\hat {Y}}_{pwr})={\frac {n}{n-1}}\sum _{i=1}^{n}\left(w_{i}y_{i}-{\overline {wy}}\right)^{2}}wherewy¯=i=1nwiyin{\displaystyle {\overline {wy}}=\sum _{i=1}^{n}{\frac {w_{i}y_{i}}{n}}}.

The above formula was taken from Sarndal et al. (1992) (also presented in Cochran 1977), but was written differently.[2]: 52 [1]: 307 (11.35)  The left side is how the variance was written and the right side is how we've developed the weighted version:

Var(Y^pwr)=1n1n1i=1n(yipiY^pwr)2=1n1n1i=1n(nnyipinni=1nwiyi)2=1n1n1i=1n(nyiπini=1nwiyin)2=n2n1n1i=1n(wiyiwy¯)2=nn1i=1n(wiyiwy¯)2{\displaystyle {\begin{aligned}\operatorname {Var} ({\hat {Y}}_{\text{pwr}})&={\frac {1}{n}}{\frac {1}{n-1}}\sum _{i=1}^{n}\left({\frac {y_{i}}{p_{i}}}-{\hat {Y}}_{pwr}\right)^{2}\\&={\frac {1}{n}}{\frac {1}{n-1}}\sum _{i=1}^{n}\left({\frac {n}{n}}{\frac {y_{i}}{p_{i}}}-{\frac {n}{n}}\sum _{i=1}^{n}w_{i}y_{i}\right)^{2}={\frac {1}{n}}{\frac {1}{n-1}}\sum _{i=1}^{n}\left(n{\frac {y_{i}}{\pi _{i}}}-n{\frac {\sum _{i=1}^{n}w_{i}y_{i}}{n}}\right)^{2}\\&={\frac {n^{2}}{n}}{\frac {1}{n-1}}\sum _{i=1}^{n}\left(w_{i}y_{i}-{\overline {wy}}\right)^{2}\\&={\frac {n}{n-1}}\sum _{i=1}^{n}\left(w_{i}y_{i}-{\overline {wy}}\right)^{2}\end{aligned}}}

And we got to the formula from above.

An alternative term, for when the sampling has a random sample size (as inPoisson sampling), is presented in Sarndal et al. (1992) as:[2]: 182 

Var(Y¯^pwr (known N))=1N2i=1nj=1n(Δˇijyˇiyˇj){\displaystyle \operatorname {Var} ({\hat {\bar {Y}}}_{{\text{pwr (known }}N{\text{)}}})={\frac {1}{N^{2}}}\sum _{i=1}^{n}\sum _{j=1}^{n}\left({\check {\Delta }}_{ij}{\check {y}}_{i}{\check {y}}_{j}\right)}

Withyˇi=yiπi{\displaystyle {\check {y}}_{i}={\frac {y_{i}}{\pi _{i}}}}. Also,C(Ii,Ij)=πijπiπj=Δij{\displaystyle C(I_{i},I_{j})=\pi _{ij}-\pi _{i}\pi _{j}=\Delta _{ij}} whereπij{\displaystyle \pi _{ij}} is the probability of selecting both i and j.[2]: 36  AndΔˇij=1πiπjπij{\displaystyle {\check {\Delta }}_{ij}=1-{\frac {\pi _{i}\pi _{j}}{\pi _{ij}}}}, and for i=j:Δˇii=1πiπiπi=1πi{\displaystyle {\check {\Delta }}_{ii}=1-{\frac {\pi _{i}\pi _{i}}{\pi _{i}}}=1-\pi _{i}}.[2]: 43 

If the selection probability are uncorrelated (i.e.:ij:C(Ii,Ij)=0{\displaystyle \forall i\neq j:C(I_{i},I_{j})=0}), and when assuming the probability of each element is very small, then:

Var(Y¯^pwr (known N))=1N2i=1n(wiyi)2{\displaystyle \operatorname {Var} ({\hat {\bar {Y}}}_{{\text{pwr (known }}N{\text{)}}})={\frac {1}{N^{2}}}\sum _{i=1}^{n}\left(w_{i}y_{i}\right)^{2}}
Proof

We assume that(1πi)1{\displaystyle (1-\pi _{i})\approx 1} and thatVar(Y^pwr (known N))=1N2i=1nj=1n(Δˇijyˇiyˇj)=1N2i=1n(Δˇiiyˇiyˇi)=1N2i=1n((1πi)yiπiyiπi)=1N2i=1n(wiyi)2{\displaystyle {\begin{aligned}\operatorname {Var} ({\hat {Y}}_{{\text{pwr (known }}N{\text{)}}})&={\frac {1}{N^{2}}}\sum _{i=1}^{n}\sum _{j=1}^{n}\left({\check {\Delta }}_{ij}{\check {y}}_{i}{\check {y}}_{j}\right)\\&={\frac {1}{N^{2}}}\sum _{i=1}^{n}\left({\check {\Delta }}_{ii}{\check {y}}_{i}{\check {y}}_{i}\right)\\&={\frac {1}{N^{2}}}\sum _{i=1}^{n}\left((1-\pi _{i}){\frac {y_{i}}{\pi _{i}}}{\frac {y_{i}}{\pi _{i}}}\right)\\&={\frac {1}{N^{2}}}\sum _{i=1}^{n}\left(w_{i}y_{i}\right)^{2}\end{aligned}}}

