scholarly journals Kinetic quasi-viscous and bulk flow inertia effects in collisionless magnetotail reconnection

1998 ◽  
Vol 103 (A1) ◽  
pp. 199-213 ◽  
Author(s):  
Masha M. Kuznetsova ◽  
Michael Hesse ◽  
Dan Winske
Keyword(s):  
Bulk Flow ◽  
Inertia Effects ◽  
Magnetotail Reconnection ◽  
Flow Inertia

Inertia Effects in Squeeze-Film Damper Bearings Generated by Circumferential Oil Supply Groove

2001 ◽  
Author(s):  
Jørgen W. Lund ◽  
Claus M. Myllerup ◽  
Henning Hartmann
Keyword(s):  
Dynamic Properties ◽  
Bulk Flow ◽  
Squeeze Film ◽  
Perturbation Approach ◽  
Inertia Effects ◽  
Squeeze Film Damper ◽  
Oil Supply ◽  
Reaction Forces ◽  
Flow Approximation ◽  
Acceleration Term

Abstract The dynamic properties of an industrial Squeeze-Film Damper (SFD) bearing design are described using the well-known perturbation approach, where the reaction forces induced by small movements away from the position of equilibrium are expanded into a Taylor series in terms of displacement, velocity, and acceleration. Although generally negligible, the acceleration term can become significant in SFD bearings when inertia effects in the damper lands are enhanced by the flow in a central circumferential oil supply groove. By using a bulk flow approximation in the oil supply groove an explicit expression is derived for the acceleration term. Experimental results confirm the significance of the oil supply groove geometry and appear to validate the bulk flow approximation.

Significance of Inertia in Subcompartment Analysis

2001 ◽  
Author(s):  
G. K. Ashley ◽  
W. E. Schuh
Keyword(s):  
Method Of Characteristics ◽  
Flow Path ◽  
Pressure Differential ◽  
Fluid Inertia ◽  
Inertia Effects ◽  
Flow Approximation ◽  
Accepted Practice ◽  
Flow Inertia ◽  
Static Flow

Abstract When simulating quasi-static inter-compartment flow it is currently accepted practice to include fluid inertia effects in the compartments by extending the flow path beyond its geometrical limits. Such an extension simulates inertia by effectively adding mass to the flow path that the pressure differential between the compartments must overcome. In this paper, the effects of flow inertia are investigated by comparing results for two connected compartments using a quasi-static flow approximation that neglects inertia with results from a method of characteristics program that does include inertia. Comparison of simulations employing these methodologies can be used to assess the influence of inertia during inter-compartment flow.

Inertia Effects in Squeeze-Film Damper Bearings Generated by Circumferential Oil Supply Groove

2003 ◽  
Vol 125 (4) ◽  
pp. 495-499 ◽  
Author(s):  
Jørgen W. Lund ◽  
Claus M. Myllerup ◽  
Henning Hartmann
Keyword(s):  
Dynamic Properties ◽  
Bulk Flow ◽  
Squeeze Film ◽  
Perturbation Approach ◽  
Inertia Effects ◽  
Squeeze Film Damper ◽  
Oil Supply ◽  
Reaction Forces ◽  
Flow Approximation ◽  
Acceleration Term

The dynamic properties of an industrial Squeeze-Film Damper (SFD) bearing design are described using the well-known perturbation approach, where the reaction forces induced by small movements away from the position of equilibrium are expanded into a Taylor series in terms of displacement, velocity, and acceleration. Although generally negligible, the acceleration term can become significant in SFD bearings when inertia effects in the damper lands are enhanced by the flow in a central circumferential oil supply groove. By using a bulk flow approximation in the oil supply groove an explicit expression is derived for the acceleration term. Experimental results confirm the significance of the oil supply groove geometry and appear to validate the bulk flow approximation.

Bulk flow driven by a viscous monolayer

2015 ◽  
Vol 785 ◽  
pp. 283-300 ◽  
Author(s):  
Aditya Raghunandan ◽  
Juan M. Lopez ◽  
Amir H. Hirsa
Keyword(s):  
Stokes Flow ◽  
Water Surface ◽  
Bulk Flow ◽  
Bulk Liquid ◽  
Knife Edge ◽  
Viscous Coupling ◽  
Interfacial Film ◽  
Monomolecular Film ◽  
Wide Range ◽  
Flow Inertia

The flow in the bulk driven by a viscous interfacial film set in motion by a rotating sharp circular knife edge has been examined through experiments and computations. In the experiments, the water surface is covered by an insoluble monomolecular film of dipalmitoylphosphatidylcholine (DPPC), a molecule of wide interest in biology and medicine. It is shown that the viscous coupling between the interfacial film and the bulk liquid leads to a strong bulk flow. Depending on the surface packing and corresponding surface tension, DPPC monolayers exhibit a wide range of phase morphologies. Upon shearing the monolayer, its viscous response varies from that of an essentially inviscid film at low surface packing, to that of a highly viscous non-Newtonian (shear thinning) film when the packing is dense. The more viscous the film, the stronger the driven bulk flow. We have examined this behaviour for hydrodynamic regimes straddling the Stokes flow regime and where flow inertia is important.

