Variance, covariance and correlation
For square-integrable real X,Y, Var X=E[(X−EX)²] and Cov(X,Y)=E[(X−EX)(Y−EY)].
Key knowledge
For square-integrable real X,Y, Var X=E[(X−EX)²] and Cov(X,Y)=E[(X−EX)(Y−EY)]. If both variances are positive, Corr=Cov/√(Var X Var Y) lies in [−1,1]. Independence gives zero covariance; its converse generally fails.
Conditions and scope
- Finite second moments are required.
- Correlation measures linear association and does not establish a causal relation.
Sources · 1
References
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Evidence and review
Sections 18.1–18.3 covariance formula, normalized correlation and independence distinction.
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- Uses definition
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Linked statements
- For square-integrable real X,Y, Var X=E[(X−EX)²] and Cov(X,Y)=E[(X−EX)(Y−EY)]. If both variances are positive, Corr=Cov/√(Var X Var Y) lies in [−1,1]. Independence gives zero covariance; its converse generally fails.
- Uses definition
Relationship sources · 1
Linked statements
- For square-integrable real X,Y, Var X=E[(X−EX)²] and Cov(X,Y)=E[(X−EX)(Y−EY)]. If both variances are positive, Corr=Cov/√(Var X Var Y) lies in [−1,1]. Independence gives zero covariance; its converse generally fails.
- Uses definition
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Linked statements
- For square-integrable X, Var(X)=E[Var(X|Y)]+Var(E[X|Y]). The terms separate average within-condition variation from variation of the conditional mean.
- Uses definition
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- M_X(t)=E[eᵗˣ] is an MGF when it is finite on an open interval about zero. Its derivatives at zero yield moments; in particular EX=M′(0) and Var X=M″(0)−[M′(0)]².
- Uses definition
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- For estimator T of θ, bias is EθT−θ and MSE is Eθ[(T−θ)²]=Varθ(T)+bias². Unbiasedness means zero bias at every allowed θ and does not itself imply a small error or consistency.
- Uses definition
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- For fixed full-column-rank X and Y=Xβ+ε with Eε=0 and Cov ε=σ²I, least squares gives β̂=(XᵀX)⁻¹XᵀY, Eβ̂=β and Cov β̂=σ²(XᵀX)⁻¹. Independent normal errors additionally make β̂ exactly multivariate normal.
- Uses definition
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- Residuals eᵢ=yᵢ−f(xᵢ;β̂) compare observed and fitted responses. Patterns against predictors, fitted values or run order can expose functional misspecification, changing variance or dependence. A high R² does not certify model adequacy.
- Uses definition
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- A rate-λ Poisson counting process starts at zero, has independent increments and N(t+s)−N(s) distributed Poisson(λt). Successive interarrival times are independent exponentials of rate λ; EN(t)=Var N(t)=λt.
- Uses definition
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- Standard Brownian motion has B(0)=0, almost surely continuous paths and independent increments with B(t)−B(s)∼N(0,t−s) for 0≤s<t. It is a mean-zero Gaussian process with Cov(B(s),B(t))=min(s,t).
- Uses definition
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- The sum of squares of k independent standard normal variables has chi-square law χ²ₖ=Gamma(k/2,1/2), with mean k and variance 2k.
- Uses definition
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- For nonnegative X with finite mean and a>0, P(X≥a)≤E[X]/a. For finite-variance Y and t>0, P(|Y−E[Y]|≥t)≤Var(Y)/t², by applying the first bound to (Y−E[Y])².
- Uses definition
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- NIST/SEMATECH e-Handbook: Calibration of future measurements ↗
- NIST/SEMATECH e-Handbook: Uncertainty of calibrated values ↗
- NIST/SEMATECH e-Handbook: Propagation of calibration errors ↗
Linked statements
- For the valid linear calibration y=a+bx, an unknown input is estimated as x̂=(y₀−â)/b̂. Its uncertainty includes the future indication, fitted intercept/slope, their covariance, reference standards and applicable extra influences. First-order propagation uses gradient (1/b̂,−1/b̂,−x̂/b̂) with respect to (y₀,â,b̂).
Intercept/slope dependence and any future-indication dependence must remain in the covariance matrix.
