A Numerical and Experimental Investigation of Taylor Flow Instabilities in Narrow Gaps and Their Relationship to Turbulent Flow
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Experimental and Numerical Characterization of the Thermal and Hydraulic Performance of a Canned Motor Pump Operating with Two-P
EXPERIMENTAL AND NUMERICAL CHARACTERIZATION OF THE THERMAL AND HYDRAULIC PERFORMANCE OF A CANNED MOTOR PUMP OPERATING WITH TWO-PHASE FLOW A Dissertation by YINTAO WANG Submitted to the Office of Graduate and Professional Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Chair of Committee, Adolfo Delgado Committee Members, Karen Vierow Kirkland Michael Pate Je-Chin Han Head of Department, Andreas A. Polycarpou May 2019 Major Subject: Mechanical Engineering Copyright 2019 Yintao Wang ABSTRACT Canned motor pump (CMP), as one kind of sealless pump, has been utilized in industry for many years to handle hazards or toxic product and to minimize leakage to the environment. In a canned motor pump, the impeller is directly mounted on the motor shaft and the pump bearing is usually cooled and lubricated by the pump process liquid. To be employed in oil field, CMP must have the ability to work under multiphase flow conditions, which is a common situation for artificial lift. In this study, we studied the performance and reliability of a vertical CMP from Curtiss-Wright Corporation in oil and air two-phase flow condition. Part of the process liquid in this CMP is recirculated to cool the motor and lubricate the thrust bearing. The pump went through varying flow rates and different gas volume fractions (GVFs). In the test, three important parameters, including the hydraulic performance, the pump inside temperature and the thrust bearing load were monitored, recorded and analyzed. The CMP has a second recirculation loop inside the pump to lubricate the thrust bearing as well as to cool down the motor windings. -
Simulation and Modeling of the Hydrodynamic, Thermal, and Structural Behavior of Foil Thrust Bearings
Simulation and Modeling of the Hydrodynamic, Thermal, and Structural Behavior of Foil Thrust Bearings by Robert Jack Bruckner Submitted in partial fulfillment of the requirements For the degree of Doctor of Philosophy Dissertation Advisor: Dr. Joseph M. Prahl Department of Mechanical and Aerospace Engineering CASE WESTERN RESERVE UNIVERSITY August, 2004 Dedications All of the work leading to and included in these pages is dedicated to the loving support of my family, Lisa, Eric, and Elisabeth Table of Contents CHAPTER 1 Introduction to Foil Bearings .........................................................................................17 1.1 Historical Context of Hydrodynamics.............................................................17 1.2 Foil Bearing State of the Art...........................................................................19 1.3 Aviation Turbofan Engine Application...........................................................22 1.4 Typical Geometries and Characteristics of Foil Thrust Bearings.....................23 CHAPTER 2 Development of the Governing Equations......................................................................29 2.1 The Generalized Foil Bearing Problem...........................................................29 2.2 Reynolds Equation .........................................................................................29 2.2.1 Development from Mass and Momentum Conservation..............................29 2.2.3 Cylindrical (Thrust Pad) Form of Reynolds Equation .................................40 -
Concentric Cylinder Viscometer Flows of Herschel-Bulkley Fluids Received Sep 09, 2019; Accepted Nov 28, 2019