Variance of the weighted mean (π-estimator for ratio-mean)

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The previous section dealt with estimating the population mean as a ratio of an estimated population total (Y^{\displaystyle {\hat {Y}}}) with a known population size (N{\displaystyle N}), and the variance was estimated in that context. Another common case is that the population size itself (N{\displaystyle N}) is unknown and is estimated using the sample (i.e.:N^{\displaystyle {\hat {N}}}). The estimation ofN{\displaystyle N} can be described as the sum of weights. So whenwi=1πi{\displaystyle w_{i}={\frac {1}{\pi _{i}}}} we getN^=i=1nwiIi=i=1nIiπi=i=1n1ˇi{\displaystyle {\hat {N}}=\sum _{i=1}^{n}w_{i}I_{i}=\sum _{i=1}^{n}{\frac {I_{i}}{\pi _{i}}}=\sum _{i=1}^{n}{\check {1}}'_{i}}. With the above notation, the parameter we care about is the ratio of the sums ofyi{\displaystyle y_{i}}s, and 1s. I.e.:R=Y¯=i=1Nyiπii=1N1πi=i=1Nyˇii=1N1ˇi=i=1Nwiyii=1Nwi{\displaystyle R={\bar {Y}}={\frac {\sum _{i=1}^{N}{\frac {y_{i}}{\pi _{i}}}}{\sum _{i=1}^{N}{\frac {1}{\pi _{i}}}}}={\frac {\sum _{i=1}^{N}{\check {y}}_{i}}{\sum _{i=1}^{N}{\check {1}}_{i}}}={\frac {\sum _{i=1}^{N}w_{i}y_{i}}{\sum _{i=1}^{N}w_{i}}}}. We can estimate it using our sample with:R^=Y¯^=i=1NIiyiπii=1NIi1πi=i=1Nyˇii=1N1ˇi=i=1Nwiyii=1Nwi1i=i=1nwiyii=1nwi1i=y¯w{\displaystyle {\hat {R}}={\hat {\bar {Y}}}={\frac {\sum _{i=1}^{N}I_{i}{\frac {y_{i}}{\pi _{i}}}}{\sum _{i=1}^{N}I_{i}{\frac {1}{\pi _{i}}}}}={\frac {\sum _{i=1}^{N}{\check {y}}'_{i}}{\sum _{i=1}^{N}{\check {1}}'_{i}}}={\frac {\sum _{i=1}^{N}w_{i}y'_{i}}{\sum _{i=1}^{N}w_{i}1'_{i}}}={\frac {\sum _{i=1}^{n}w_{i}y'_{i}}{\sum _{i=1}^{n}w_{i}1'_{i}}}={\bar {y}}_{w}}. As we moved from using N to using n, we actually know that all the indicator variables get 1, so we could simply write:y¯w=i=1nwiyii=1nwi{\displaystyle {\bar {y}}_{w}={\frac {\sum _{i=1}^{n}w_{i}y_{i}}{\sum _{i=1}^{n}w_{i}}}}. This will be theestimand for specific values of y and w, but the statistical properties comes when including the indicator variabley¯w=i=1nwiyii=1nwi1i{\displaystyle {\bar {y}}_{w}={\frac {\sum _{i=1}^{n}w_{i}y'_{i}}{\sum _{i=1}^{n}w_{i}1'_{i}}}}.[2]: 162, 163, 176 

This is called aRatio estimator and it is approximately unbiased forR.[2]: 182 

In this case, the variability of theratio depends on the variability of the random variables both in the numerator and the denominator - as well as their correlation. Since there is no closed analytical form to compute this variance, various methods are used for approximate estimation. PrimarilyTaylor series first-order linearization, asymptotics, and bootstrap/jackknife.[2]: 172  The Taylor linearization method could lead to under-estimation of the variance for small sample sizes in general, but that depends on the complexity of the statistic. For the weighted mean, the approximate variance is supposed to be relatively accurate even for medium sample sizes.[2]: 176  For when the sampling has a random sample size (as inPoisson sampling), it is as follows:[2]: 182 

V(y¯w)^=1(i=1nwi)2i=1nwi2(yiy¯w)2{\displaystyle {\widehat {V({\bar {y}}_{w})}}={\frac {1}{(\sum _{i=1}^{n}w_{i})^{2}}}\sum _{i=1}^{n}w_{i}^{2}(y_{i}-{\bar {y}}_{w})^{2}}.

Ifπipin{\displaystyle \pi _{i}\approx p_{i}n}, then either usingwi=1πi{\displaystyle w_{i}={\frac {1}{\pi _{i}}}} orwi=1pi{\displaystyle w_{i}={\frac {1}{p_{i}}}} would give the same estimator, since multiplyingwi{\displaystyle w_{i}} by some factor would lead to the same estimator. It also means that if we scale the sum of weights to be equal to a known-from-before population sizeN, the variance calculation would look the same. When all weights are equal to one another, this formula is reduced to the standard unbiased variance estimator.

