scholarly journals Disordered spherical bead packs are anisotropic

2010 ◽  
Vol 90 (3) ◽  
pp. 34001 ◽  
Author(s):  
G. E. Schröder-Turk ◽  
W. Mickel ◽  
M. Schröter ◽  
G. W. Delaney ◽  
M. Saadatfar ◽  
...  
Keyword(s):  
Author(s):  
Giulia Mancardi ◽  
Matteo Alberghini ◽  
Neus Aguilera-Porta ◽  
Monica Calatayud ◽  
Pietro Asinari ◽  
...  

Titanium dioxide nanoparticles have risen concerns about their possible toxicity and the European Food Safety Authority recently banned the use of TiO2 nano-additive in food products. Following the intent of relating nanomaterials atomic structure with their toxicity without having to conduct large scale experiments on living organisms, we investigate the aggregation of titanium dioxide nanoparticles using a multi-scale technique: starting from ab initio Density Functional Theory to get an accurate determination of the energetics and electronic structure, we switch to classical Molecular Dynamics simulations to calculate the Potential of Mean Force for the connection of two identical nanoparticles in water; the fitting of the latter by a set of mathematical equations is the key for the upscale. Lastly, we perform Brownian Dynamics simulations where each nanoparticle is a spherical bead. This coarsening strategy allows studying the aggregation of a few thousand nanoparticles. Applying this novel procedure, we find three new molecular descriptors, namely, the aggregation free energy and two numerical parameters used to correct the observed deviation from the aggregation kinetic described by the Smoluchowski theory. Molecular descriptors can be fed into QSAR models to predict the toxicity of a material knowing its physicochemical properties, without having to conduct large scale experiments on living organisms.


2009 ◽  
Vol 24 (1) ◽  
pp. 253-259 ◽  
Author(s):  
Jun-Ho Lee ◽  
Hyoukryeol Choi ◽  
Jae-Do Nam

Gold-coated polystyrene (PS) beads were fabricated by an in situ metallization route involving a cationic-gold complex with a controlled amount of sulfonic acid groups formed on the PS bead surface. The interaction ratio of SO3− to [Au(phen)Cl2]+ may be estimated to be 2.4, which means that 2.4 sulfonated groups will interact with one gold cationic ligand based on geometric considerations. A modeling methodology was developed to predict the mechanical deformation, conductivity, and contact surface area of a spherical bead under compression.


Author(s):  
Sassan Etemad

Turbulent convective heat transfer and radiation is simulated for a hot gas jet, impinging perpendicular on a flat surface at 2 jet diameters away from the jet nozzle. A small solid spherical bead, located in the jet centre half way from the wall, represents a thermocouple sensitive point. The bead becomes so hot that it radiates some heat to the colder surrounding surfaces. This phenomenon is responsible for a gap between the jet temperature and the bead temperature. The jet Reynolds number ranged from 7.67*103 to 4.52*104. Bead sizes 1.0 and 2.0 mm are used in jets at 500°C and 900°C. The simulations show that the mentioned temperature differences are significant and grow rapidly with high temperatures but decrease with Reynolds number. The temperature gap, which can be regarded as the thermocouple measurement error, increases also with the bead size. Simulations can be conducted for specific thermocouples with other shapes and materials to assist the measurement process. The modelling methodology is found to be promising for such demanding simulations that require a fine grid for resolving the field near the bead without using excessive cells in the rest of the domain. Hence, further work in this field is envisaged using the same methodology for solving convection, conduction and radiation in one single model and at a reasonable computational cost together with validating measurements. Hopefully this study contributes to a better understanding of the measurement of hot gas jet temperature and its improvement with the aid of simulations.


Author(s):  
Sassan Etemad

Computational fluid dynamics (CFD) simulations have been carried out for the turbulent convective heat transfer, conduction and radiation for metal thermocouple tips, accommodated in hot gas jets to study the measurement accuracy of the thermocouples. The study covers several thermocouple sizes, jet temperatures, and Reynolds numbers. The spherical bead, representing the tip, becomes so hot that it radiates some heat to the colder surrounding surfaces. This phenomenon is responsible for a gap between the jet temperature and the bead temperature. The mentioned temperature difference is significant. It grows both with bead size and gas temperatures but decreases with the Reynolds number.


2015 ◽  
Vol 137 (01) ◽  
pp. 40-41
Author(s):  
Adrian Bejan

This article discusses various aspects of snowflake architectures. It is certain that every snowflake conforms to only one architecture: a flat star with six fishbones connected at the center. The latent heat of solidification, which is released by the water vapor that becomes solid at the bead surface. There comes a critical time when the spherical bead is no longer an efficient architecture for dissipating heat. The principle calls for design change, toward faster heat release and solidification. The growth of ice morphs abruptly into a ball continued in one plane by needles. Because of the configuration of the water molecule, the needles grow in six directions. The flat star transfers heat to the surroundings more easily than a spherical bead with the same diameter. In order to give credit to the view that every snowflake is unique, the actual configuration depends on many secondary effects, which are of random origin.


Author(s):  
Choongbae Park ◽  
Steven T. Wereley ◽  
Osvaldo H. Campanella ◽  
David E. Nivens ◽  
Kenneth M. Little ◽  
...  

We developed a novel method to measure the rheological properties of single red blood cells (RBC) using the atomic force microscope (AFM). A spherical bead at the AFM cantilever tip compressed and relaxed the RBC. The force and displacement were converted into effective stress and strain. The impulse viscoelastic technique was used to compute the effective storage (E') and loss (E") moduli and phase lag (δ). Unfixed and fixed red blood cells were tested. Both cells were on glass coated with poly-l-lysine and then kept in phosphate buffered saline (PBS) until the experiment was finished. Measurements were done with height change and force up to 451nm and 64nN. The cells were found to be quite elastic, with phase lag on the order of 10-2 to 10-1 rad. Stepped changes in oscillation rate from 0.5Hz to 2.5Hz did not result in significant change in the measured results. To improve accuracy, we also design a bimaterial cantilever which consists of a gold layer on silicon with controlled thermal stresses such that the cantilever is curved. The curvature allows the root to fits the angle of the AFM head and the tip to be parallel to the substrate so that the RBC is squeezed between two parallel surfaces.


1967 ◽  
Vol 48 (9) ◽  
pp. 676-683 ◽  
Author(s):  
Marvin Kays ◽  
Robert O. Olsen

A comparative study is made of various rocket instrumentation and sensing techniques for collecting stratospheric wind and temperature data. The rocketsondes employed in synoptic studies in general use the spherical bead thermistor as the temperature sensing element. Different designs of sensors were launched in close proximity, and results agree within 3C. Different parachute configurations and chaff are compared for their ability to sense winds. In most cases, wind velocities agree within reason (5 m sec−1) among the different types of sensors. The major corrections that are applied to wind and temperature data are discussed. The corrections are small (less than 2° and 10 mps) below 50 km but increase with height and in some extreme cases can reach values of 200 m sec−1 for winds and 11C for temperatures at 60–65 km.


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