Fisiopatología de la hidrocefália idiopática de presión normal (parte 3): sistemaa glinfático

2016 ◽  
Vol 21 (2) ◽  
pp. 28-37
Author(s):  
Oscar Solís-Salgado ◽  
José Luis López-Payares ◽  
Mauricio Ayala-González
Keyword(s):  
Amyloid Beta ◽  
Interstitial Fluid ◽  
Amyloid Β ◽  
Bulk Flow ◽  
Polyethylene Glycols ◽  
Brain Interstitial Fluid ◽  
El Sistema ◽  
Arterial Pulsation ◽  
The Brain

Las vías de drenaje solutos del sistema nervioso central (SNC) participan en el recambio de liquido intersticial con el líquido cefalorraquídeo (LIT-LCR), generando un estado de homeostasis. Las alteraciones dentro de este sistema homeostático afectará la eliminación de solutos del espacio intersticial (EIT) como el péptido βa y proteína tau, los cuales son sustancias neurotóxicas para el SNC. Se han utilizado técnicas experimentales para poder analizar el intercambio LIT-LCR, las cuales revelan que este intercambio tiene una estructura bien organizada. La eliminación de solutos del SNC no tiene una estructura anatómica propiamente, se han descubierto vías de eliminación de solutos a través de marcadores florecentes en el espacio subaracnoideo, cisternas de la base y sistema ventricular que nos permiten observar una serie de vías ampliamente distribuidas en el cerebro. El LCR muestra que tiene una función linfática debido a su recambio con el LIT a lo largo de rutas paravasculares. Estos espacios que rodean la superficie arterial así como los espacios de Virchow-Robin y el pie astrocitico junto con la AQP-4, facilitan la entrada de LCR para-arterial y el aclaramiento de LIT para-venoso dentro del cerebro. El flujo y dirección que toma el LCR por estas estructuras, es conducido por la pulsación arterial. Esta función será la que finalmente llevara a la eliminación de estas sustancias neurotóxicas. En base a la dependencia de este flujo para la eliminación de sustancias se propone que el sistema sea llamado “ la Vía Glinfática”. La bibliografía así como las limitaciones que se encuentran en esta revisión están dadas por la metodología de búsqueda que ha sido realizada principalmente en PubMed utilizando los siguientes términos Mesh: Cerebral Arterial Pulsation, the brain via paravascular, drainage of amyloid-beta, bulk flow of brain interstitial fluid, radiolabeled polyethylene glycols and albumin, amyloid-β, the perivascular astroglial sheath, Brain Glymphatic Transport.

Secretory Bulk Flow of Soluble Proteins Is Efficient and COPII Dependent

2001 ◽  
Vol 13 (9) ◽  
pp. 2005-2020 ◽  
Author(s):  
B. A. Phillipson
Keyword(s):  
Soluble Proteins ◽  
Bulk Flow

Investigation of the Squeeze Film Dynamics Underneath a Microstructure With Large Oscillation Amplitudes and Inertia Effects

2016 ◽  
Vol 138 (3) ◽  
Author(s):  
Nadim A. Diab ◽  
Issam A. Lakkis
Keyword(s):  
Rarefied Gas ◽  
Direct Simulation Monte Carlo ◽  
Squeeze Film ◽  
Dsmc Method ◽  
Inertia Effects ◽  
Flow Parameters ◽  
Fluid Behavior ◽  
Dimensionless Groups ◽  
Simulation Monte Carlo ◽  
The Impact

This paper presents direct simulation Monte Carlo (DSMC) numerical investigation of the dynamic behavior of a gas film in a microbeam. The microbeam undergoes large amplitude harmonic motion between its equilibrium position and the fixed substrate underneath. Unlike previous work in literature, the beam undergoes large displacements throughout the film gap thickness and the behavior of the gas film along with its impact on the moving microstructure (force exerted by gas on the beam's front and back faces) is discussed. Since the gas film thickness is of the order of few microns (i.e., 0.01 < Kn < 1), the rarefied gas exists in the noncontinuum regime and, as such, the DSMC method is used to simulate the fluid behavior. The impact of the squeeze film on the beam is investigated over a range of frequencies and velocity amplitudes, corresponding to ranges of dimensionless flow parameters such as the Reynolds, Strouhal, and Mach numbers on the gas film behavior. Moreover, the behavior of compressibility pressure waves as a function of these dimensionless groups is discussed for different simulation case studies.

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