scholarly journals Use of Nanomaterials in Cryobiology and Cryomedicine

2020 ◽  
Vol 30 (4) ◽  
pp. 313-330
Author(s):  
Anatoliy Goltsev ◽  
◽  
Mykola Bondarovych ◽  
Natalya Babenko ◽  
Yuliya Gaevska ◽  
...  

The review considers the possibility of using modern nanotechnological developments aimed to achieve alternative cryobiological goals. On the one hand, the use of nanomaterials will increase the functional value of thawed cells due to such unique characteristics of nanoparticles as size, shape, surface charge, chemical composition, etc. Nanomaterials can be used as nanocontainers for impermeable cryoprotective agents (CPAs) and cause significant changes in crystal formation, thermal conductivity and other properties of cells, tissues and organs, that increases the efficiency of their cryopreservation. On the other hand, the combined use of nanomaterials and low-temperature freezing factors is considered a promising method of destruction of pathologically altered cells and tissues, as it minimizes the risk of recurrence of oncopathology after insufficient freezing-out of the tumor site.

1878 ◽  
Vol 28 (2) ◽  
pp. 571-582 ◽  
Author(s):  
Crum Brown ◽  
E. A. Letts

The analogies existing between elements belonging to one “family,” such, for instance, as the nitrogen family or the sulphur family, have long been recognised, and are pointed out and insisted upon even in elementary textbooks; but the very important analogies existing between substances of different quantivalence are apt to be forgotten or overlooked. For illustrations of such analogies we may point to boron and silicon, elements closely resembling one another in themselves and also in their compounds,—differing, indeed, in little else but that the one is triad and the other tetrad. A similar relation exists between gold and platinum.The elementary substances, sulphur and phosphorus, have many points of similarity: both fuse at a comparatively low temperature, both are transformed by heat into amorphous insoluble modifications, and both have anomalous vapour densities.


2017 ◽  
Vol 31 (27) ◽  
pp. 1750344 ◽  
Author(s):  
Chunsheng Ma ◽  
Rui Qi ◽  
Feng Yuan ◽  
Shaou Chen ◽  
Huaisong Zhao

By considering the pseudogap effect, the doping and energy dependences of thermal conductivity in cuprate superconductors are studied. Our results show that the thermal conductivity as a function of energy exhibits a characteristic peak from underdoping to overdoping due to the presence of the pseudogap in pseudogap phase of cuprate superconductors. The thermal conductivity is strongly doping dependent. On the one hand, with increasing doping concentration, the weight of thermal conductivity increases quickly, especially the residual thermal conductivity which is in qualitative agreement with the experimental data. On the other hand, the characteristic energy corresponding to the position of the characteristic peak decreases monotonically upon increasing doping concentration, and it scales with the doping dependence of pseudogap. In particular, we have studied the doping dependence of the ratio of quasiparticle velocities normal and tangential to the Fermi surface at the nodes [Formula: see text]. It is shown that [Formula: see text] increases with the increase of doping concentration. Moreover, we explain that both the residual thermal conductivity and [Formula: see text] increase rapidly upon the increase in doping concentration in heavily overdoped cuprate superconductors.


2002 ◽  
Vol 20 (9) ◽  
pp. 897-905 ◽  
Author(s):  
Ireneusz Kocemba ◽  
Sławomir Szafran ◽  
Jacek Rynkowski ◽  
Tadeusz Paryjczak

Semiconductor gas sensors based on metal oxides have been widely accepted as an important tool for the detection of different gases in air. An understanding of all the mechanisms related to such detection is essential in order to improve the sensitivity and selectivity of these gas detectors. This paper considers the mechanism of detection by semiconductor oxide gas sensors in terms of catalytic reactions described by Rideal–Eley and Langmuir–Hinshelwood mechanisms. Some relationships were discussed between the catalytic and detection properties of SnO2 and Pt/SnO2 systems used on the one hand as catalysts of low-temperature CO oxidation and on the other hand as sensors of CO in air.


2006 ◽  
Vol 45 ◽  
pp. 107-112 ◽  
Author(s):  
W. Pabst ◽  
Eva Gregorová

The cross-property relations between the elastic moduli and the thermal conductivity of porous ceramics are reviewed from the viewpoint of micromechanics (composite theory). Consequences of the rigorous Milton-Torquato and Gibiansky-Torquato relations (in the form of bounds, i.e. inequalities derived between bulk or shear moduli on the one hand and thermal conductivity on the other) are compared to various approximate relations (equalities) recently proposed between the tensile modulus (Young’s modulus) and thermal conductivity, among them the two new cross-property relations proposed by the authors. The relations are critically discussed and applied to the case of porous alumina, zirconia and alumina-zirconia composite ceramics.


Author(s):  
М.А. Kholkina ◽  
◽  
R.I. Muravev ◽  
А.М. Zhulnikov ◽  

There is a common idea in publications about pottery traditions and cultural and historical processes in Eastern Fennoscandian Neolithic that the tradition of asbestos-tempered pottery was spread so widely and for such a long time due to the technological advantages of this temper. On the one hand, this idea contradicts the notions on conservativeness and traditionality in ancient pottery making. On the other hand, we can confidently state that asbestos as a temper had a certain non-functional value. At the same time, we cannot deny the functional advantages of asbestos without carrying out relevant experiments. One can prove or deny the mentioned hypothesis by comparing the characteristics of asbestos as a temper with other materials, first of all, crushed stone and bird down. According to the preliminary program of the experiments to answer all the main questions about asbestos as tempering material one should make at least 60 experimental vessels and the same amount of small experimental models, produce low, medium, and high temperature firing and run all the necessary tests. The experiment turns out to be quite lengthy and labor intensive, but quite manageable in case of proper preparation.


