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At least 127 records · Page 7Linked to original sources
PubMed1996

The influence of loading time and lubricant on the friction of articular cartilage.

Friction of cartilage on metal, metal on cartilage and cartilage on cartilage contact configurations, within a mixed lubrication regime, was measured using synovial fluid, Ringer's solution or with no lubricant present. The main test variable was the period of stationary loading which ranged from 5 s to 45 min, prior to sliding and consequently measuring friction. The coefficient of friction rose gradually with increasing stationary loading time, up to a value of approximately 0.3 at 45 min for all the contact configurations. Following the re-application of load, after short periods of load removal, friction was also found to drop sharply. The flow of liquid in the biphasic cartilage and load carriage by the fluid phase was highlighted as being an important factor in reducing friction within the mixed or boundary lubrication regime. Movement of the contact zone over the cartilage counterface ensured very low friction as the slider moved over fully hydrated cartilage. For the cartilage--cartilage contacts synovial fluid significantly reduced friction compared to Ringer's solution. This was attributed to an effective boundary lubrication action, which was not as effective for the cartilage--metal contacts.

Animals↗
PubMed2004

Frictional resistances of different bracket-wire combinations.

BACKGROUND: It has been suggested that the frictional resistance of ceramic brackets can be reduced by either lining the slots with stainless steel or by contouring the base of the slot. OBJECTIVES: The objectives of this investigation were to compare in vitro the static and kinetic frictional resistances of ceramic brackets with metal lined slots ("Clarity", CL), stainless steel brackets ("Miniature Twin", MT), and two ceramic brackets with different slot designs ("Contour", CO; "Transcend", TR). METHOD: Two sizes (0.018 x 0.025 inch; 0.021 x 0.025 inch) of stainless steel (SS), nickel titanium (NiTi) and beta titanium (beta-Ti) wires were drawn through the brackets. All brackets had 0.022 inch slots, and the brackets and wires were used once. The brackets were of different widths: CL, 0.180 inch; CO, 0.114 inch; MT, 0.118 inch; TR, 0.138 inch. An Instron Universal Testing Machine was used in this study. RESULTS: There were no significant static or kinetic frictional differences when the smaller 0.018 x 0.025 inch wires were drawn through the brackets. There were no statistically significant static or kinetic frictional differences between the CL-CO, CL-MT and CO-MT bracket pairs when the 0.021 x 0.025 inch wires (SS, NiTi, beta-Ti) were used. There were no significant kinetic frictional resistance differences between the CL-TR and MT-TR when the SS wires were used. In general the static and kinetic resistances of the 0.021 x 0.025 inch wires of NiTi wire < SS wire < beta-Ti wire. Regardless of wire type some of the lowest kinetic resistances were found with the narrow CO brackets with the rounded slot bases. The highest static and kinetic frictional resistances were found with the wide TR bracket, and with stainless steel and beta-Ti wires. CONCLUSION: The high static and kinetic frictional resistances of ceramic brackets can be reduced either by lining the slots with stainless steel or by reducing the bracket width and rounding the slot base.

Ceramics↗
PubMed2002

Static coefficient of friction between Ti-6Al-4V and PMMA for cemented hip and knee implants.

The static coefficient of friction between Ti-6Al-4V and PMMA was determined experimentally. A microtopographic surface analysis of the Ti-6Al-4V and PMMA specimens used in the experiments was performed to characterize the surfaces. The coefficient of friction between Ti-6Al-4V and PMMA in both dry and wet conditions, using both Ringer's solution and bovine serum, was determined by the standard inclined plane test, following the ASTM 4516-91 method, and by a prototype computerized sliding friction tester. The effects of surface roughness and of contact pressure on the coefficient of friction also have been investigated. Tests were performed at 26 degrees C and at body temperature of 37 degrees C. Considering all the tests, the overall range of the mean coefficients of friction varied between 0.17 and 0.32 in dry or wet conditions. For the same surface roughness in contact, in general the coefficient of friction using Ringer's solution was slightly lower than it was in dry conditions whereas bovine serum had a very high surface tension, which significantly increased the static coefficient of friction.

Alloys↗
PubMed1990

[The effect of the ligature on the friction between bracket and arch].