Proof

The Taylor linearization states that for a general ratio estimator of two sums (R^=Y^Z^{\displaystyle {\hat {R}}={\frac {\hat {Y}}{\hat {Z}}}}), they can be expanded around the true value R, and give:[2]: 178 

R^=Y^Z^=i=1nwiyii=1nwiziR+1Zi=1n(yiπiRziπi){\displaystyle {\hat {R}}={\frac {\hat {Y}}{\hat {Z}}}={\frac {\sum _{i=1}^{n}w_{i}y'_{i}}{\sum _{i=1}^{n}w_{i}z'_{i}}}\approx R+{\frac {1}{Z}}\sum _{i=1}^{n}\left({\frac {y'_{i}}{\pi _{i}}}-R{\frac {z'_{i}}{\pi _{i}}}\right)}

And the variance can be approximated by:[2]: 178, 179 

V(R^)^=1Z^2i=1nj=1n(ΔˇijyiR^ziπiyjR^zjπj)=1Z^2[V(Y^)^+R^V(Z^)^2R^C^(Y^,Z^)]{\displaystyle {\widehat {V({\hat {R}})}}={\frac {1}{{\hat {Z}}^{2}}}\sum _{i=1}^{n}\sum _{j=1}^{n}\left({\check {\Delta }}_{ij}{\frac {y_{i}-{\hat {R}}z_{i}}{\pi _{i}}}{\frac {y_{j}-{\hat {R}}z_{j}}{\pi _{j}}}\right)={\frac {1}{{\hat {Z}}^{2}}}\left[{\widehat {V({\hat {Y}})}}+{\hat {R}}{\widehat {V({\hat {Z}})}}-2{\hat {R}}{\hat {C}}({\hat {Y}},{\hat {Z}})\right]}.

The termC^(Y^,Z^){\displaystyle {\hat {C}}({\hat {Y}},{\hat {Z}})} is the estimated covariance between the estimated sum of Y and estimated sum of Z. Since this is thecovariance of two sums of random variables, it would include many combinations of covariances that will depend on the indicator variables. If the selection probability are uncorrelated (i.e.:ij:Δij=C(Ii,Ij)=0{\displaystyle \forall i\neq j:\Delta _{ij}=C(I_{i},I_{j})=0}), this term would still include a summation ofn covariances for each elementi betweenyi=Iiyi{\displaystyle y'_{i}=I_{i}y_{i}} andzi=Iizi{\displaystyle z'_{i}=I_{i}z_{i}}. This helps illustrate that this formula incorporates the effect of correlation between y and z on the variance of the ratio estimators.

When definingzi=1{\displaystyle z_{i}=1} the above becomes:[2]: 182 

V(R^)^=V(y¯w)^=1N^2i=1nj=1n(Δˇijyiy¯wπiyjy¯wπj).{\displaystyle {\widehat {V({\hat {R}})}}={\widehat {V({\bar {y}}_{w})}}={\frac {1}{{\hat {N}}^{2}}}\sum _{i=1}^{n}\sum _{j=1}^{n}\left({\check {\Delta }}_{ij}{\frac {y_{i}-{\bar {y}}_{w}}{\pi _{i}}}{\frac {y_{j}-{\bar {y}}_{w}}{\pi _{j}}}\right).}

If the selection probability are uncorrelated (i.e.:ij:Δij=C(Ii,Ij)=0{\displaystyle \forall i\neq j:\Delta _{ij}=C(I_{i},I_{j})=0}), and when assuming the probability of each element is very small (i.e.:(1πi)1{\displaystyle (1-\pi _{i})\approx 1}), then the above reduced to the following:V(y¯w)^=1N^2i=1n((1πi)yiy¯wπi)2=1(i=1nwi)2i=1nwi2(yiy¯w)2.{\displaystyle {\widehat {V({\bar {y}}_{w})}}={\frac {1}{{\hat {N}}^{2}}}\sum _{i=1}^{n}\left((1-\pi _{i}){\frac {y_{i}-{\bar {y}}_{w}}{\pi _{i}}}\right)^{2}={\frac {1}{(\sum _{i=1}^{n}w_{i})^{2}}}\sum _{i=1}^{n}w_{i}^{2}(y_{i}-{\bar {y}}_{w})^{2}.}

A similar re-creation of the proof (up to some mistakes at the end) was provided by Thomas Lumley in crossvalidated.[3]

We have (at least) two versions of variance for the weighted mean: one with known and one with unknown population size estimation. There is no uniformly better approach, but the literature presents several arguments to prefer using the population estimation version (even when the population size is known).[2]: 188  For example: if all y values are constant, the estimator with unknown population size will give the correct result, while the one with known population size will have some variability. Also, when the sample size itself is random (e.g.: inPoisson sampling), the version with unknown population mean is considered more stable. Lastly, if the proportion of sampling is negatively correlated with the values (i.e.: smaller chance to sample an observation that is large), then the un-known population size version slightly compensates for that.

For the trivial case in which all the weights are equal to 1, the above formula is just like the regular formula for the variance of the mean (but notice that it uses the maximum likelihood estimator for the variance instead of the unbiased variance. I.e.: dividing it by n instead of (n-1)).

