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Method agreement — Examples

1 · Prerequisites

2 · Summary

The examples show a constant method offset hidden by perfect correlation and a finite repeated-measures model whose shared random intercept makes paired differences dependent. Both calculations keep the population/model assumptions visible and do not claim endpoint coverage or empirical interchangeability.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

ExampleConstruction: AI-generatedVerification: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

Perfect correlation can coexist with a method offset

Example

Let Ω={0,1} have probability 1/2 at each point, and let two methods on the same target report A(ω)=ω and B(ω)=ω+c for a fixed c>0. Their correlation is 1, but their difference is the nonzero constant −c and their conventional limits of agreement both equal −c.

Facts & Assumptions

Given: Ω={0,1} with weights 1/2,1/2, A(ω)=ω, B(ω)=ω+c, and c>0. For this example define Corr⁡(A,B):=Cov⁡(A,B)Var⁡(A)Var⁡(B).

[F1]

For D=A−B, the bias is E[D], the spread is Var⁡(D), and conventional limits are their mean plus or minus 1.96 times that spread. Method agreement and limits of agreement

[F2]

Variance and covariance are expectations of the centered square and centered product. Moments, variance, and covariance on a probability space

[F3]

On a finite probability space, expectation is the weighted sum of values over its atoms. Expectation agrees with the published finite weighted sum

[F4]

Covariance is symmetric and bilinear on finite linear combinations, including constant summands. Covariance is symmetric and bilinear in finite linear combinations

Verification

Given: The two-point probability model and method values in the Example. Verify the correlation and limits.

1.1F2F3F4givenalgebra

By [F3], E[A]=1/2 and E[B]=1/2+c. Directly summing the two centered squares gives Var⁡(A)=Var⁡(B)=1/4. By [F4], Cov⁡(A,B)=Cov⁡(A,A+c)=Var⁡(A)+Cov⁡(A,c)=1/4, since covariance with a constant is zero. Thus the denominator in the definition of correlation is 1/4 and Corr⁡(A,B)=1.

1.2F1F2F3algebra

At both points D=A−B=−c, so by [F2] and [F3], E[D]=−c and Var⁡(D)=0. Hence its conventional limits are −c±1.96⋅0=(−c,−c), while its bias is nonzero.

2.1step 1.1step 1.2given∎

Therefore perfect correlation does not imply zero bias or interchangeable measurements; any practical tolerance must be supplied for the intended use.

ExampleConstruction: AI-generatedVerification: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

Repeated method differences can share a random intercept

Example

Let Ω={−1,1}3 have uniform probability, and let U,ϵ1,ϵ2 be its coordinate variables. For two repeated paired measurements on one target, suppose the differences follow the random-intercept model Dj=U+ϵj, j=1,2. Then each difference has mean 0 and variance 2, but Cov⁡(D1,D2)=1. In fact, P(D1=2,D2=2)=18≠116=P(D1=2)P(D2=2). The repeated differences are dependent and hence are not an iid sample.

Facts & Assumptions

Given: The eight equally likely triples in Ω, coordinate functions U,ϵ1,ϵ2, and differences Dj=U+ϵj.

[F1]

Independent random elements are those whose generated sigma-algebras are independent. Independent random elements

[F2]

An iid family is independent and has a common law. Identical distribution and IID families

[F3]

Finite-space expectations are weighted sums over atoms. Expectation agrees with the published finite weighted sum

[F4]

Variance and covariance are the expectations of centered squares and centered products. Moments, variance, and covariance on a probability space

[F5]

Covariance is bilinear on finite linear combinations. Covariance is symmetric and bilinear in finite linear combinations

[F6]

Independent square-integrable real random variables have zero covariance. Independence forces covariance to vanish

Verification

Given: Ω={−1,1}3 with uniform weights and Dj=U+ϵj. Verify the marginal moments and the within-target dependence.

1.1F1F3F4givenalgebra

Each triple has mass 1/8=(1/2)3, so for arbitrary subsets S1,S2,S3⊆{−1,1}, P(U∈S1,ϵ1∈S2,ϵ2∈S3)=∏j=13∣Sj∣/2. Thus [F1] makes the coordinates independent. Each coordinate has mean 0 and variance 1 by the finite weighted sum [F3] and centered-square definition [F4].

2.1F3F4F5F6step 1.1algebra

By [F5] and [F6], E[Dj]=0, Var⁡(Dj)=Var⁡(U)+Var⁡(ϵj)+2Cov⁡(U,ϵj)=2, and Cov⁡(D1,D2)=Var⁡(U)=1; all cross terms vanish because they are covariances of distinct independent coordinates.

3.1F1F2F3givenalgebra∎

The event D1=D2=2 requires the single triple (1,1,1), so its probability is 1/8. Each event Dj=2 requires U=1 and ϵj=1 and has probability 1/4, making the product of marginal probabilities 1/16. The factorization required for independence therefore fails; by [F2] the two differences are not iid.