The combinations of five different wire materials and six ligatures were analysed with the help of a testing apparatus in order to determine the loss in orthodontic force caused by friction between arch wire and ligature. The bracket was fixed at an angulation of zero degrees with respect to the arch wire. The results of our measurements can be summarized as follows: 1. Friction is determined mostly by the sort of ligature and by the way of ligation and not by the dimensions of the different arch wires. 2. Friction caused by alastics is significantly less than friction caused by steel-ligatures. This can be observed especially if standard-steel wires are used. 3. Frictional forces are astonishingly low if multistrand wires are used. Even the 0.016 x 0.022 Force 9 wire shows little friction. 4. Orthodontic force may even be neutralized if a steel ligature is combined with standard steel wires (0.016 and 0.016 x 0.022). 5. This leads to the proposal that a steel ligature should be retwisted for about 90 to 180 degrees next to the bracket, if orthodontic tooth translation is to be achieved. 6. Using the Unitek Quicksticks causes least friction beneath the alastics.

Biomechanical Phenomena↗
PubMed1980

A comparative study of frictional resistances between orthodontic bracket and arch wire.

Practitioners are aware of the presence of friction in those orthodontic appliances where relative motion between bracket system and arch wire occurs in ordinary deactivation processes. Numerous comments on friction have appeared in the published dental/orthodontic literature, but little controlled research into the problem has been reported. The objective of this investigation was to evaluate and compare frictional forces generated in an experimental stimulation of the canine-retraction procedure on a continuous arch wire. Six independent variables were chosen for study: arch wire size and shape, bracket width and style, second-order angulation between bracket and passive arch wire, arch wire material, ligature force and type of ligation, and interbracket distances. Frictional resistance was found to be nonlinearly dependent upon bracket/arch wire angulation. With small and generally nonbinding angulations, bracket width and ligature force were the dominant influences on level of friction. As angulations were increased, producing binding between wire and bracket, this variable itself became the controlling parameter. Wire shape and arch wire stiffness in bending, a function of three of the variables studied, apparently exerted substantial influence on frictional-force magnitude at relatively high angulations. The reduced data, together with structural computations, were employed to deduce a minimum frictional-resistance combination of edgewise appliance components.

Biomechanical Phenomena↗
PubMed1993

Friction between hand and handle. Effects of oil and lard on textured and non-textured surfaces; perception of discomfort.

This paper discusses coefficient of dynamic friction mu(k), and perceived discomfort for differently textured surfaces when touched by a normal hand, a 'sweaty' hand and a hand contaminated with glycerol, paraffin oil or lard. Fourteen male subjects applied forces of 1, 10 or 20 N using the index finger of the dominant hand while striking across a specimen of the same polycarbonate material with 100, 75, 50 or 25% skin-contact area (by ridges). Surface pressures in the range 6-288 kPa were recorded. Generally there was a very low correlation between mu(k) and perceived discomfort. Wider grooves and increased normal forces were associated with discomfort but did not necessarily provide more friction. Unlike most materials, palmar skin showed sticky characteristics and mu(k) frequently exceeded 1.0 when the surface loads were low. The coefficient of friction on palmar skin decreased with increasing surface loads. A considerable reduction of mu(k) was noticed when the normal force increased. A 20-fold increase in normal force from 1 to 20 N (an increase in surface load from 6.3 to 81.4 kPa) resulted in only an eight-fold increase in frictional force while mu(k) dropped from 2.22 to 0.85. A decrease was noticed for all tested surfaces and during all tested environmental conditions; however, increased normal force increased the perceived discomfort. A 25-50% increase in coefficient of friction could be gained under contaminated conditions using two out of four fairly similar textures. Grooves in surfaces reduced mu(k) under normal and sweaty conditions, but improved mu(k) when contaminants were present. Patterns with a large skin-contact area showed either a high or a low coefficient of friction depending on the environmental conditions. A plain, glossy, non-textured surface of polycarbonate under normal skin conditions yielded [Formula: see text] when the surface pressure was low (6 kPa). When the skin was exposed to paraffin oil, mu(k) dropped drastically to 0.28. Oil and lard reduced mu(k), but sweat increased it in relation to a normal hand. Wider grooves in the texture provide friction during contaminated conditions at the price of discomfort.

Journal Article↗
PubMed1996

Use of robotics technology to measure friction in animal joints.

