Exact(1)
From the GMMr model an irreversible alternative is established by setting all product concentrations to zero.
Similar(58)
TACs were analysed using six plasma input models: a reversible single-tissue model (1T2k), an irreversible two-tissue model (2T3k), and a reversible two-tissue model (2T4k), all three both with and without additional blood volume parameter (V B) [18].
We have tested four different compartmental models: (a) irreversible uptake of tracer in a single non-vascular compartment, (b) reversible tissue uptake, (c) reversible uptake of tracer in the first non-vascular compartment from which tracer was irreversibly taken up in a second non-vascular compartment and (d) reversible uptake of tracer in the first and second non-vascular compartments.
After describing several such models, we will concentrate on the model, called an irreversible k-threshold process, where a vertex enters state 1 if at least k of its neighbors are in state 1, and where a vertex never leaves state 1 once it is in it.
Finally we derive the formulation of the balance equations of a CSTR model as an Irreversible Port-Hamiltonian System and give two alternative lifts of the CSTR model to a control contact system defined on the complete Thermodynamic Phase Space.
Within this framework, an irreversible interface model is developed for the one-dimensional case and subsequently extended to three-dimensional transverse isotropy.
A generalized model of an irreversible thermal Brownian microscopic heat pump is established in this paper.
It is defined as the heat-pumping load divided by the total cost per unit time and its expression is derived from the general cycle model of an irreversible heat-transformer.
A generalized model of an irreversible thermal Brownian refrigerator, which consists of Brownian particles moving in a periodic sawtooth potential with external forces and contacting with the alternating hot and cold reservoirs along the space coordinate, is established in this paper.
A thermodynamic model of an irreversible Carnot refrigerator with heat recovery (CRHR) working between two high temperature reservoirs (TH and TR) and one low temperature heat reservoir (TL) has been established in this paper for optimization of allocation of heat transfer areas.
A general model of an irreversible Ericsson refrigeration cycle employing paramagnetic materials as the working substance is presented, in which multi-irreversibilities such as finite-rate heat transfer, regenerative loss, heat leak, efficiency of regenerator and internal irreversibility resulting from magnetic working substances are taken into account.
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