Bootstrapping validation

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It has been shown, by Gatz et al. (1995), that in comparison tobootstrapping methods, the following (variance estimation of ratio-mean usingTaylor series linearization) is a reasonable estimation for the square of the standard error of the mean (when used in the context of measuring chemical constituents):[4]: 1186 

σx¯w2^=n(n1)(nw¯)2[(wixiw¯x¯w)22x¯w(wiw¯)(wixiw¯x¯w)+x¯w2(wiw¯)2]{\displaystyle {\widehat {\sigma _{{\bar {x}}_{w}}^{2}}}={\frac {n}{(n-1)(n{\bar {w}})^{2}}}\left[\sum (w_{i}x_{i}-{\bar {w}}{\bar {x}}_{w})^{2}-2{\bar {x}}_{w}\sum (w_{i}-{\bar {w}})(w_{i}x_{i}-{\bar {w}}{\bar {x}}_{w})+{\bar {x}}_{w}^{2}\sum (w_{i}-{\bar {w}})^{2}\right]}

wherew¯=win{\displaystyle {\bar {w}}={\frac {\sum w_{i}}{n}}}. Further simplification leads to

σx¯2^=n(n1)(nw¯)2wi2(xix¯w)2{\displaystyle {\widehat {\sigma _{\bar {x}}^{2}}}={\frac {n}{(n-1)(n{\bar {w}})^{2}}}\sum w_{i}^{2}(x_{i}-{\bar {x}}_{w})^{2}}

Gatz et al. mention that the above formulation was published by Endlich et al. (1988) when treating the weighted mean as a combination of a weighted total estimator divided by an estimator of the population size,[5] based on the formulation published by Cochran (1977), as an approximation to the ratio mean. However, Endlich et al. didn't seem to publish this derivation in their paper (even though they mention they used it), and Cochran's book includes a slightly different formulation.[1]: 155  Still, it's almost identical to the formulations described in previous sections.

Replication-based estimators

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Because there is no closed analytical form for the variance of the weighted mean, it was proposed in the literature to rely on replication methods such as theJackknife andBootstrapping.[1]: 321 

Other notes

[edit]

For uncorrelated observations with variancesσi2{\displaystyle \sigma _{i}^{2}}, the variance of the weighted sample mean is[citation needed]

σx¯2=i=1nwi2σi2{\displaystyle \sigma _{\bar {x}}^{2}=\sum _{i=1}^{n}{w_{i}'^{2}\sigma _{i}^{2}}}

whose square rootσx¯{\displaystyle \sigma _{\bar {x}}} can be called thestandard error of the weighted mean (general case).[citation needed]

Consequently, if all the observations have equal variance,σi2=σ02{\displaystyle \sigma _{i}^{2}=\sigma _{0}^{2}}, the weighted sample mean will have variance

σx¯2=σ02i=1nwi2,{\displaystyle \sigma _{\bar {x}}^{2}=\sigma _{0}^{2}\sum _{i=1}^{n}{w_{i}'^{2}},}

where1/ni=1nwi21{\textstyle 1/n\leq \sum _{i=1}^{n}{w_{i}'^{2}}\leq 1}. The variance attains its maximum value,σ02{\displaystyle \sigma _{0}^{2}}, when all weights except one are zero. Its minimum value is found when all weights are equal (i.e., unweighted mean), in which case we haveσx¯=σ0/n{\textstyle \sigma _{\bar {x}}=\sigma _{0}/{\sqrt {n}}}, i.e., it degenerates into thestandard error of the mean, squared.

Because one can always transform non-normalized weights to normalized weights, all formulas in this section can be adapted to non-normalized weights by replacing allwi=wii=1nwi{\displaystyle w_{i}'={\frac {w_{i}}{\sum _{i=1}^{n}{w_{i}}}}}.

Related concepts

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Weighted sample variance

[edit]
See also:§ Correcting for over- or under-dispersion

Typically when a mean is calculated it is important to know thevariance andstandard deviation about that mean. When a weighted meanμ{\displaystyle \mu ^{*}} is used, the variance of the weighted sample is different from the variance of the unweighted sample.

Thebiased weightedsample varianceσ^w2{\displaystyle {\hat {\sigma }}_{\mathrm {w} }^{2}} is defined similarly to the normalbiased sample varianceσ^2{\displaystyle {\hat {\sigma }}^{2}}:

σ^2 =i=1N(xiμ)2Nσ^w2=i=1Nwi(xiμ)2i=1Nwi{\displaystyle {\begin{aligned}{\hat {\sigma }}^{2}\ &={\frac {\sum \limits _{i=1}^{N}\left(x_{i}-\mu \right)^{2}}{N}}\\{\hat {\sigma }}_{\mathrm {w} }^{2}&={\frac {\sum \limits _{i=1}^{N}w_{i}\left(x_{i}-\mu ^{*}\right)^{2}}{\sum _{i=1}^{N}w_{i}}}\end{aligned}}}

wherei=1Nwi=1{\displaystyle \sum _{i=1}^{N}w_{i}=1} for normalized weights. If the weights arefrequency weights (and thus are random variables), it can be shown[citation needed] thatσ^w2{\displaystyle {\hat {\sigma }}_{\mathrm {w} }^{2}} is the maximum likelihood estimator ofσ2{\displaystyle \sigma ^{2}} foriid Gaussian observations.

For small samples, it is customary to use anunbiased estimator for the population variance. In normal unweighted samples, theN in the denominator (corresponding to the sample size) is changed toN − 1 (seeBessel's correction). In the weighted setting, there are actually two different unbiased estimators, one for the case offrequency weights and another for the case ofreliability weights.