Appl. Rheol. 2019; 29 (1):173–181 Research Article Hans Joakim Skadsem* and Arild Saasen Concentric cylinder viscometer flows of Herschel-Bulkley fluids https://doi.org/10.1515/arh-2019-0015 Received Sep 09, 2019; accepted Nov 28, 2019 Abstract: Drilling fluids and well cements are example τ non-Newtonian fluids that are used for geothermal and Cement slurry petroleum well construction. Measurement of the non- Spacer Newtonian fluid viscosities are normally performed using a concentric cylinder Couette geometry, where one of the Shear stress, Drilling fluid cylinders rotates at a controlled speed or under a con- trolled torque. In this paper we address Couette flow of yield stress shear thinning fluids in concentric cylinder geometries. We focus Chemical wash on typical oilfield viscometers and discuss effects of yield Shear rate,γ ˙ stress and shear thinning on fluid yielding at low viscome- ter rotational speeds and errors caused by the Newtonian Figure 1: Example of typical flow curves for fluids involved in well shear rate assumption. We relate these errors to possible construction. implications for typical wellbore flows. Keywords: Drilling fluids, Herschel-Bulkley, Viscometry The operation schedule involves drilling, where the drilling fluid transports out drilled cuttings, displacement PACS: 83.85.Jn, 83.60.La, 83.10.Gr, 47.57.Qk of the drilling fluid from the narrow annular space be- tween the casing string and the formation and replace it by a cement slurry to create a total zonal isolation in the well. 1 Introduction Once in place, the cement slurry is allowed to harden into a cement sheath. -
Friction Losses and Heat Transfer in High-Speed Electrical Machines
XK'Sj Friction losses and heat transfer in high-speed electrical machines Juha Saari DJSTR10UTK)N OF THI6 DOCUMENT IS UNLIMITED Teknillinen korkeakoulu Helsinki University of Technology Sahkotekniikan osasto Faculty of Electrical Engineering Sahkomekaniikan laboratorio Laboratory of Electromechanics Otaniemi 1996 1 50 2 Saari J. 1996. Friction losses and heat transfer in high-speed electrical machines. Helsinki University of Technology, Laboratory of Electromechanics, Report 50, Espoo, Finland, p. 34. Keywords: Friction loss, heat transfer, high-speed electrical machine Abstract High-speed electrical machines usually rotate between 20 000 and 100 000 rpm and the peripheral speed of the rotor exceeds 150 m/s. In addition to high power density, these figures mean high friction losses, especially in the air gap. In order to design good electrical machines, one should be able to predict accurately enough the friction losses and heat-transfer rates in the air gap. This report reviews earlier investigations concerning frictional drag and heat transfer between two concentric cylinders with inner cylinder. rotating. The aim was to find out whether these studies cover the operation range of high-speed electrical machines. Friction coefficients have been measured at very high Reynolds numbers. If the air-gap surfaces are smooth, the equations developed can be applied into high-speed machines. The effect of stator slots and axial cooling flows, however, should be studied in more detail. Heat-transfer rates from rotor and stator are controlled mainly by the Taylor vortices in the air-gap flow. Their appearance is affected by the flow rate of the cooling gas. The papers published do not cover flows with both high rotation speed and flow rate. -
Couette and Planar Poiseuille Flow
An Internet Book on Fluid Dynamics COUETTE AND PLANAR POISEUILLE FLOW Couette and planar Poiseuille flow are both steady flows between two infinitely long, parallel plates a fixed distance, h, apart as sketched in Figures 1 and 2. The difference is that in Couette flow one of the plates Figure 1: Couette flow. Figure 2: Planar Poiseuille flow. has a velocity U in its own plane (the other plate is at rest) as a result of the application of a shear stress, τ, and there is no pressure gradient in the fluid. In contrast in planar Poiseuille flow both plates are at rest and the flow is caused by a pressure gradient, dp/dx, in the direction, x, parallel to the plates. It is however, convenient, to begin the analysis of these flows together. We will omit any conservative body forces like gravity since their effects are can be simply added to the final solutions. Then, assuming that the only non-zero component of the velocity is ux and that the velocity and pressure are independent of time the resulting planar continuity equation for an incompressible fluid yields ∂ux ∂x =0 (Bib1) so that ux(y) is a function only of y, the coordinate perpendicular to the plates. Using this the planar Navier-Stokes equations for an incompressible fluid of constant and uniform viscosity reduce to 2 ∂p ∂ ux = μ (Bib2) ∂x ∂y2 ∂p ∂y =0 (Bib3) The second of these shows that the pressure, p(x), is a function only of x and hence the gradient, dp/dx, is well defined and a parameter of the problem. -