- Derived from
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Linked statements
- For repeated indications, the mean has variance Var(x̄)=(1/n²)Σ_iΣ_j Cov(x_i,x_j). It reduces to σ²/n for independent equal-variance observations; shared offsets, temporal correlation and drift can prevent the usual square-root improvement from averaging.
Mean variance is a double sum of sample covariance; the independent 1/N law is only a specialization.
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- For a differentiable real model Y=f(X), first-order output covariance is Σ_Y≈JΣ_XJᵀ, J_ai=∂f_a/∂x_i at the input estimate; the rule is exact for an affine model with finite input covariance. For impedance inferred from voltage/current amplitudes and phase, R=V cosφ/I and X_r=V sinφ/I share the same uncertain inputs, so their covariance must be retained as well as their separate uncertainties.
An affine transformed vector has exactly JΣJᵀ covariance; nonlinear use requires an adequately controlled local approximation.
- Related to
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- Experimental Design Assistant, Experimental Unit ↗
- Key Elements of a Well-Designed Experiment, randomization and blinding ↗
Linked statements
- The experimental unit is the entity independently assigned to a treatment in a specified design. Multiple observations from one treated unit need an appropriate within-unit analysis and do not automatically increase the number of independent treatment replicates. Defining units, randomization and masking helps relate biological variability and measurement variability to the intended inference.
Dependence affects variance of an estimated response.
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- In a specified population model, narrow-sense heritability is the ratio of additive genetic variance to phenotypic variance. Genetic effects, environment and their interactions contribute to trait variation. Heritability depends on the sampled population and environment; it is not the fraction of one individual's trait caused by genes.
The variance decomposition requires stated covariance assumptions.
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- Species traits can be correlated because related lineages share evolutionary history. Under an explicit Brownian trait model on a timed tree, shared branch history determines expected covariance; independent-contrast or likelihood methods account for that structure instead of treating every tip as an independent observation. Tree/model uncertainty and measurement error affect the resulting rate or association inference.
Shared history creates off-diagonal covariance.
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- PCA finds an orthogonal low-rank subspace minimizing squared reconstruction error for centered observations. Leading covariance eigenvectors solve this objective; scale choices and outliers change the subspace. Large explained variance need not carry the target signal, and a low-dimensional representation does not establish causal factors. Identifiability can fail when relevant eigenvalues repeat.
Covariance structure determines the selected directions.
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- A precision Standard Model fit compares predicted electroweak observables with correlated measurements, jointly propagating input-parameter, systematic and missing-order uncertainties. The inspected PDG review uses a declared renormalization convention and assumptions such as lepton universality. A residual or an excluded input tests that specific model/fit construction; it is not automatically evidence for a unique new particle.
Correlated likelihoods require the full covariance structure.
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- For constant-density incompressible flow, averaging u=U+u′ adds the Reynolds stress R_ij=⟨u′_iu′_j⟩ to the mean momentum equation. Its transport introduces higher correlations, so averaging does not close the equations. Eddy-viscosity, Reynolds-stress and data-informed closures encode different assumptions; a fitted mean velocity alone does not validate every stress or transient.
Velocity correlations are tensor covariance components.
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- For a vector measurand Y=f(X), propagating a joint input distribution retains output dependence and non-Gaussian shape. Local U_Y≈J U_X Jᵀ is only a linearization. For the explicit X∼N(0,u²), Y=(X,X²), Cov(Y₁,Y₂)=0 although the outputs are dependent; a covariance matrix alone need not specify their joint distribution.
Zero covariance is weaker than independence.
- Related to
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- JCGM GUM-6:2020 · Developing measurement models ↗
- Statistical methods for next-generation clock networks (2025 project update) ↗
Linked statements
- For linear observations z=Aθ+ε with known positive-definite covariance Σ and full-column-rank A, generalized least squares yields θ̂=(AᵀΣ⁻¹A)⁻¹AᵀΣ⁻¹z. Shared reference, environmental and transfer errors create off-diagonal covariance; they do not average away as independent scatter. Fix an identifiable reference/gauge and model synchronization separately.
Common uncertainty enters a joint covariance matrix.
- Uses definition
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Linked statements
- For y = f(x₁,…,xₙ), first-order propagation weights input variances and covariances by the model's sensitivity coefficients. Correlations must be retained when the input estimates are correlated.
The uncertainty rule uses the joint covariance of input quantities. Finite covariance in the declared measurement model; retain shared dependencies.
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