Frequency weights

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If the weights arefrequency weights (where a weight equals the number of occurrences), then the unbiased estimator is:

s2 =i=1Nwi(xiμ)2i=1Nwi1{\displaystyle s^{2}\ ={\frac {\sum \limits _{i=1}^{N}w_{i}\left(x_{i}-\mu ^{*}\right)^{2}}{\sum _{i=1}^{N}w_{i}-1}}}

This effectively applies Bessel's correction for frequency weights. For example, if values{2,2,4,5,5,5}{\displaystyle \{2,2,4,5,5,5\}} are drawn from the same distribution, then we can treat this set as an unweighted sample, or we can treat it as the weighted sample{2,4,5}{\displaystyle \{2,4,5\}} with corresponding weights{2,1,3}{\displaystyle \{2,1,3\}}, and we get the same result either way.

If the frequency weights{wi}{\displaystyle \{w_{i}\}} are normalized to 1, then the correct expression after Bessel's correction becomes

s2 =i=1Nwii=1Nwi1i=1Nwi(xiμ)2{\displaystyle s^{2}\ ={\frac {\sum _{i=1}^{N}w_{i}}{\sum _{i=1}^{N}w_{i}-1}}\sum _{i=1}^{N}w_{i}\left(x_{i}-\mu ^{*}\right)^{2}}

where the total number of samples isi=1Nwi{\displaystyle \sum _{i=1}^{N}w_{i}} (notN{\displaystyle N}). In any case, the information on total number of samples is necessary in order to obtain an unbiased correction, even ifwi{\displaystyle w_{i}} has a different meaning other than frequency weight.

The estimator can be unbiased only if the weights are notstandardized nornormalized, these processes changing the data's mean and variance and thus leading to aloss of the base rate (the population count, which is a requirement for Bessel's correction).

Reliability weights

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If the weights are insteadreliability weights (non-random values reflecting the sample's relative trustworthiness, often derived from sample variance), we can determine a correction factor to yield an unbiased estimator. Assuming each random variable is sampled from the same distribution with meanμ{\displaystyle \mu } and actual varianceσactual2{\displaystyle \sigma _{\text{actual}}^{2}}, taking expectations we have,

E[σ^2]=i=1NE[(xiμ)2]N=E[(XE[X])2]1NE[(XE[X])2]=(N1N)σactual2E[σ^w2]=i=1NwiE[(xiμ)2]V1=E[(XE[X])2]V2V12E[(XE[X])2]=(1V2V12)σactual2{\displaystyle {\begin{aligned}\operatorname {E} [{\hat {\sigma }}^{2}]&={\frac {\sum \limits _{i=1}^{N}\operatorname {E} [(x_{i}-\mu )^{2}]}{N}}\\&=\operatorname {E} [(X-\operatorname {E} [X])^{2}]-{\frac {1}{N}}\operatorname {E} [(X-\operatorname {E} [X])^{2}]\\&=\left({\frac {N-1}{N}}\right)\sigma _{\text{actual}}^{2}\\\operatorname {E} [{\hat {\sigma }}_{\mathrm {w} }^{2}]&={\frac {\sum \limits _{i=1}^{N}w_{i}\operatorname {E} [(x_{i}-\mu ^{*})^{2}]}{V_{1}}}\\&=\operatorname {E} [(X-\operatorname {E} [X])^{2}]-{\frac {V_{2}}{V_{1}^{2}}}\operatorname {E} [(X-\operatorname {E} [X])^{2}]\\&=\left(1-{\frac {V_{2}}{V_{1}^{2}}}\right)\sigma _{\text{actual}}^{2}\end{aligned}}}

whereV1=i=1Nwi{\displaystyle V_{1}=\sum _{i=1}^{N}w_{i}} andV2=i=1Nwi2{\displaystyle V_{2}=\sum _{i=1}^{N}w_{i}^{2}}. Therefore, the bias in our estimator is(1V2V12){\displaystyle \left(1-{\frac {V_{2}}{V_{1}^{2}}}\right)}, analogous to the(N1N){\displaystyle \left({\frac {N-1}{N}}\right)} bias in the unweighted estimator (also notice that V12/V2=Neff{\displaystyle \ V_{1}^{2}/V_{2}=N_{eff}} is theeffective sample size). This means that to unbias our estimator we need to pre-divide by1(V2/V12){\displaystyle 1-\left(V_{2}/V_{1}^{2}\right)}, ensuring that the expected value of the estimated variance equals the actual variance of the sampling distribution. The final unbiased estimate of sample variance is:

sw2 =σ^w21(V2/V12)=i=1Nwi(xiμ)2V1(V2/V1),{\displaystyle {\begin{aligned}s_{\mathrm {w} }^{2}\ &={\frac {{\hat {\sigma }}_{\mathrm {w} }^{2}}{1-(V_{2}/V_{1}^{2})}}\\[4pt]&={\frac {\sum \limits _{i=1}^{N}w_{i}(x_{i}-\mu ^{*})^{2}}{V_{1}-(V_{2}/V_{1})}},\end{aligned}}}[6]

whereE[sw2]=σactual2{\displaystyle \operatorname {E} [s_{\mathrm {w} }^{2}]=\sigma _{\text{actual}}^{2}}. The degrees of freedom of this weighted, unbiased sample variance vary accordingly fromN − 1 down to 0. The standard deviation is simply the square root of the variance above.

As a side note, other approaches have been described to compute the weighted sample variance.[7]

Weighted sample covariance

[edit]

In a weighted sample, each row vectorxi{\displaystyle \mathbf {x} _{i}} (each set of single observations on each of theK random variables) is assigned a weightwi0{\displaystyle w_{i}\geq 0}.