Study on Mechanical Bearing Strength and Failure Modes of Composite Materials for Marine Structures
Journal of Marine Science and Engineering Article Study on Mechanical Bearing Strength and Failure Modes of Composite Materials for Marine Structures Dong-Uk Kim 1 , Hyoung-Seock Seo 1,* and Ho-Yun Jang 2 1 School of Naval Architecture & Ocean Engineering, University of Ulsan, Ulsan 44610, Korea; [email protected] 2 Green Ship Research Division, Research Institute of Medium & Small Shipbuilding, Busan 46757, Korea; [email protected] * Correspondence: [email protected] Abstract: With the gradual application of composite materials to ships and offshore structures, the structural strength of composites that can replace steel should be explored. In this study, the mechanical bearing strength and failure modes of a composite-to-metal joining structure connected by mechanically fastened joints were experimentally analyzed. The effects of the fiber tensile strength and stress concentration on the static bearing strength and failure modes of the composite structures ◦ ◦ ◦ ◦ were investigated. For the experiment, quasi-isotropic [45 /0 /–45 /90 ]2S carbon fiber-reinforced plastic (CFRP) and glass fiber-reinforced plastic (GFRP) specimens were prepared with hole diameters of 5, 6, 8, and 10 mm. The experimental results showed that the average static bearing strength of the CFRP specimen was 30% or higher than that of the GFRP specimen. In terms of the failure mode of the mechanically fastened joint, a cleavage failure mode was observed in the GFRP specimen for hole diameters of 5 mm and 6 mm, whereas a net-tension failure mode was observed for hole diameters of 8 mm and 10 mm. Bearing failure occurred in the CFRP specimens. -
Chapter 5 Footing Design
Chapter 5 Footing Design By S. Ali Mirza1 and William Brant2 5.1 Introduction Reinforced concrete foundations, or footings, transmit loads from a structure to the supporting soil. Footings are designed based on the nature of the loading, the properties of the footing and the properties of the soil. Design of a footing typically consists of the following steps: 1. Determine the requirements for the footing, including the loading and the nature of the supported structure. 2. Select options for the footing and determine the necessary soils parameters. This step is often completed by consulting with a Geotechnical Engineer. 3. The geometry of the foundation is selected so that any minimum requirements based on soils parameters are met. Following are typical requirements: • The calculated bearing pressures need to be less than the allowable bearing pressures. Bearing pressures are the pressures that the footing exerts on the supporting soil. Bearing pressures are measured in units of force per unit area, such as pounds per square foot. • The calculated settlement of the footing, due to applied loads, needs to be less than the allowable settlement. • The footing needs to have sufficient capacity to resist sliding caused by any horizontal loads. • The footing needs to be sufficiently stable to resist overturning loads. Overturning loads are commonly caused by horizontal loads applied above the base of the footing. • Local conditions. • Building code requirements. 1 Professor Emeritus of Civil Engineering, Lakehead University, Thunder Bay, ON, Canada. 2 Structural Engineer, Black & Veatch, Kansas City, KS. 1 4. Structural design of the footing is completed, including selection and spacing of reinforcing steel in accordance with ACI 318 and any applicable building code. -
Design for Hydrostatic Bearing of Vertical Type Pump
