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J. B. Sokoloff

Publications and source records attributed to J. B. Sokoloff.

At least 19 recordsLinked to original sources

Ion Flow under an Applied Electric Field in Semiconducting and Metallic Carbon Nanotubes

Measurements made by Li, et. al., showed that the flow rates of potassium ions through 11nm long, subnanometer diameter, metallic and semiconducting carbon nanotubes under an applied electric field are almost the same. In contrast, measurements of the electrical conductivity of potassium chloride solution through 100 long metallic and semiconducting carbon nanotubes with diameters between 2.6-5.4nm by Cui, et. al., show that the ionic conductivity in the semiconducting nanotubes is larger than that of the metallic nanotubes. Possible theoretical origins of these differences are explored in this article.

cond-mat.mes-hall

Electronic screening of the friction acting on ions and water molecules in narrow carbon nanotubes

Li, et. al., have observed a larger flow rate, resulting from osmotic pressure, of protons and water molecules in nanometer scale diameter metallic carbon nanotubes compared to that in semiconducting carbon nanotubes. The flow rate of potassium ions, however, under an applied electric field is almost the same in metallic and semiconducting nanotubes. We propose a simple physical picture to understand these experimental results by examining the effects of screening by conduction electrons in electrically conducting carbon nanotubes on the friction experienced by protons, water molecules, and ions flowing through the nanotube.

cond-mat.mes-hall

Theory of the force of Friction Acting on Water Chains Flowing through Carbon Nanotubes

A simple model for the friction experienced by the one dimensional water chains that flow through subnanometer diameter carbon nanotubes is studied. The model is based on a lowest order perturbation theory treatment of the friction experienced by the water chains due to the excitation of phonon and electron excitations in both the nanotube and the water chain, as a result of the motion of the chain. On the basis of this model, we are able to demonstrate that the observed flow velocities of water chains through carbon nanotubes of the order of cm/s can be accounted for, if the nanotube is metallic. If it is insulating, however, our calculations imply that the flow velocity of the water could be much larger for the pressure gradient in experimental studies of water flow through subnanometer diameter nanotubes.

physics.flu-dyn

Hydrophilic Porous Materials as Helmet Padding Able to Prevent Traumatic Brain Injuries

The minimum possible value of the average deceleration of the head of a player engaged in an impact sport such as football or hockey, as a result of an impact of his/her helmet with a surface or another player, is inversely proportional to the helmet padding thickness. Since there are practical limits to its maximum thickness, it is difficult to significantly reduce the average acceleration. There is evidence, however, that the peak, rather than the average, acceleration is the most significant cause of brain injury. It is proposed here that brain injuries that occur as a result of an impact, could be reduced by using as padding a hydrophilic porous material swollen with fluid. The friction experienced by the fluid as it is squeezed out of the porous material in an impact can "tune" the acceleration of the skull so that it is never significantly higher than its average during the impact.

physics.med-ph

Droplet evaporation residue indicating SARS-COV-2 survivability on surfaces

SARS-CoV-2 survives and remains viable on surfaces for several days under different environments as reported in recent studies. However, it is unclear how the viruses survive for such a long time and why their survivability varies across different surfaces. To address these questions, we conduct systematic experiments investigating the evaporation of droplets produced by a nebulizer and human-exhaled gas on surfaces. We found that these droplets do not disappear with evaporation, but instead shrink to a size of a few micrometers (referred to as residues), persist for more than 24 hours, and are highly durable against changes of environmental conditions. The characteristics of these residues change significantly across surface types. Specifically, surfaces with high thermal conductivity like copper do not leave any resolvable residues, while stainless steel, plastic, and glass surfaces form residues from a varying fraction of all deposited droplets at 40% relative humidity. Lowering humidity level suppresses the formation of residues while increasing humidity level enhances it. Our results suggest that these microscale residues can potentially insulate the virus against environmental changes, allowing them to survive inhospitable environments and remain infectious for prolonged durations after deposition. Our findings can also be extended to other viruses transmitted through respiratory droplets (e.g., SARS-CoV, flu viruses, etc.), and can thus lead to practical guidelines for disinfecting surfaces and other prevention measures (e.g., humidity control) for limiting viral transmission.

physics.med-ph

Desalination due to Electrical Image Forces

It will be shown that for a solution of salt dissolved in water in contact with a metallic wall, the concentration of salt ions (both positive and negative) within a few Angstroms of the wall can be large enough to exceed the solubility limit of the salt, as a result of electrical image charge forces. In addition, since the dielectric constant of water increases from 2.1 at the wall to 81 at about a nanometer from a solid wall, there will be an attractive image potential near the plane on which this increase of the dielectric constant occurs. The possible existence of these image potentials suggests that the salt can be removed from the water by making salt water flow between an array of parallel solid plates..

cond-mat.soft

Theory of a Possible Mechanism for Lubrication and Surface Protection by an Electrically Neutral Hydrogels

It is demonstrated that polymers sticking out of the surface of a neutral hydrogel are capable of preventing adhesive forces from pulling a hydrogel into close contact with a surface against which it is pressed. The proposed mechanism for lubrication or surface protection suggests a possible mechanism for protecting the cornea from a contact lens, which is held against the eye by Laplace pressure. This mechanism, however, is only able to keep a gel coated surface from sticking to a surface against which it is pressed, if the gel and surface are bathed in fluid. Expected optical properties of the gel-surface interface are discussed, in order to suggest possible ways to study the gel-solid interface experimentally.

