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Elliott et al. [ 70] developed an elemental model of the cochlea in order to analyse the interaction between the fluid coupling and BM motion and represented the cochlear mechanics by defining a single longitudinal variable for the pressure difference and for the BM velocity.
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Changing the elemental properties in the finite element model of the microstructure is performed based on this sensitivity analyses and by imposing volume constraints on the constituent phases.
Elemental models of compound processing predict a preference for the non-trained stimulus AC while configural models predict a preference for the trained stimulus BC.
Chemical Engineering Science 60, 4083 4091] developed a discrete elemental model to simulate the mixing of solids in a rotary kiln.
This kind of elemental model was used, for example, by Neely and Kim [ 19], to simulate an early model of the active cochlea, and has been used by many authors since then.
Although the finite element cochlear model is an elemental representation of the real continuous cochlea, the flexibility of the finite elements allows the possibility of considering more detailed and complicated cochlear structure than in the elemental model above.
Different proposals of elemental models to get analytical expressions of energy of Si-nC are found in the literature, which pretend to explain correctly the energy spectrum of this type of nanostructures.
A numerical model of the type used in repository performance assessments was developed for elemental transport at the site.
The elemental values of the model are determined by cross-sectional areas A1 ⋯ A n and cylinder lengths l1 ⋯ l n.
The elemental basis of the model is a discrete "fault" along an internal weak interface, constrained at its ends by an elastic matrix and subject to frictional sliding, in the subsurface zone of high shear stress in the Hertzian field.
As described in Section 2.1.2 (elemental cochlear model), the linear coupled behaviour of the cochlear dynamics can be represented by two separate phenomena: the way that the pressure distribution is determined by the fluid coupling within the cochlear chambers when driven by the BM velocity and the way in which the BM dynamics respond to the imposed distribution of pressure difference.
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