Titlebook: Non-Fourier Heat Conduction; From Phase-Lag Model Alexander I. Zhmakin Book 2023 The Editor(s) (if applicable) and The Author(s), under exc

錯事

Alexander I. Zhmakinr structural elements to form distinct RNA–protein complexes. Since these complexes are required for the normal regulation of gene expression, mutations that alter RBP functions may result in a cascade of deleterious events that lead to severe disease. Here, we focus on a group of hereditary disorde

Ganglion

Alexander I. Zhmakintumors can be controlled by a primary tumor with/without a surgery and the microenvironment. This control system is composed of fibroblast growth factor-2 (FGF2), urokinase-type plasminogen activator (uPA), plasmin, transforming growth factor-beta (TGFβ), latent TGFβ (LTGFβ), and tumor density. The

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雄辯

Phase-Lag Modelsl–Cattaneo–Vernotte equation, the dual-phase-lag model and the triple-phase-lag model (that introduce two and three relaxation times, respectively) as well as their non-local modifications and the compatibility of the phase-lag models with the second law of thermodynamics are considered.

follicular-unit

Phonon Modelsiption of the phonon transport regimes the Guyer–Krumhansl equation, the two-fluid models, the ballistic–diffusive and the extended ballistic–diffusive models, the unified non-diffusive-diffusive model, the generalized Fourier law by Hua et al., phonon hydrodynamics, flux-limited behaviour and relax

STELL

Thermomass Modelics is considered as well as the equation of states of the thermon gas in different media (ideal gas, dielectric, metals). The equations of motion of the thermon gas and the heat flow choking phenomenon are discussed.

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Mesoscopic Moment Equationsrgamasko who introduced the additional . moments to derive the two-moment and the three-moment systems that are simpler than the microscopic integro-differential Boltzmann transport equation for the phonon distribution function is briefly discussed.

Robust

Androgen

Thermodynamic Modelszation of the entropy density under the constraints of the state variables with the Lagrange multipliers is considered, in particularity, the approaches exploited by Jou & Cimmelli, by Sellitto & Cimmelli, by Kovács & Ván, by Rogolino et al. and extended ballistic–diffusive model are discussed.

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