Then theweighted mean vectorμ{\displaystyle \mathbf {\mu ^{*}} } is given by

μ=i=1Nwixii=1Nwi.{\displaystyle \mathbf {\mu ^{*}} ={\frac {\sum _{i=1}^{N}w_{i}\mathbf {x} _{i}}{\sum _{i=1}^{N}w_{i}}}.}

And the weighted covariance matrix is given by:[8]

C=i=1Nwi(xiμ)T(xiμ)V1.{\displaystyle \mathbf {C} ={\frac {\sum _{i=1}^{N}w_{i}\left(\mathbf {x} _{i}-\mu ^{*}\right)^{T}\left(\mathbf {x} _{i}-\mu ^{*}\right)}{V_{1}}}.}

Similarly to weighted sample variance, there are two different unbiased estimators depending on the type of the weights.

Frequency weights

[edit]

If the weights arefrequency weights, theunbiased weighted estimate of the covariance matrixC{\displaystyle \textstyle \mathbf {C} }, with Bessel's correction, is given by:[8]

C=i=1Nwi(xiμ)T(xiμ)V11.{\displaystyle \mathbf {C} ={\frac {\sum _{i=1}^{N}w_{i}\left(\mathbf {x} _{i}-\mu ^{*}\right)^{T}\left(\mathbf {x} _{i}-\mu ^{*}\right)}{V_{1}-1}}.}

This estimator can be unbiased only if the weights are notstandardized nornormalized, these processes changing the data's mean and variance and thus leading to aloss of the base rate (the population count, which is a requirement for Bessel's correction).

Reliability weights

[edit]

In the case ofreliability weights, the weights arenormalized:

V1=i=1Nwi=1.{\displaystyle V_{1}=\sum _{i=1}^{N}w_{i}=1.}

(If they are not, divide the weights by their sum to normalize prior to calculatingV1{\displaystyle V_{1}}:

wi=wii=1Nwi{\displaystyle w_{i}'={\frac {w_{i}}{\sum _{i=1}^{N}w_{i}}}}

Then theweighted mean vectorμ{\displaystyle \mathbf {\mu ^{*}} } can be simplified to

μ=i=1Nwixi.{\displaystyle \mathbf {\mu ^{*}} =\sum _{i=1}^{N}w_{i}\mathbf {x} _{i}.}

and theunbiased weighted estimate of the covariance matrixC{\displaystyle \mathbf {C} } is:[9]

C=i=1Nwi(i=1Nwi)2i=1Nwi2i=1Nwi(xiμ)T(xiμ)=i=1Nwi(xiμ)T(xiμ)V1(V2/V1).{\displaystyle {\begin{aligned}\mathbf {C} &={\frac {\sum _{i=1}^{N}w_{i}}{\left(\sum _{i=1}^{N}w_{i}\right)^{2}-\sum _{i=1}^{N}w_{i}^{2}}}\sum _{i=1}^{N}w_{i}\left(\mathbf {x} _{i}-\mu ^{*}\right)^{T}\left(\mathbf {x} _{i}-\mu ^{*}\right)\\&={\frac {\sum _{i=1}^{N}w_{i}\left(\mathbf {x} _{i}-\mu ^{*}\right)^{T}\left(\mathbf {x} _{i}-\mu ^{*}\right)}{V_{1}-(V_{2}/V_{1})}}.\end{aligned}}}

The reasoning here is the same as in the previous section.

Since we are assuming the weights are normalized, thenV1=1{\displaystyle V_{1}=1} and this reduces to:

C=i=1Nwi(xiμ)T(xiμ)1V2.{\displaystyle \mathbf {C} ={\frac {\sum _{i=1}^{N}w_{i}\left(\mathbf {x} _{i}-\mu ^{*}\right)^{T}\left(\mathbf {x} _{i}-\mu ^{*}\right)}{1-V_{2}}}.}

If all weights are the same, i.e.wi/V1=1/N{\displaystyle w_{i}/V_{1}=1/N}, then the weighted mean and covariance reduce to the unweighted sample mean and covariance above.

Vector-valued estimates

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Main article:Weighted least squares

The above generalizes easily to the case of taking the mean of vector-valued estimates. For example, estimates of position on a plane may have less certainty in one direction than another. As in the scalar case, the weighted mean of multiple estimates can provide amaximum likelihood estimate. We simply replace the varianceσ2{\displaystyle \sigma ^{2}} by thecovariance matrixC{\displaystyle \mathbf {C} } and thearithmetic inverse by thematrix inverse (both denoted in the same way, via superscripts); the weight matrix then reads:[10]

Wi=Ci1.{\displaystyle \mathbf {W} _{i}=\mathbf {C} _{i}^{-1}.}

The weighted mean in this case is:x¯=Cx¯(i=1nWixi),{\displaystyle {\bar {\mathbf {x} }}=\mathbf {C} _{\bar {\mathbf {x} }}\left(\sum _{i=1}^{n}\mathbf {W} _{i}\mathbf {x} _{i}\right),}(where the order of thematrix–vector product is notcommutative), in terms of the covariance of the weighted mean:Cx¯=(i=1nWi)1,{\displaystyle \mathbf {C} _{\bar {\mathbf {x} }}=\left(\sum _{i=1}^{n}\mathbf {W} _{i}\right)^{-1},}