Transactions of the Korean Nuclear Society Autumn Meeting Gyeongju, Korea, October 29-30, 2015 Design for Hydrostatic Bearing of Vertical Type Pump Kang Soo Kim a, Sung Kyun Kim a, Gyeong Hoi Koo a, Keun Bae Park a aKorea Atomic Energy Research Institute, 989-111 Daedeok-daero, Yuseong-gu, Daejeon *Corresponding author: [email protected] 1. Introduction of sodium(η) at 100 ℃ and 400 ℃ are 0.682 cp, 0.278 cp respectively[2]. 0.278 cp = 0.000278 Pa.s = 0.278×10-9 kg. The primary pump of PGSFR(Prototype Gen IV Sodium sec/mm2. Fast Reactor) performs an important safety function of circulating the coolant across the core to remove the nuclear heat under all operating conditions of the reactor. Design and selection of materials and manufacturing technology for sodium pumps differ to a large extent from conventional pumps because these pumps operate relatively at high temperatures and have high reliability. The configuration of the primary pump of PGSFR is shown in Figure 1. In order to provide guide to the shaft at the bottom part, there is a hydrostatic bearing above the impeller level. In this paper, the FEM(Finite Element Method) analysis was performed to evaluate the unbalance force for the rotary shaft for the design of the hydrostatic bearing and the design methodology and procedures for the hydrostatic bearing are established. Figure 2 FEM model for the unbalance force 2.1 Bearing Pressure Calculation The sodium flow way due to the pressure difference is shown in Figure 3. The sodium discharged from the impellor flows through the diffuser and then, the small part of sodium flows from the diffuser oriffice to the hydrostatic bearing due to the pressure difference. -
Rayleigh-Bernard Convection Without Rotation and Magnetic Field
Nonlinear Convection of Electrically Conducting Fluid in a Rotating Magnetic System H.P. Rani Department of Mathematics, National Institute of Technology, Warangal. India. Y. Rameshwar Department of Mathematics, Osmania University, Hyderabad. India. J. Brestensky and Enrico Filippi Faculty of Mathematics, Physics, Informatics, Comenius University, Slovakia. Session: GD3.1 Core Dynamics Earth's core structure, dynamics and evolution: observations, models, experiments. Online EGU General Assembly May 2-8 2020 1 Abstract • Nonlinear analysis in a rotating Rayleigh-Bernard system of electrical conducting fluid is studied numerically in the presence of externally applied horizontal magnetic field with rigid-rigid boundary conditions. • This research model is also studied for stress free boundary conditions in the absence of Lorentz and Coriolis forces. • This DNS approach is carried near the onset of convection to study the flow behaviour in the limiting case of Prandtl number. • The fluid flow is visualized in terms of streamlines, limiting streamlines and isotherms. The dependence of Nusselt number on the Rayleigh number, Ekman number, Elasser number is examined. 2 Outline • Introduction • Physical model • Governing equations • Methodology • Validation – RBC – 2D – RBC – 3D • Results – RBC – RBC with magnetic field (MC) – Plane layer dynamo (RMC) 3 Introduction • Nonlinear interaction between convection and magnetic fields (Magnetoconvection) may explain certain prominent features on the solar surface. • Yet we are far from a real understanding of the dynamical coupling between convection and magnetic fields in stars and magnetically confined high-temperature plasmas etc. Therefore it is of great importance to understand how energy transport and convection are affected by an imposed magnetic field: i.e., how the Lorentz force affects convection patterns in sunspots and magnetically confined, high-temperature plasmas. -
Performance of Hydrodynamic Journal Bearing Under the Combined Influence of Textured Surface and Journal Misalignment
Performance of hydrodynamic journal bearing under the combined influence of textured surface and journal misalignment: A numerical survey Belkacem Manser, Idir Belaidi, Abderrachid Hamrani, Sofiane Khelladi, Farid Bakir To cite this version: Belkacem Manser, Idir Belaidi, Abderrachid Hamrani, Sofiane Khelladi, Farid Bakir. Performance of hydrodynamic journal bearing under the combined influence of textured surface and journal misalign- ment: A numerical survey. Comptes Rendus Mécanique, Elsevier Masson, 2019, 347 (2), pp.141-165. 10.1016/j.crme.2018.11.002. hal-02438009 HAL Id: hal-02438009 https://hal.archives-ouvertes.fr/hal-02438009 Submitted on 14 Jan 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Performance of hydrodynamic journal bearing under the combined influence of textured surface and journal misalignment: a numerical survey B. MANSER1;∗; I. BELAIDI1; A. HAMRANI1; S. KHELLADI2 & F. BAKIR2 1 LEMI., FSI., University of M’hamed Bougara, Avenue de I’independance,´ 35000-Boumerdes, Algeria. 