A new system to measure friction in animal joints has been designed. The system utilizes a robotic arm. Force control of the robotic arm was used to survey the geometry of a sliding surface before the friction of the joint is measured. This enables the precise measurement of friction in joints of complex shape. To test the reliability of the new system we took friction measurements from 10 rabbit stifles. The experimental conditions were: (i) intact joints, (ii) joints after the surfaces were washed. The mean values of the frictional coefficients were 0.008 in the intact joints and 0.015 in the washed joints. These mean values were similar to some previous results obtained from canine hip joints under the same experimental conditions. Furthermore, the standard deviations in this study were smaller than in the previous study. These facts suggest that the new system is reliable. RELEVANCE:--The pathology of osteoarthritis is related to the lubrication mechanisms of joints. In any study of the lubrication mechanisms, an accurate friction measurement is important. In this study we used robotics technology to measure friction in joints.

Journal Article↗
PubMed1998

The effect of resurfacing on friction, speeds and safety on main roads in Finland.

This study aimed at examining how resurfacing and the first winter period after resurfacing affect the safety of main roads in Finland. The study consisted of three substudies. In the first substudy the changes of side friction and lock braking friction were measured on newly paved roads after resurfacing and after the first winter period. The effect of different resurfacing methods was also compared in the course of the study. All the 50 road sections in the study were resurfaced in summer 1991 and measured with the friction truck of the Technical Research Centre of Finland (VTT). Friction was found to be highly dependent on the type of resurfacing treatment. In general, the friction of surfaces with high coefficients after resurfacing decrease and the lowest frictions increase with time, locked braking friction values immediately after resurfacing can be undesirably low. The second substudy dealt with the effect of resurfacing on the vehicle speeds. The analysis was based on automatic speed and weather measurement in 1991 and 1992 on resurfaced roads, which were resurfaced in the summer 1991 and on a sample of comparison roads which had not been resurfaced. There is little change in speeds on the non-resurfaced roads during the study period, but there is some indication that resurfacing increases the average speeds, at least when the road is dry. Complete data were available for only one site, where the result was that average speeds on dry roads increased after resurfacing by 0.6 km/h and increased still more (by 0.5 km/h) after the first winter period. The third substudy analysed fatal and injury accidents reported to the police on the resurfaced and comparison roads one and two years before, the same year resurfacing was performed and one and two years after the resurfacing. The accident results were similar to the speed findings. The most likely effect is a risk increase immediately after resurfacing by somewhat less than 7% and of 3 to 7% of the first winter period. These results are, however, subject to large uncertainty because of the small number of accidents on the treatment roads.

Accidents, Traffic↗
PubMed2002

The effect of friction reduction in presence of ultrasonic vibrations and its relevance to travelling wave ultrasonic motors.

In many ultrasonic applications frictional effects play an important role (e.g. ultrasonic machining, ultrasonic motors). For optimising the applications in terms of quality, efficiency and lifetime it is important to understand the frictional coupling of the vibrating and the non-vibrating part. This contribution is devoted to give an explanation for the reduction of friction forces which is often observed when ultrasonic vibrations are superimposed to macroscopic motions. Usually adopted coefficients of friction are used for modelling such conditions suggesting special frictional mechanisms for high frequency oscillations, whereas the present paper shows that Coulomb's friction law provides a very good description of the observed phenomena if the kinematics of the system is taken into account. Two systems are investigated. In the first system the ultrasonic and macroscopic movements are parallel and in the second they are perpendicular to each other but also within the plane of contact. Both systems were investigated analytically and experimentally using a specially designed test rig. The measurements confirmed the analytically derived equations and therefore the validity of Coulomb's friction law even for ultrasonic conditions.

Journal Article↗
PubMed2002

Effect of friction on anodic polarization properties of metallic biomaterials.

The effect of friction on the anodic polarization properties of metallic biomaterials in a physiological saline solution was investigated. The current density during friction becomes higher than during the static condition. The fluctuation range of the current density caused by the destruction and formation of passive film was observed. For SUS316L stainless steel and Co-Cr-Mo casting alloy, the fluctuation range was observed in the passivity zone. Otherwise, for Ti alloys, the fluctuation range was observed in both the activity and passivity zones. The decrease of the corrosion potential for Ti alloys due to friction was much larger than that of SUS316L stainless steel and Co-Cr-Mo casting alloy. From this result, it was considered that in a the frictional environment, the stressing zone turned anodic and its periphery cathodic, and corrosion tended to progress more than in the static environment. The effect of wear on the anodic polarization curves also changed depending on the frictional load, potential zone and the pH of the solution. A rapid increase in current density due to corrosion starting from the frictional area was found in the Ti-6Al-4V and Ti-15Mo-5Zr-3Al alloys containing Al. However, for the new Ti-15Zr-4Nb-4Ta alloy, this rapid increase was not seen in the high-potential region. The effect of the lateral reciprocal speed was also negligible for the new Ti alloy. It was found that the new Ti-15Zr-4Nb-4Ta alloy exhibited excellent corrosion resistance under friction.

