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Θ = {ΘU,ΘV,ΘZ}, where ∀F ∈ {U,V,Z},ΘF = {µF,ΣF} Finding a good value for Θ is a difficult task, even if we assume that the prior means are zero and the covariances spherical Another concern is that information between entities can only be shared indirectly, through.

Fu vz. The invariant I is always zero when the assumption of incompressibility is made For the shear flows discussed in Section 1, both I and III are zero and I I = γ yx 2 = (d v x / d y) 2For the shearfree flows of Section 2, the invariant I is zero, II = (6 2b 2)ɛ̇ 2 and III = (6−6b 2)ɛ̇ 3Another quantity often used is the magnitude of the rate of strain tensor γ = (1 / 2) I. ó X v } Z ï î r v } v Z Æ u o P î ñ ^ µ u u Ç v Æ u o. & v Z À o µ } ( Z } P v o ( µ v } v Z } v B s ;.

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