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Several numerical examples without interfacial debonding show the applicability of the virtual matrix concept to elastoplastic materials.
The virtual matrix is an elastic material in which real matrix material and inhomogeneities are embedded, and its volume vanishes as a limit after homogenization.
This bleak atmosphere, the creepy man-machine pattern embodied in the "brain-computer interface," and the virtual "Matrix" where the action takes place, comprise the foundational elements of the "cyberpunk" aesthetic.
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With regard to elasticity, depending on the choice of material properties of this virtual matrix, many kinds of average moduli between the classical bounds can be predicted.
The channel matrix can be assumed as the virtual channel matrix of user after precoding.
The matrix H v = G v HF v = diag σ1,..., σ b ) is the virtual channel matrix of size b × b, σ i stands for every subchannel gain (sorted by decreasing order), v v = G v v is the virtual noise, G v and F v are unitary matrices obtained from applying the SVD operation on the channel matrix.
Also: A post at the New APPS blog explains the so-called simulation hypothesis, which says we are significantly likelier to be living in a virtual (Matrix) world than the ordinary physical world.
We show how to compute the spectrum of these matrices by using "virtual" matrix elements and characteristic operator functions.
Here "virtual matrix" H v is the combination of two codes H without "cross constraint" (edge between nodes from different codes in Tanner Graph) between each other.
The frequency equation of the fluid plate system is derived by combining mass, stiffness, and the virtual mass matrix.
H v is the virtual channel matrix, whose elements represent subchannel gains arranged in a descending order.
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