851 research outputs found
Mechanics of a gaseous film barrier to lubricant wetting of elastohydrodynamically lubricated conjunctions
Two analytical models, one based on simple hydrodynamic lubrication and the other on soft elastohydrodynamic lubrication, are presented and compared to delineate the dominant physical parameters that govern the mechanics of a gaseous film between a small droplet of lubricant and the outer race of a ball bearing. Both models are based on the balance of gravity forces, air drag forces, and air film lubrication forces and incorporate a drag coefficient C sub D and a lubrication coefficient C sub L to be determined from experiment. The soft elastohydrodynamic lubrication (EHL) model considers the effects of droplet deformation and solid-surface geometry; the simpler hydrodynamic lubrication (HL) model assumes that the droplet remains essentially spherical. The droplet's angular position depended primarily on the ratio of gas inertia to droplet gravity forces and on the gas Reynolds number and weakly on the ratio of droplet gravity forces to surface tension forces (Bond number) and geometric ratios for the soft EHL. An experimental configuration in which an oil droplet is supported by an air film on the rotating outer race of a ball bearing within a pressure-controlled chamber produced measurements of droplet angular position as a function of outer-race velocity droplet size and type, and chamber pressure
Navier-Stokes cascade analysis with a stiff Kappa-Epsilon turbulence solver
The two dimensional, compressible, thin layer Navier-Stokes equations with the Baldwin-Lomax turbulence model and the kinetic energy-energy dissipation (k-epsilon) model are solved numerically to simulate the flow through a cascade. The governing equations are solved for the entire flow domain, without the boundary layer assumptions. The stiffness of the k-epsilon equations is discussed. A semi-implicit, Runge-Kutta, time-marching scheme is developed to solve the k-epsilon equations. The impact of the k-epsilon solver on the explicit Runge-Kutta Navier-Stokes solver is discussed. Numerical solutions are presented for two dimensional turbulent flow over a flat plate and a double circular arc cascade and compared with experimental data
On the numerical solution of the dynamically loaded hydrodynamic lubrication of the point contact problem
The transient analysis of hydrodynamic lubrication of a point-contact is presented. A body-fitted coordinate system is introduced to transform the physical domain to a rectangular computational domain, enabling the use of the Newton-Raphson method for determining pressures and locating the cavitation boundary, where the Reynolds boundary condition is specified. In order to obtain the transient solution, an explicit Euler method is used to effect a time march. The transient dynamic load is a sinusoidal function of time with frequency, fractional loading, and mean load as parameters. Results include the variation of the minimum film thickness and phase-lag with time as functions of excitation frequency. The results are compared with the analytic solution to the transient step bearing problem with the same dynamic loading function. The similarities of the results suggest an approximate model of the point contact minimum film thickness solution
A Sexier Literacy: Information Literacy through Media Literacy
The similarities in scope and objectives between information literacy and media literacy education are remarkable. On the surface, each is concerned with issues of access, analysis, evaluation, and use or production. But even beyond these basic tenets, guiding learners toward critical thought, creative agency, ethical use and production of information, and civic empowerment are shared concerns. In fact, as we begin to work with the generation of students dubbed Generation M by the Kaiser Family Foundation, we will increasingly find the distinctions between information and media literacies breaking down. Generation M, or the media generation, has grown up steeped in media exposure and with unprecedented access to technologies enabling information consumption and production. Recognizing and addressing the unique relationship this generation feels to media and information offers us an exciting opportunity to re-imagine information literacy instruction at the college level. Additionally, media literacy instruction invites librarians to forge dynamic working partnerships with professors, information technologists, and local media activists. While the term information literacy might alienate some potential allies, media studies scholarship is a familiar discipline for faculty and media-makers already working with film, television, journalism cyber-journalism, and digital media
Fluctuations in a diffusive medium with gain
We present a stochastic model for amplifying, diffusive media like, for
instance, random lasers. Starting from a simple random-walk model, we derive a
stochastic partial differential equation for the energy field with contains a
multiplicative random-advection term yielding intermittency and power-law
distributions of the field itself. Dimensional analysis indicate that such
features are more likely to be observed for small enough samples and in lower
spatial dimensions
Damage functions for climate-related hazards: Unification and uncertainty analysis
Most climate change impacts manifest in the form of natural
hazards. Damage assessment typically relies on damage functions that
translate the magnitude of extreme events to a quantifiable damage. In
practice, the availability of damage functions is limited due to a lack of
data sources and a lack of understanding of damage processes. The study of
the characteristics of damage functions for different hazards could
strengthen the theoretical foundation of damage functions and support their
development and validation. Accordingly, we investigate analogies of damage
functions for coastal flooding and for wind storms and identify a unified
approach. This approach has general applicability for granular portfolios and
may also be applied, for example, to heat-related mortality. Moreover, the
unification enables the transfer of methodology between hazards and a
consistent treatment of uncertainty. This is demonstrated by a sensitivity
analysis on the basis of two simple case studies (for coastal flood and storm
damage). The analysis reveals the relevance of the various uncertainty
sources at varying hazard magnitude and on both the microscale and the
macroscale level. Main findings are the dominance of uncertainty from the
hazard magnitude and the persistent behaviour of intrinsic uncertainties on
both scale levels. Our results shed light on the general role of
uncertainties and provide useful insight for the application of the unified
approach
Analytic Modeling of the Hydrodynamic, Thermal, and Structural Behavior of Foil Thrust Bearings
A simulation and modeling effort is conducted on gas foil thrust bearings. A foil bearing is a self acting hydrodynamic device capable of separating stationary and rotating components of rotating machinery by a film of air or other gaseous lubricant. Although simple in appearance these bearings have proven to be complicated devices in analysis. They are sensitive to fluid structure interaction, use a compressible gas as a lubricant, may not be in the fully continuum range of fluid mechanics, and operate in the range where viscous heat generation is significant. These factors provide a challenge to the simulation and modeling task. The Reynolds equation with the addition of Knudsen number effects due to thin film thicknesses is used to simulate the hydrodynamics. The energy equation is manipulated to simulate the temperature field of the lubricant film and combined with the ideal gas relationship, provides density field input to the Reynolds equation. Heat transfer between the lubricant and the surroundings is also modeled. The structural deformations of the bearing are modeled with a single partial differential equation. The equation models the top foil as a thin, bending dominated membrane whose deflections are governed by the biharmonic equation. A linear superposition of hydrodynamic load and compliant foundation reaction is included. The stiffness of the compliant foundation is modeled as a distributed stiffness that supports the top foil. The system of governing equations is solved numerically by a computer program written in the Mathematica computing environment. Representative calculations and comparisons with experimental results are included for a generation I gas foil thrust bearing
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