Alloys↗
PubMed2006

Friction and adhesion between C60 single crystal surfaces and AFM tips: effects of the orientational phase transition.

We have investigated the nanotribological properties of C60 single crystal (111) and (100) surfaces around its orientational order-disorder phase transition temperature, approximately 260 K, by atomic force microscopy and frictional force microscopy (AFM/FFM) in high vacuum. Results show that for both surfaces across the phase transition temperature, the friction force and the adhesive force between a C60 coated AFM tip and the C60 crystal surfaces exhibit discontinuous behavior. The friction force within the applied external load range in the low temperature phase is significantly larger than that in the high temperature phase, with no obvious change in the slope of the friction force curves (the friction coefficient) in the low and high temperature phases. The abrupt change in friction was found to be caused mainly by the abrupt change in adhesion, which, in turn, can be qualitatively understood through changes in the van der Waals interaction and the short-range Coulomb interaction associated with the structural changes across the phase transition. Compared to most other degrees of freedom, the rotation of C60 molecules was found to have little effect on friction and is an ineffective energy dissipation channel.

Journal Article↗
PubMed2004

Role of friction in pattern formation in oscillated granular layers.

Particles in granular flows are often modeled as frictionless (smooth) inelastic spheres; however, there exist no frictionless grains, just as there are no elastic grains. Our molecular dynamics simulations reveal that friction is essential for realistic modeling of vertically oscillated granular layers: simulations of frictionless particles yield patterns with an onset at a container acceleration about 30% smaller than that observed in experiments and simulations with friction. More importantly, even though square and hexagonal patterns form for a wide range of the oscillation parameters in experiments and in our simulations of frictional inelastic particles, only stripe patterns form in the simulations without friction, even if the inelasticity is increased to obtain as much dissipation as in frictional particles. We also consider the effect of particle friction on the shock wave that forms each time the granular layer strikes the container. While a shock wave still forms for frictionless particles, the spatial and temporal dependence of the hydrodynamic fields differ for the cases with and without friction.

Journal Article↗
PubMed2004

Effects of surface friction on a two-dimensional granular system: cooling bound system.

Experiments performed by Phys. Rev. E 62, 2380 (2000)] on two-particle collisions and dynamics emphasized the importance of the role played by substrate friction, in particular kinetic friction, on the particle dynamics after collisions on a substrate. We present a numerical model which accounts for collisional and surface frictional dissipation and their influence on particle dynamics for a quasi-two-dimensional cooling initially dilute granular material. This model makes the simplifying assumption that the collision dynamics is determined solely by the incoming velocity and angular velocities of the colliding particles. We apply this model to a numerical simulation of a monolayer of monodisperse particles moving on a substrate, enclosed between inelastic walls. We find that surface friction-in particular, kinetic friction-plays a dominant role in determining the dynamics of quasi-two-dimensional multiparticle systems where the particles are in continuous contact with a substrate. Results from simulations performed for different system sizes indicate that surface friction and the inelastic walls lead to clustering of the particles in and near the vicinity of the walls. We find that the rate of decrease of average total kinetic energy is the highest when the majority of the particles have just collided and are experiencing kinetic frictional forces and torques. We also find from our calculations that, on average, particle-wall collisions lead to more dissipation than particle-particle collisions for a single particle for fixed restitutional parameters.

Journal Article↗
PubMed2005

Friction drag of a spherical particle in a liquid crystal above the isotropic-nematic transition.

We study the friction drag of a spherical particle in the isotropic phase of a nematic liquid crystal close to the isotropic-nematic transition point. To describe the orientational order in the liquid crystal, the second-rank tensor order parameter Qalphabeta is employed. We solve the hydrodynamic equations for Qalphabeta and the fluid velocity nu in order to determine the friction drag. In our discussion of the friction drag, we concentrate on four parameters: the temperature, the surface order parameter, the particle radius, and the Ericksen number Er (characterizing the ratio of the viscous force to the elastic force). The temperature dependence of the friction drag agrees well with experiments that show an increasing friction drag when the isotropic-nematic phase transition is approached from above. Furthermore the friction drag increases with the surface order parameter due to the more pronounced surface nematic layer, and for larger particles it is less affected by this layer. Finally, we observe that in the range of Er we study, the friction drag is almost independent of Er although flow-induced order occurs for sufficiently large Er and surface order parameter.

