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Discrete steps involved in traveling from the origin to a given response, y,.

Discrete steps involved in traveling from.the origin to a given response, i i,.

Discrete supramolecular metal complexes. Synthesis of catenaries, knots adapted from P. Mobian, J.-M. Kern, and J.-P, Sauvage. J. Am. Chem. Soc. 125

Discrete system.

Discrete Time Markov Chain representing the p-automaton for the case study.

Discrete time-domain vibration curves

Discrete variables used in difference equations

Discrete-appended receptors

Discrete-dynode electron multiplier. When the ions hit the surface of the detector electrons are emitted to form an avalanche of electrons which generates the signal.

Discrete-time simulation of the ideal, lossy waveguide. Each per-sample loss factor g may be pushed through delay elements and combined with other loss factors until an input or output is encountered which inhibits further migration. If further consolidation is possible on the other side of a branching node, a loss factor can be pushed through the node by pushing a copy into each departing branch. If there are other inputs to the node, the inverse of the loss factor must appear on each of them. Similar remarks apply to pushing backwards through a node.

Discretely changing cross-section geometries and resulting braid stmcture .

Discretised Wheel and Elliptical Contact Co-ordinate Systems

Discretization of a cylindrical battery for finite differences simulation and reduction to a radial ID heat transfer problem.

Discretization of a transmission-line model of a porous electrode or diffusion process.

Discretization of HEB 220 section to fibers

Discretization of the boundary

Discretization of the convex cross-section beam with shell finite elements.

Discretization of the domain with approximating functions.

Discretization of the forecast area and indexing of nodal blocks in finite differences grid relative point I, J .

Discretization of the Kadanoff-Baym contour y in the complex-time plane.

Discretization of the net balance state space.

Discretization of the problem domain

Discretization of the simulated domain. Numbers in the boxes are cell numbers.

Discretization of the Tube and Exciter Coil

Discretization scheme used for the solution of the PNP equations. Values of the current density are computed at the points designated by empty circles the potential and charge density values are computed at points corresponding to the filled circles.



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