2 DynFluid Lab., Arts et Metiers´ ParisTech, 151 boulevard de l’Hopital,ˆ 75013-Paris, France. ∗ Corresponding author : [email protected] Abstract A wisely chosen geometry of micro textures with the favorable relative motion of lubricated surfaces in contacts can enhance tribological characteristics, in this paper, a computational investigation related to the combined influence of bearing surface texturing and journal misalignment on the performances of hydrodynamic journal bearings is reported. -
Transition to Turbulence in Plane Poiseuille and Plane Couette Flow by STEVEN A
J. Fluid Mech. (1980), vol. 96, part 1, pp. 159-205 169 Printed in Great Britain Transition to turbulence in plane Poiseuille and plane Couette flow By STEVEN A. ORSZAG AND LAWRENCE C. KELLST Department of Mathematics, Massachusetts Institute of Technology, Cambridge, MA 02139 [Received 8 June 1978 and in revised form 2 October 1978) Direct numerical solutions of the three-dimensional time-dependent Navier-Stokes equations are presented for the evolution of three-dimensional finite-amplitude disturbances of plane Poiseuille and plane Couette flows. Spectral methods using Fourier series and Chebyshev polynomial series are used. It is found that plane Poiseuille flow can sustain neutrally stable two-dimensional finite-amplitude dis- turbances at Reynolds numbers larger than about 2800. No neutrally stable two- dimensional finite-amplitude disturbances of plane Couette flow were found. Three-dimensional disturbances are shown to have a strongly destabilizing effect. It is shown that finite-amplitude disturbances can drive transition to turbulence in both plane Poiseuille flow and plane Couette flow at Reynolds numbers of order 1000. Details of the resulting flow fields are presented. It is also shown that plane Poiseuille flow cannot sustain turbulence at Reynolds numbers below about 500. I. Introduction One of the oldest unsolved problems of fluid mechanics is the theoretical description of the inception and growth of instabilities in laminar shear flows that lead to trans- ition to turbulence. The behaviour of small-amplitude disturbances on a laminar flow is reasonably well understood, but understanding of the behaviour of finite-amplitude disturbances is in a much less satisfactory state. -
Simulation of Taylor-Couette Flow. Part 2. Numerical Results for Wavy-Vortex Flow with One Travelling Wave
J. E’l~idM(&. (1984),FOI. 146, pp. 65-113 65 Printed in Chat Britain Simulation of Taylor-Couette flow. Part 2. Numerical results for wavy-vortex flow with one travelling wave By PHILIP S. MARCUS Division of Applied Sciences and Department of Astronomy, Harvard University (Received 26 July 1983 and in revised form 23 March 1984) We use a numerical method that was described in Part 1 (Marcus 1984a) to solve the time-dependent Navier-Stokes equation and boundary conditions that govern Taylor-Couette flow. We compute several stable axisymmetric Taylor-vortex equi- libria and several stable non-axisymmetric wavy-vortex flows that correspond to one travelling wave. For each flow we compute the energy, angular momentum, torque, wave speed, energy dissipation rate, enstrophy, and energy and enstrophy spectra. We also plot several 2-dimensional projections of the velocity field. Using the results of the numerical calculations, we conjecture that the travelling waves are a secondary instability caused by the strong radial motion in the outflow boundaries of the Taylor vortices and are not shear instabilities associated with inflection points of the azimuthal flow. We demonstrate numerically that, at the critical Reynolds number where Taylor-vortex flow becomes unstable to wavy-vortex flow, the speed of the travelling wave is equal to the azimuthal angular velocity of the fluid at the centre of the Taylor vortices. For Reynolds numbers larger than the critical value, the travelling waves have their maximum amplitude at the comoving surface, where the comoving surface is defined to be the surface of fluid that has the same azimuthal velocity as the velocity of the travelling wave.