For example, consider the weighted mean of the point [1 0] with high variance in the second component and [0 1] with high variance in the first component. Then

x1:=[10],C1:=[100100]{\displaystyle \mathbf {x} _{1}:={\begin{bmatrix}1&0\end{bmatrix}}^{\top },\qquad \mathbf {C} _{1}:={\begin{bmatrix}1&0\\0&100\end{bmatrix}}}
x2:=[01],C2:=[100001]{\displaystyle \mathbf {x} _{2}:={\begin{bmatrix}0&1\end{bmatrix}}^{\top },\qquad \mathbf {C} _{2}:={\begin{bmatrix}100&0\\0&1\end{bmatrix}}}

then the weighted mean is:

x¯=(C11+C21)1(C11x1+C21x2)=[0.9901000.9901][11]=[0.99010.9901]{\displaystyle {\begin{aligned}{\bar {\mathbf {x} }}&=\left(\mathbf {C} _{1}^{-1}+\mathbf {C} _{2}^{-1}\right)^{-1}\left(\mathbf {C} _{1}^{-1}\mathbf {x} _{1}+\mathbf {C} _{2}^{-1}\mathbf {x} _{2}\right)\\[5pt]&={\begin{bmatrix}0.9901&0\\0&0.9901\end{bmatrix}}{\begin{bmatrix}1\\1\end{bmatrix}}={\begin{bmatrix}0.9901\\0.9901\end{bmatrix}}\end{aligned}}}

which makes sense: the [1 0] estimate is "compliant" in the second component and the [0 1] estimate is compliant in the first component, so the weighted mean is nearly [1 1].

Accounting for correlations

[edit]
See also:Generalized least squares andVariance § Sum of correlated variables

In the general case, suppose thatX=[x1,,xn]T{\displaystyle \mathbf {X} =[x_{1},\dots ,x_{n}]^{T}},C{\displaystyle \mathbf {C} } is thecovariance matrix relating the quantitiesxi{\displaystyle x_{i}},x¯{\displaystyle {\bar {x}}} is the common mean to be estimated, andJ{\displaystyle \mathbf {J} } is adesign matrix equal to avector of ones[1,,1]T{\displaystyle [1,\dots ,1]^{T}} (of lengthn{\displaystyle n}). TheGauss–Markov theorem states that the estimate of the mean having minimum variance is given by:

σx¯2=(JTWJ)1,{\displaystyle \sigma _{\bar {x}}^{2}=(\mathbf {J} ^{T}\mathbf {W} \mathbf {J} )^{-1},}

and

x¯=σx¯2(JTWX),{\displaystyle {\bar {x}}=\sigma _{\bar {x}}^{2}(\mathbf {J} ^{T}\mathbf {W} \mathbf {X} ),}

where:

W=C1.{\displaystyle \mathbf {W} =\mathbf {C} ^{-1}.}

Decreasing strength of interactions

[edit]

Consider the time series of an independent variablex{\displaystyle x} and a dependent variabley{\displaystyle y}, withn{\displaystyle n} observations sampled at discrete timesti{\displaystyle t_{i}}. In many common situations, the value ofy{\displaystyle y} at timeti{\displaystyle t_{i}} depends not only onxi{\displaystyle x_{i}} but also on its past values. Commonly, the strength of this dependence decreases as the separation of observations in time increases. To model this situation, one may replace the independent variable by its sliding meanz{\displaystyle z} for a window sizem{\displaystyle m}.

zk=i=1mwixk+1i.{\displaystyle z_{k}=\sum _{i=1}^{m}w_{i}x_{k+1-i}.}

Exponentially decreasing weights

[edit]
See also:Exponentially weighted moving average

In the scenario described in the previous section, most frequently the decrease in interaction strength obeys a negative exponential law. If the observations are sampled at equidistant times, then exponential decrease is equivalent to decrease by a constant fraction0<Δ<1{\displaystyle 0<\Delta <1} at each time step. Settingw=1Δ{\displaystyle w=1-\Delta } we can definem{\displaystyle m} normalized weights by

wi=wi1V1,{\displaystyle w_{i}={\frac {w^{i-1}}{V_{1}}},}

whereV1{\displaystyle V_{1}} is the sum of the unnormalized weights. In this caseV1{\displaystyle V_{1}} is simply

V1=i=1mwi1=1wm1w,{\displaystyle V_{1}=\sum _{i=1}^{m}{w^{i-1}}={\frac {1-w^{m}}{1-w}},}

approachingV1=1/(1w){\displaystyle V_{1}=1/(1-w)} for large values ofm{\displaystyle m}.

The damping constantw{\displaystyle w} must correspond to the actual decrease of interaction strength. If this cannot be determined from theoretical considerations, then the following properties of exponentially decreasing weights are useful in making a suitable choice: at step(1w)1{\displaystyle (1-w)^{-1}}, the weight approximately equalse1(1w)=0.39(1w){\displaystyle {e^{-1}}(1-w)=0.39(1-w)}, the tail area the valuee1{\displaystyle e^{-1}}, the head area1e1=0.61{\displaystyle {1-e^{-1}}=0.61}. The tail area at stepn{\displaystyle n} isen(1w){\displaystyle \leq {e^{-n(1-w)}}}. Where primarily the closestn{\displaystyle n} observations matter and the effect of the remaining observations can be ignored safely, then choosew{\displaystyle w} such that the tail area is sufficiently small.

