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Dive into the research topics where Ashraf A Abdou is active.

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Featured researches published by Ashraf A Abdou.


Journal of Nuclear Science and Technology | 2010

Distribution of Microbubble Sizes and Behavior of Large Bubbles in Mercury Flow in a Mockup Target Model of J-PARC

Katsuhiro Haga; Takashi Naoe; Hiroyuki Kogawa; Hidetaka Kinoshita; Masato Ida; Masatoshi Futakawa; Bernie Riemer; Mark Wendel; David K Felde; Ashraf A Abdou

(2010). Distribution of Microbubble Sizes and Behavior of Large Bubbles in Mercury Flow in a Mockup Target Model of J-PARC. Journal of Nuclear Science and Technology: Vol. 47, No. 10, pp. 849-852.


ASME 2010 3rd Joint US-European Fluids Engineering Summer Meeting collocated with 8th International Conference on Nanochannels, Microchannels, and Minichannels | 2010

Creating Small Gas Bubbles in Flowing Mercury Using Turbulence at an Orifice

Mark Wendel; Ashraf A Abdou; Vincent C. Paquit; David K Felde; Bernie Riemer

Pressure waves created in liquid mercury pulsed spallation targets have been shown to create cavitation damage to the target container. One way to mitigate such damage would be to absorb the pressure pulse energy into a dispersed population of small bubbles, however, creating such a population in mercury is difficult due to the high surface tension and particularly the non-wetting behavior of mercury on gas-injection hardware. If the larger injected gas bubbles can be broken down into small bubbles after they are introduced to the flow, then the material interface problem is avoided. Research at the Oak Ridge National Labarotory is underway to develop a technique that has shown potential to provide an adequate population of small-enough bubbles to a flowing spallation target. This technique involves gas injection at an orifice of a geometry that is optimized to the turbulence intensity and pressure distribution of the flow, while avoiding coalescence of gas at injection sites. The most successful geometry thus far can be described as a square-toothed orifice having a 2.5 bar pressure drop in the mercury flow of 8 L/s for one of the target inlet legs. High-speed video and high-resolution photography have been used to quantify the bubble population on the surface of the mercury downstream of the gas injection site. Also, computational fluid dynamics has been used to optimize the dimensions of the toothed orifice based on a RANS computed mean flow including turbulent energies such that the turbulent dissipation and pressure field are best suited for turbulent break-up of the gas bubbles.Copyright


ASME 2009 Fluids Engineering Division Summer Meeting | 2009

CFD Validation of Gas Injection in Flowing Mercury Over Vertical Smooth and Grooved Wall

Ashraf A Abdou; Mark Wendel; David K Felde; Bernard Reimer

The Spallation Neutron Source (SNS) is an accelerator-based neutron source at Oak Ridge National Laboratory (ORNL).The nuclear spallation reaction occurs when a proton beam hits liquid mercury. This interaction causes thermal expansion of the liquid mercury which produces high pressure waves. When these pressure waves hit the target vessel wall, cavitation can occur and erode the wall. Research and development efforts at SNS include creation of a vertical protective gas layer between the flowing liquid mercury and target vessel wall to mitigate the cavitation damage erosion and extend the life time of the target. Since mercury is opaque, computational fluid dynamics (CFD) may be used as a diagnostic tool to visualize the behavior of the liquid mercury and guide the experimental efforts. In this study, CFD simulations of three dimensional, unsteady, turbulent, two-phase flow of helium gas injection in flowing liquid mercury over smooth, vertically grooved and horizontally grooved walls are carried out with the commercially available CFD code Fluent-12 from ANSYS. The Volume of Fluid (VOF) model is used to track the helium-mercury interface. V-shaped vertical and horizontal grooves with 0.5 mm pitch and about 0.7 mm depth were machined in the transparent wall of acrylic test sections. Flow visualization data of helium gas coverage through transparent test sections is obtained with a high-speed camera at the ORNL Target Test Facility (TTF). The helium gas mass flow rate is 8 mg/min and introduced through a 0.5 mm diameter port. The inlet mercury mass flow rate is 51 kg/s and the predicted local mercury velocity is 0.9 m/s. In this paper, the helium gas flow rate and the local mercury velocity are kept constant for the three cases. Time integration of predicted helium gas volume fraction over time is done to evaluate the gas coverage and calculate the average thickness of the helium gas layer. The predicted time-integrated gas coverage over vertically grooved and horizontally grooved test sections is better than over a smooth wall. The simulations show that the helium gas is trapped inside the grooves.Copyright


