Repeat-count targets under shared model error choose how many independent readings are worth averaging when part of the uncertainty is common to every repeat. In the local measurement model Xi=S+D+ϵi, let the shared discrepancy have variance τ2, and the independent repeat noise have variance σ2. Assuming the two components are independent,The common term produces covariance between readings and survives averaging. The GUM's correlated-input rule retains precisely such shared contributions.[ref]
un2=Var(X)=τ2+nσ2.
For a desired total standard uncertainty u∗>τ, solve the inequality before choosing the integer repeat count:If σ>0, a target equal to τ cannot be attained with any finite repeat count, and a target below τ is unattainable within this model. This is the feasibility threshold for averaging under shared uncertainty.
n≥u∗2−τ2σ2,nmin=max{1,⌈u∗2−τ2σ2⌉}.
In an original body surface area example, take σ=0.04m2 and τ=0.08m2. A target u∗=0.081m2 needs ten repeats; u∗=0.0801m2 needs one hundred. A target of 0.079m2 instead requires reducing the shared component or changing the model. Merely collecting more readings is insufficient.
Two relative criteria illustrate why the target must be explicit. Requiring repeat-noise variance to be at most ητ2 gives n≥σ2/(ητ2): at η=0.01, 25 repeats suffice. Requiring total standard uncertainty within 1% of its floor instead giveswhich needs 13 repeats with the same stipulated numbers. A 1% variance criterion and a 1% standard-uncertainty criterion are different requirements.
n≥τ2[(1.01)2−1]σ2,
The calculation assumes independent repeat noise and a justified shared-error model. Repeated observations alone cannot estimate an individual fixed discrepancy; independent reference measurements or a suitable validation population are needed to constrain it.
A feasibility threshold for averaging under shared uncertainty is the smallest uncertainty that repetition can approach while a common uncertain contribution remains unchanged. In the measurement model Xi=S+D+ϵi, suppose the shared term has variance τ2 and independent repeat noise has variance σ2. ThenFor σ>0, every finite repeat count has un>τ, although un tends to τ as n grows. A target below the floor is infeasible within this model, and a target exactly at it needs an infinite count. The GUM's correlated-input propagation explains why a common contribution is retained rather than divided by the repeat count.[ref]
un=τ2+σ2/n.
Approaching the floor has a quantifiable cost. To obtain un≤τ(1+δ) with τ>0, solveFor small positive δ, the required count grows approximately as 1/δ. With stipulated σ=0.04m2 and τ=0.08m2, getting within 1% of the floor needs 13 repeats, within 0.1% needs 125, and within 0.01% needs 1,250. These are planning examples for body surface area prediction, not observed clinical performance limits.
n≥τ2(2δ+δ2)σ2.
Precision limits of weighting correlated repeats show why a clever average cannot remove the common term for free. A linear estimate S=∑iwiXi that preserves the unknown S requires ∑iwi=1. The shared discrepancy therefore enters with coefficient one as well, givingThe inequality follows from ∑iwi2≥1/n; equal weights attain it under the stipulated equal independent repeat-noise variances. Negative weights do not evade the floor while preserving the signal coefficient.
Var(S)=τ2+σ2∑iwi2≥τ2+nσ2.
Reaching a lower uncertainty requires additional information or a changed measurement model that reduces the common contribution. Repeating a validation method with genuinely independent reference errors can supply different information, whereas repeating one person's height and mass measurements does not redraw that person's model discrepancy. A known bias calls for a correction, not a claim that averaging will make it disappear.[ref]
Guide to the expression of uncertainty in measurement by JCGM. §4.1.2, corrections and incomplete knowledge in a measurement model
Precision limits of weighting correlated repeats describes what a weighted mean can achieve when repeated observations share an uncertain contribution. Supposewith independent, zero-mean repeat errors ϵi independent of D. An estimate S=∑iwiXi must satisfy ∑iwi=1 to preserve the unknown signal S. The shared contribution then has coefficient one as well:This is a special case of correlated-input measurement uncertainty propagation. The covariance matrix is Σ=τ211T+diag(σi2); omitting its off-diagonal terms would incorrectly treat the common uncertainty as independently redrawn.[ref]
Xi=S+D+ϵi,Var(D)=τ2,Var(ϵi)=σi2>0,
Var(S)=τ2+∑iwi2σi2.
The Cauchy-Schwarz inequality gives a sharp bound:Equality occurs for inverse-variance weighting,For equal repeat variances this reduces to equal weights and umin2=τ2+σ2/n. Allowing negative weights cannot improve this bound within the stated model.
1=(∑i(wiσi)σi−1)2≤(∑iwi2σi2)(∑iσi−2).
wi=∑jσj−2σi−2,umin2=τ2+∑iσi−21.
For an original body surface area prediction example, take shared standard uncertainty τ=0.050m2 and two repeat-noise values σ1=0.040m2 and σ2=0.080m2. The optimal weights are 0.8 and 0.2, giving umin=0.0025+0.00128≈0.0615m2. Equal weights give approximately 0.0671m2. Weighting helps, but it does not erase the shared 0.050m2 contribution. These values are stipulated, not clinical performance data.
For a fixed individual, D can represent an unknown constant model discrepancy rather than a fluctuation between readings. No weights summing to one can distinguish that discrepancy from S, because both enter every observation identically. Independent reference information or a better anatomical measurement model is required to constrain it. If the residual errors themselves have further covariance, their full matrix replaces the diagonal repeat-noise model; the displayed inverse-variance weights no longer follow automatically.
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