cond-mat.soft

Theory of the Observed Ultra-Low Friction between Sliding Polyelectrolyte Brushes

It is shown using a method based on a modified version of the mean field theory of Miklavic Marcelja that it should be possible for osmotic pressure due to the counterions associated with the two polyelectrolyte polymer brush coated surfaces to support a reasonable load (i.e., about $10^6 Pa$) with the brushes held sufficiently far apart to prevent entanglement of polymers belonging to the two brushes, thus avoiding what is believed to be the dominant mechanisms for static and dry friction.

cond-mat.mtrl-sci

Static and Dry Friction due to Multiscale Surface Roughness

It is shown on the basis of scaling arguments that a disordered interface between two elastic solids will quite generally exhibit static and "dry friction" (i.e., kinetic friction which does not vanish as the sliding velocity approaches zero), because of Tomlinson model instabilities that occur for small length scale asperities. This provides a possible explanation for why static and "dry" friction are virtually always observed, and superlubricity almost never occurs.

cond-mat.mtrl-sci

Friction between Polymer Brushes

By solving the equilibrium equations for a polymer in a neutral polymer brush, the degree of interpenetration of two polymer brushes in contact and near contact is calculated. These results are used to calculate values of the force of static friction in agreement with recent friction measurements for polymer brush lubricated surfaces. It is shown that at sufficiently light loads polymer brush coated surfaces can slide, with the load supported entirely by osmotic pressure, at a sufficiently large spatial separation so as to avoid entanglement, and hence static friction.

cond-mat.mtrl-sci

Theory of De-Pinning of Monolayer Films Adsorbed on a Quartz Crystal Microbalance

In quartz crystal microbalance (QCM) studies of the friction between an adsorbed monolayer film and a metallic substrate, the films are observed to slide relative to the substrate under inertial forces of order $10^{-14}dyn$ per film atom, a force much smaller than all theoretical estimates of the force that surface defects are capable of exerting. In this letter we propose, in order to resolve this issue, that if the defect potentials have a range of greater than an atomic spacing, the net force on a relatively stiff film due to the defects is likely to be extremely small. Line defects (e.g., step and facet edges and grain boundaries) as well as more localized defects (e.g., vacancies) are considered.

cond-mat.mtrl-sci

Lack of Pinning for Rigid Sliding Monolayers in Microbalance Experiments

Recent work on the dynamics of monolayers on a metallic substrate attached to a quartz oscillator has provided interesting data on kinetic friction at the microscopic level. Sliding of the film relative to the substrate is often observed even in situations in which theory seems to predict that the film should be pinned by substrate imperfections. In this letter we propose, in order to attempt to resolve this issue, that if the defect potentials have a range of a little more than an atomic spacing, the net forces on the film due to the defects are likely to be quite small due to cancellations.

cond-mat.mtrl-sci

A Mechanism for Lubrication between Surfaces with Atomic Level Roughness

It is proposed that lubricant molecules adsorbed on an interface between two asperities in contact, which is rough on the atomic scale, can switch the interface from the strong to weak pinning regime, resulting in a large reduction in the static friction. This is proposed as a possible mechanism for boundary lubrication. \

cond-mat.mtrl-sci

Dry Friction due to Adsorbed Molecules

Using an adiabatic approximation method, which searches for Tomlinson model-like instabilities for a simple but still realistic model for two crystalline surfaces in the extremely light contact limit, with mobile molecules present at the interface, sliding relative to each other, we are able to account for the virtually universal occurrence of "dry friction." The model makes important predictions for the dependence of friction on the strength of the interaction of each surface with the mobile molecules.

cond-mat.mtrl-sci

Kinetic Friction due to Ohm's Law Heating

Using both a recent calculation by Bruch of the damping of the motion of a monolayer nitrogen film oscillating harmonically on a metallic surface due to Ohm's law heating and a Thomas-Fermi approximation treatment of the Ohm's law heating mechanism, which accounts for the nonzero thickness of the surface region of a metal, it is argued that this mechanism for friction is able to account for recent measurements of the drop in the friction for anitrogen film sliding over a lead substrate as it goes below its superconducting transition temperature. Bruch's calculation is also made more transparent by re-doing the calculation for a film sliding at constant speed, instead of oscillating. Using this treatment, it is easily shown that Bruch's calculation is equivalent to integrating Boyer's solution of the problem of a charge sliding over a metallic surface over the charge density of the monolayer nitrogen film.

cond-mat.mtrl-sci

Explaining the Virtual Universal Occurrence of Static Friction

Perturbation theory, simulations and scaling arguments predict that there should be no static friction for two weakly interacting flat atomically smooth clean solid surfaces. The absence of static friction results from the fact that the atomic level interfacial potential energy is much weaker than the elastic potential energy, which prevents the atoms from sinking to their interfacial potential minima. Consequently, we have essentially two rigid solids, for which the forces at randomly distributed "pinning sites" cancel. It is shown here that even fluctuations in the concentration of atomic level defects at the interface do not account for static friction. It is also argued that the sliding of contacting asperities, which occurs when the problem is studied at the multi-micron length scale, relative to each other involves the shearing of planes of atoms. Since this results in a force for the interaction of two asperities which varies over sliding distances of the order of an atomic spacing, the contacting asperities at the surface are able to sink to their interfacial potential minima, with negligible cost in elastic potential energy. This results in static friction.

cond-mat.mtrl-sci