Real Solid and Liquid Bodies

Author(s):  
Wolfgang Demtröder
Keyword(s):  
2021 ◽  
Vol 10 (1) ◽  
pp. 23
Author(s):  
Luca Masucci ◽  
Gianluca Quaranta

The gut microbiota is composed of trillions of different microorganisms: bacteria, archaea, phages and protozoa, which represent a real solid organ, with an approximate weight of 2 kg [...]


2013 ◽  
Vol 2013 ◽  
pp. 1-14 ◽  
Author(s):  
Oldřich Coufal

The concepts of resistance and inductance are strewn with misunderstanding and errors that result from inaccurate terminology, mistakes in their definitions, and from the fact that they are quantities that characterize elements of ideal electrical circuits as well as real solid conductors. This is shown unfavourably not only in the respective field of the theory of electrical engineering, but also in the calculation of resistance and inductance. In this paper, a brief theoretical analysis of the state of the art is given, and its results are applied in the calculation of the current density, resistance, and inductance of two coaxial solid tubular conductors.


2003 ◽  
Vol 81 (8) ◽  
pp. 1015-1036 ◽  
Author(s):  
F E Irons

To reduce the general formula for lattice specific heat to Einstein's formula of 1907, one traditionally models the spectrum of lattice modes-of-vibration as a set of independent oscillators all of one frequency, ν1. Not only is this a poor representation of a real solid, but no formula is provided for the frequency ν1, which has to be determined empirically. We offer a new and more compelling method for reducing the general formula to Einstein's formula. The reduction involves a simple mathematical approximation, proceeds without any reference to independent oscillators all of one frequency, and leads to a formula for the characteristic frequency, ν1, equal to the mean modal frequency. The mathematical approximation is valid at all but low temperatures, thereby providing insight into the failure of Einstein's formula at low temperatures. A simple extension of the new method leads to the Nernst–Lindemann formula for specific heat, proposed in 1911 on the basis of trial and error and currently without a sound theoretical basis. Empirical values (from the literature) of the frequencies that characterize the Einstein, the Nernst–Lindemann, and also the Debye formulae are all in support of the present theory. PACS Nos.: 65.40.Ba, 01.55.+b


2008 ◽  
Vol 64 (1) ◽  
pp. 1-13
Author(s):  
Hideki YOSHIDA ◽  
Kazutoshi SAKATA ◽  
Masaaki KATAGIRI ◽  
Masaaki TERASHI ◽  
Shiro MURAKAWA

Entropy ◽  
2021 ◽  
Vol 24 (1) ◽  
pp. 70
Author(s):  
Yuriy Povstenko ◽  
Tamara Kyrylych ◽  
Bożena Woźna-Szcześniak ◽  
Renata Kawa ◽  
Andrzej Yatsko

In a real solid there are different types of defects. During sudden cooling, near cracks, there can appear high thermal stresses. In this paper, the time-fractional heat conduction equation is studied in an infinite space with an external circular crack with the interior radius R in the case of axial symmetry. The surfaces of a crack are exposed to the constant heat flux loading in a circular ring R<r<ρ. The stress intensity factor is calculated as a function of the order of time-derivative, time, and the size of a circular ring and is presented graphically.


1981 ◽  
Vol 59 (4) ◽  
pp. 530-534 ◽  
Author(s):  
Michael L. Klein ◽  
D. Levesque ◽  
J.-J. Weis

A molecular dynamics study has been carried out of the structure and dynamics of solid nitrogen in its high pressure, room temperature, plastic crystal phase: cubic Pm3n. We employed a system of 512 molecules interacting via atom–atom potentials. As in the real solid our simulated crystal is composed of two types of molecules whose dynamical behaviour is quite distinct. We present calculations of the power spectra associated with translational and rotational motions as well as the phonon response embodied in the dynamical structure factor S(Q, ω).


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