Scalar rescaling invariance of a tie-line weight matrix means that multiplying every fit weight by the same positive number leaves the fitted phase fraction unchanged. Let endpoint compositions and overall composition be expressed in independent mole fraction coordinates. With , a fixed symmetric positive-definite matrix defines the tie-line phase-fraction fit by minimizingFor , . Multiplication by a positive constant preserves every comparison between objective values, so the sets of minimizers agree. The proof also applies when the same constraint is imposed in both fits.
For distinct endpoints, the unconstrained formula makes the cancellation visible:The differential in sensitivity of a tie-line fit to its weight matrix agrees: for a perturbation , its numerator is by the fit's normal equation. Thus the scalar direction is insensitive even when the residual is nonzero.
In an original example, take , , and . The remaining composition coordinate is fixed by closure. These values giveReplacing by gives the same fraction, although the minimum objective increases from0.00072to0.00504. Changing only the second diagonal weight from4to7 instead changes the fitted fraction to0.640625. Relative weights determine the geometry; their common multiplier does not.
Point-estimate invariance does not by itself establish invariance of physical measurement uncertainty. Merely rewriting the same objective with leaves propagation through the same measured-input covariance matrix unchanged. If instead represents absolute precision and asserts a genuinely different covariance , that is a different noise model. With exact endpoints, the linear-model variance then decreases by a factor . The measurement model and covariance interpretation must be stated.[ref]
Guide to the expression of uncertainty in measurement by JCGM. Sections 5.1.3 and 5.2.2, model sensitivities and covariance propagation; tie-line result derived here
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