Author(s):  
Thomas Hellman Morton

In an ode addressed to his friend Fabullus, the Roman poet Catullus speaks of a fragrance so pleasing that “when you smell it you will beg the gods to make you all nose.” Would that the recipe for such a scent had been transmitted through the ages! Even today, however, it is not possible to document chemical composition with adequate fidelity to reconstruct an odor perfectly. Catullus writes that the gods of love gave the perfume to his girlfriend. Suppose such gods existed and could list the ingredients of its aroma. The list would contain hundreds—perhaps thousands—of chemical structures and their relative proportions. Very likely, many of the structures would stand for compounds that are currently unknown, but they could be synthesized in the laboratory. Would that knowledge permit me to reproduce the odor? This chapter argues that the answer remains uncertain. The current state of chemical knowledge can neither account for why an odor smells the way it does nor what determines its intensity. The recipe for replicating a sensory experience—what is essential and what is superfluous—remains obscure. The sense of smell challenges chemical understanding. On the one hand, given the structure of a new molecule a chemist can predict its spectroscopic properties over a wide domain of electromagnetic frequencies. A mixture ordinarily displays a spectrum that superimposes the spectra of its individual components, unless they physically interact with each other. In the chemical senses, on the other hand, perceptions of mixtures often cannot be inferred from their constituents, even though the components do not interact at the molecular level. Moreover, no one can reliably predict the organoleptic properties (taste or smell) of a new molecule from its structure. Even if that were possible, the English language does not offer a vocabulary with which to describe new smells, except by analogy to odors that are already familiar. The poverty of descriptors means that, in talking about olfactory stimuli, many people allude to direct experiences. These allusions call on memories of characteristic odors of familiar objects, which represent “unitary percepts.”


Author(s):  
Walter Wahl

The investigation of the crystalline properties of the simpler organic bodies, gaseous or liquid at Ordinary temperature, has been described in Parts I and II.* In this paper the experimental results will be discussed with regard to their bearing upon the problem of the relationship between molecular constitution and crystal symmetry. In order to facilitate a comparison the experimental results are summarised in the table on p. 2. As seen from the table, more than 50 per cent, of the substances investigated are polymorphic, and to this class nearly all the substances which contain only one carbon atom belong. The question therefore arises which one of the crystalline modifications of a substance is to be compared with the one or the other form of another substance, or with the crystals of a substance of which only one modification is known. In most of the cases investigated very little is known with regard to the modification stable at low temperature, and thus for practical reasons only the form crystallising directly out of the liquid state can be taken into account.


1966 ◽  
Vol 44 (10) ◽  
pp. 2293-2302 ◽  
Author(s):  
H. L. Malm ◽  
S. B. Woods

Low-temperature measurements of electrical resistivity, thermal conductivity, and thermoelectric power on silver alloys containing 0.005, 0.067, 0.11, and 0.31 at.% of manganese are reported. The same specimens were used for the measurement of all properties over the temperature range from 2 to 25 °K. The well-known minimum and maximum are observed in the electrical resistivity of the three more concentrated alloys and the minimum is visible in the most dilute alloy near the lowest temperatures of measurement. Associated effects are observed in the other properties and their possible relationship to theoretical electron scattering mechanisms, particularly that of Kondo, is discussed.


The unusual characteristics of heat transfer in liquid He II have been reported in several recent papers. The very high thermal conductivity of the low-temperature modification of liquid helium was first noted by Keesom and Keesom (1935). It was then found by Allen, Peierls and Uddin (1937) and subsequently verified by Keesom, Keesom and Saris (1938) that the rate of transfer of heat varied with the temperature gradient. The discovery of the momentum transfer accompanying heat flow in He II which was made by Allen and Jones (1938) and the work on mobile surface films of the liquid done by Daunt and Mendelssohn (1938) show that a large part of the heat must be carried by some form of mass transfer. Several ideas and theories to explain the phenomena have been put forward by Kapitza (1938), Jones (1938), Michels, Bijl and de Boer (1938), Tisza (1938) and Keesom and Taconis (1938). The experimental evidence is as yet too meagre to prove or disprove any of the theories. It was with the intention of adding to the data already known concerning the properties of liquid He II that the present research was undertaken. The apparatus which was used is shown in fig. 1. The thermal conductivity was measured by a standard method. A constant supply of heat was supplied to one end of a long capillary containing liquid He II, and the other end was maintained at the constant temperature of the He II bath. Temperatures were observed at two points along the capillary.


Parasitology ◽  
1938 ◽  
Vol 30 (4) ◽  
pp. 543-551 ◽  
Author(s):  
N. W. Pirie ◽  
K. M. Smith ◽  
E. T. C. Spooner ◽  
W. D. McClement

Two nucleoproteins with similar chemical composition have been isolated from the leaves of tobacco plants infected with tobacco necrosis virus. One of these is crystalline and has a sedimentation constant of 130 × 10−13; the other is amorphous and its principal component has a sedimentation constant of 58 × lO−13.Each preparation will infect plants at a dilution of 1 in 108 and will precipitate specifically with antiserum at a dilution of 1 in 3·2 × 105.The nature of the difference between preparations in the two states is obscure and it has not proved possible to convert the one into the other.


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