Journal Article↗
PubMed1993

The influence of bracket material, ligation force and wear on frictional resistance of orthodontic brackets.

Planar static frictional phenomena were investigated for two types of ceramic and one type of stainless steel orthodontic bracket against rectangular stainless steel archwire. The brackets studied were 'Starfire' (single crystal aluminium oxide), 'Allure III' (polycrystalline aluminium oxide), and 'Dentaurum' (stainless steel). The investigative parameters were: bracket material, force of ligation and whether the brackets were new or 'worn'. Without exception, both types of ceramic bracket produced greater frictional resistance than the stainless steel brackets throughout testing. At a ligation force of 500 g, the Starfire bracket gave the greatest frictional resistance. At ligation forces of 200 and 50 g, the greatest frictional resistance was seen with Allure III. After a period of simulated wear, frictional resistance of Starfire tended to increase at the greatest ligation load while that of both ceramics decreased slightly at the two lower ligation loads. The ceramic brackets caused abrasive wear of the archwire surfaces and the consequent wear debris may have contributed to the changes in frictional resistance seen with Starfire and Allure III. Dentaurum brackets produced minimal frictional resistance in any test and negligible change with wear.

Aluminum Oxide↗
PubMed1975

"Stiction-friction" of total hip prostheses and its relationship to loosening.

The static friction, or "stiction-friction", in McKee-Farrar and Charnley-Müller prostheses in a hip joint simulator was compared with dynamic friction determined while the prostheses were oscillated. Under physiological conditions stiction-friction differed little from dynamic friction in both metal-on-metal and metal-on-plastic prostheses, and was affected very little by the lubricant as long as some fluid was present. Stiction-friction increased significantly only after relatively long stationary periods and high loads. However, the frictional forces generated in total hip-replacement prostheses were at least forty times higher than those generated in normal joints and may well be enough to cause late loosening of acetabular components by fatigue failure.

Acetabulum↗
PubMed1985

Effect of suture material and construction on frictional properties of sutures.

The results overwhelmingly support the view that the coefficient of friction is not a material constant of the sutures but a function of several variables, including applied tension, suture construction and suture material. The coefficient of friction decreased with an increase in applied tension with the rate of change depending upon the suture material. Prolene and Ethilon had the highest frictional values among all sutures at low tension, but dropped to a position of lowest values at high tension. On an average, braided sutures gave higher frictional values than did the monofilament sutures. Sutures with special surface coatings (silicone or Teflon) generally gave lower values than did the sutures without any such coatings. Similar results were reported in other studies on coated materials. The differences in frictional profiles are governed by the differences in the viscoelastic nature of the suture materials. The unusual traces produced by Prolene were considered as being due to its high degree of stretch and elasticity. Others similarly found that Prolene behaved peculiarly due to a high degree of stretch. Finally, coefficient of friction is an important property of suture materials as it is expected to have a direct bearing on the security of knots. A careful study of this parameter under a variety of clinical conditions is essential to gain an understanding of the behavior of surgical knots in clinical practice. The present study gives detailed information on the frictional behavior of various types of surgical suture materials.

Sutures↗
PubMed1995

Method for the measurement of friction between tendon and pulley.

An experimental system was developed that allows direct measurement of friction at the tendon-pulley interface, and the results were interpreted by use of a theoretical model for friction of a cable around a fixed pulley. Validation experiments were conducted with a nylon cable around a nylon rod. One end of the cable was connected to an actuator via a load cell, and the other end was connected to a 4.9 N load via a similar load cell. The cable was passed around the nylon rod and then pulled toward the actuator. Tests were performed at five different arcs of contact. The friction forces, as measured by the difference between two load transducers, were compared with those determined for a theoretical model and were used for calculation of the friction coefficient. The measurement system then was used to study the friction force between the flexor digitorum profundus tendon and the A2 pulley on nine fresh frozen index digits. The method allows us to measure the direct interaction between the tendon and pulley and could be used to evaluate and compare procedures for tendon-pulley and pulley repair and reconstruction, as well as for the study of tendon-pulley friction in various pathological conditions.

Fingers↗