ASME 2009 Fluids Engineering Division Summer Meeting | 2009

Update on Progress in Creating Stabilized Gas Layers in Flowing Liquid Mercury

Mark Wendel; David K Felde; Ashraf A Abdou; Bernard Reimer

The Spallation Neutron Source (SNS) facility in Oak Ridge, Tennessee uses a liquid mercury target that is bombarded with protons to produce a pulsed neutron beam for materials research and development. In order to mitigate expected cavitation damage erosion (CDE) of the containment vessel, a two-phase flow arrangement of the target has been proposed and was earlier proven to be effective in significantly reducing CDE in non-prototypical target bodies. This arrangement involves covering vulnerable surfaces with a protective layer of gas. The difficulty lies in establishing a persistent gas layer that is oriented vertically and holds up to the strong buoyancy force and the turbulent mercury flow. Several new multiphase experiments have been completed at the Oak Ridge National Laboratory toward developing such layers. The gas hold-up is accomplished by machining regular features (grooves or pits) into the wall with dimensions on the order of 1 mm. The thickness of the gas layer varies, and it is currently unknown how thick a layer must be in order to successfully mitigate the damage, although this aspect is also under investigation. The paper includes a description of the various tests, a presentation of high-speed video images of the gas/mercury interaction viewed through a transparent window, and a discussion of how the results can be used to design a new SNS target that might be resistant to cavitation damage erosion.Copyright


Volume 6: Fluids and Thermal Systems; Advances for Process Industries, Parts A and B | 2011

Two-Phase Flow Simulations of Protective Gas Layer for Spallation Neutron Source Target

Ashraf A Abdou; Mark Wendel; Bernie Riemer; Eric Volpenhein; Robert A. Brewster

The Spallation Neutron Source (SNS) is an accelerator-based neutron source at Oak Ridge National Laboratory (ORNL). The nuclear spallation reaction occurs when a proton beam hits liquid mercury. This interaction causes thermal expansion of the liquid mercury which produces high pressure waves. When these pressure waves hit the target vessel wall, cavitation can occur and erode the wall. Research and development efforts at SNS include creation of a vertical protective gas layer between the flowing liquid mercury and target vessel wall to mitigate the cavitation damage erosion and extend the life time of the target. Since mercury is opaque, computational fluid dynamics (CFD) has been used to visualize the general behavior of a protective gas layer arising from various delivery and retention concepts as a guide for design of experimental efforts. Recent advancements in capacity for large scale CFD modeling via the high performance compute systems of ORNL now enable high-fidelity simulation approaching full geometric scale. Accordingly, in this study, CFD simulations of three dimensional, unsteady, turbulent, two-phase flow of helium gas injection in flowing liquid mercury over textured walls are carried out for target design purposes with the commercially available CFD code STARCCM+. The Volume of Fluid (VOF) model is used to track the helium-mercury interface. Different combinations of conical pits and V-shaped straight grooves at different orientations with respect to the gravity vector are simulated at the SNS proton beam window to increase the helium gas holdup. Time integration of predicted helium gas volume fraction over time is done for the design alternatives considered to compare the gas coverage and average thickness of the helium gas layer.Copyright


Journal of Nuclear Materials | 2012

Status of R&D on mitigating the effects of pressure waves for the Spallation Neutron Source mercury target

Bernie Riemer; Mark Wendel; David K Felde; Ashraf A Abdou; David A McClintock


Journal of Nuclear Materials | 2014

Small Gas Bubble Experiment for Mitigation of Cavitation Damage and Pressure Waves in Short-pulse Mercury Spallation Targets

Bernie Riemer; Mark Wendel; David K Felde; R.L. Sangrey; Ashraf A Abdou; David L. West; T.J. Shea; S. Hasegawa; Hiroyuki Kogawa; Takashi Naoe; C.H. Farny; A.L. Kaminsky


Journal of Nuclear Materials | 2014

Correlation between simulations and cavitation-induced erosion damage in Spallation Neutron Source target modules after operation

Bernie Riemer; David A McClintock; Saulius Kaminskas; Ashraf A Abdou


Physics Procedia | 2014

Tests on the SNS Rotating Target Design at the RTFT (ESS BILBAO)

A. Ghiglino; M. Magán; A. Zarraoa-Garmendia; Bernie Riemer; F. Sordo; Ashraf A Abdou; Thomas J McManamy; F. J. Bermejo; J.M. Perlado


Volume 2, Fora: Cavitation and Multiphase Flow; Fluid Measurements and Instrumentation; Microfluidics; Multiphase Flows: Work in Progress | 2013

Choked-Flow Inlet Orifice Bubbler for Creating Small Bubbles in Mercury

Mark Wendel; Ashraf A Abdou; Bernie Riemer

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Bernie Riemer

Oak Ridge National Laboratory

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Mark Wendel

Oak Ridge National Laboratory

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David K Felde

Oak Ridge National Laboratory

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Bernard Reimer

Oak Ridge National Laboratory

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David A McClintock

Oak Ridge National Laboratory

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Hiroyuki Kogawa

Japan Atomic Energy Agency

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Takashi Naoe

Japan Atomic Energy Agency

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Alexander P Zhukov

Oak Ridge National Laboratory

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