Weighted averages of functions

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The concept of weighted average can be extended to functions.[11] Weighted averages of functions play an important role in the systems of weighted differential and integral calculus.[12]

Correcting for over- or under-dispersion

[edit]
See also:§ Weighted sample variance

Weighted means are typically used to find the weighted mean of historical data, rather than theoretically generated data. In this case, there will be some error in the variance of each data point. Typically experimental errors may be underestimated due to the experimenter not taking into account all sources of error in calculating the variance of each data point. In this event, the variance in the weighted mean must be corrected to account for the fact thatχ2{\displaystyle \chi ^{2}} is too large. The correction that must be made is

σ^x¯2=σx¯2χν2{\displaystyle {\hat {\sigma }}_{\bar {x}}^{2}=\sigma _{\bar {x}}^{2}\chi _{\nu }^{2}}

whereχν2{\displaystyle \chi _{\nu }^{2}} is thereduced chi-squared:

χν2=1(n1)i=1n(xix¯)2σi2;{\displaystyle \chi _{\nu }^{2}={\frac {1}{(n-1)}}\sum _{i=1}^{n}{\frac {(x_{i}-{\bar {x}})^{2}}{\sigma _{i}^{2}}};}

The square rootσ^x¯{\displaystyle {\hat {\sigma }}_{\bar {x}}} can be called thestandard error of the weighted mean (variance weights, scale corrected).

When all data variances are equal,σi=σ0{\displaystyle \sigma _{i}=\sigma _{0}}, they cancel out in the weighted mean variance,σx¯2{\displaystyle \sigma _{\bar {x}}^{2}}, which again reduces to thestandard error of the mean (squared),σx¯2=σ2/n{\displaystyle \sigma _{\bar {x}}^{2}=\sigma ^{2}/n}, formulated in terms of thesample standard deviation (squared),

σ2=i=1n(xix¯)2n1.{\displaystyle \sigma ^{2}={\frac {\sum _{i=1}^{n}(x_{i}-{\bar {x}})^{2}}{n-1}}.}

See also

[edit]

Notes

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  1. ^Technically, negatives may be used if all the values are either zero or negatives. This fills no function however as the weights work asabsolute values.

References

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  1. ^abcdCochran, W. G. (1977). Sampling Techniques (3rd ed.). Nashville, TN: John Wiley & Sons.ISBN 978-0-471-16240-7
  2. ^abcdefghijklmnopqCarl-Erik Sarndal; Bengt Swensson; Jan Wretman (1992).Model Assisted Survey Sampling. Springer.ISBN 978-0-387-97528-3.
  3. ^Thomas Lumley (https://stats.stackexchange.com/users/249135/thomas-lumley), How to estimate the (approximate) variance of the weighted mean?, URL (version: 2021-06-08):https://stats.stackexchange.com/q/525770
  4. ^Gatz, Donald F.; Smith, Luther (June 1995). "The standard error of a weighted mean concentration—I. Bootstrapping vs other methods".Atmospheric Environment.29 (11):1185–1193.Bibcode:1995AtmEn..29.1185G.doi:10.1016/1352-2310(94)00210-C. -pdf link
  5. ^Endlich, R. M.; Eymon, B. P.; Ferek, R. J.; Valdes, A. D.; Maxwell, C. (1988-12-01)."Statistical Analysis of Precipitation Chemistry Measurements over the Eastern United States. Part I: Seasonal and Regional Patterns and Correlations".Journal of Applied Meteorology and Climatology.27 (12):1322–1333.Bibcode:1988JApMe..27.1322E.doi:10.1175/1520-0450(1988)027<1322:SAOPCM>2.0.CO;2.
  6. ^"GNU Scientific Library – Reference Manual: Weighted Samples".Gnu.org. Retrieved22 December 2017.
  7. ^"Weighted Standard Error and its Impact on Significance Testing (WinCross vs. Quantum & SPSS), Dr. Albert Madansky"(PDF).Analyticalgroup.com. Retrieved22 December 2017.
  8. ^abPrice, George R. (April 1972)."Extension of covariance selection mathematics"(PDF).Annals of Human Genetics.35 (4):485–490.doi:10.1111/j.1469-1809.1957.tb01874.x.PMID 5073694.S2CID 37828617.
  9. ^Mark Galassi, Jim Davies, James Theiler, Brian Gough, Gerard Jungman, Michael Booth, and Fabrice Rossi.GNU Scientific Library - Reference manual, Version 1.15, 2011.Sec. 21.7 Weighted Samples
  10. ^James, Frederick (2006).Statistical Methods in Experimental Physics (2nd ed.). Singapore: World Scientific. p. 324.ISBN 981-270-527-9.
  11. ^G. H. Hardy, J. E. Littlewood, and G. Pólya.Inequalities (2nd ed.), Cambridge University Press,ISBN 978-0-521-35880-4, 1988.
  12. ^Jane Grossman, Michael Grossman, Robert Katz.The First Systems of Weighted Differential and Integral Calculus,ISBN 0-9771170-1-4, 1980.

Further reading

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  • Bevington, Philip R (1969).Data Reduction and Error Analysis for the Physical Sciences. New York, N.Y.: McGraw-Hill.OCLC 300283069.
  • Strutz, T. (2010).Data Fitting and Uncertainty (A practical introduction to weighted least squares and beyond). Vieweg+Teubner.ISBN 978-3-8348-1022-9.

External links

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