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We describe how the cytoskeleton and extracellular matrix form a single, tensionally integrated structural system as predicted by tensegrity, and how distinct molecular biopolymers (e.g., microfilaments vs microtubules) may bear either tensile or compressive loads inside the cell.
Hence the chosen rows and columns in the original data matrix form a solid block when combined.
After rearranging the dynamic stiffness matrix of the segment model in transfer matrix form, a periodicity condition is applied leading to an eigenvalue problem.
Now, when we assume a r ( k ) = 0 for r > N, the system (2.14) can be transformed into the matrix form, A ( k + 1 ) = D A ( k ), k = 0, 1, …, n. (2.15).
The optical observation of the molecular interdiffusion is possible owing to the mixing-induced solid state transition to the rotator phase; the molecularly mixed region and the low-temperature phase matrix form a sharp interphase boundary which is visible under the polarized microscope.
We can equivalently write EVD of a para-Hermitian matrix and SVD of a polynomial matrix in coefficient matrix form A [ n ] = U [ n ] ∗ Λ [ n ] ∗ U H [ − n ] (4) A [ n ] = U [ n ] ∗ Σ [ n ] ∗ V H [ − n ] (5). in which, U[n], V[n], Λ[n], and Σ[n] are the coefficient matrices corresponding to U z), V z), Λ z), and Σ z).
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The covariance matrix, which is symmetric positive definite matrix, forms a Riemannian manifold.
Moreover, cells had migrated deep into the matrix, forming a three dimensional, branched and interconnected cell community.
The piezoelectric particles are then fully surrounded by the polymer matrix, forming a so-called 0 3 composite (Newnham et al., 1978).
The commercial polysiloxane (S) on both stones penetrates into the crystalline matrix, forming a very thin layer which covers homogeneously the stone crystals (Fig. 5a c).
In sample 1, round-shaped Fe-Ni-S inclusions dispersed in the olivine matrix, forming a load-bearing framework (LBF) texture.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com