Studies on Attenuation in Ultrasonic Flow Meter Shalini1, G. J

Slides:



Advertisements
Similar presentations
Ultrasound sensors for micromoulding M. Kobayashi*, C.-K. Jen, C. Corbeil, Y. Ono, H. Hébert and A. Derdouri Industrial Materials Institute, National Research.
Advertisements

1 CFD Workshop on Test Cases, Databases & BPG for Nuclear Power Plants Applications, 16 July CFD Quality & Trust: mixed and natural convection test.
Computational Fluid Dynamics (CFD) Study on the Influence of Airflow Patterns on Carbon Dioxide Distribution and Emission Rate in a Scaled Livestock Building.
Convection Convection Matt Penrice Astronomy 501 University of Victoria.
EE 5340/7340, SMU Electrical Engineering Department, © Carlos E. Davila, Electrical Engineering Dept. Southern Methodist University slides can be.
Wireless Underwater Power Transmission (WUPT) for Lithium Polymer Charging James D’Amato Shawn French Warsame Heban Kartik Vadlamani December 5, 2011 School.
ECE 501 Introduction to BME
Low frequency coda decay: separating the different components of amplitude loss. Patrick Smith Supervisor: Jürgen Neuberg School of Earth and Environment,
Laminar and Turbulent Flow
Kern Method of SHELL-AND-TUBE HEAT EXCHANGER Analysis
CHAPTER 1O Measuring Fluid Flow Rate, Fluid Velocity,
What is it?. Fluid Mechanics  The study of fluids and the forces on them.  What are fluids?
Flow Measurements Identify an effect that depends on flowrate
Paul Drosinis UBC Phys 420. Introduction Short history on fluid dynamics Why bother studying fluid flow? Difference between Newtonian and Non-Newtonian.
Objective To study the effect of sub surface defects in surface roughness monitoring through ultrasonic flaw detector. To study the sizing of defects.
Doppler echocardiography & Magnetic Resonance Imaging.
GENERAL ULTRASONIC SYSTEM  TRANSMITTER CIRCUIT  ULTRASONIC TRANSDUCERS  RECEIVER CIRCUIT  MEASURING CIRCUIT  ANALYZER CIRCUIT  SIGNAL PROCESSOR 
10/20/2015Copyright © 2008 Ballios, Dow, Vogtmann, Zofchak.
GENERAL ULTRASONIC SYSTEM
Equation of State Thermal Expansion Bulk Modulus Shear Modulus Elastic Properties.
HYDRAULICS of steady and pulsatile flow in systemic circulation Motivation Experimental techniques for measurement pressure and flowrate How to calculate.
CLIC Prototype Test Module 0 Super Accelerating Structure Thermal Simulation Introduction Theoretical background on water and air cooling FEA Model Conclusions.
A RANS Based Prediction Method of Ship Roll Damping Moment Kumar Bappaditya Salui Supervisors of study: Professor Dracos Vassalos and Dr. Vladimir Shigunov.
4.2 Notes RESISTANCE IN FLUID SYSTEMS. Resistance in Fluid Systems Drag - the force opposing motion when a solid moves through a fluid Drag occurs only.
Analysis of flow through packed beds WJS van der Merwe, CG du Toit, J-H Kruger North-West University Energy Postgraduate Conference 2013.
University of Kurdistan Food Quality Evaluation Methods (FQEM) Lecturer: Kaveh Mollazade, Ph.D. Department of Biosystems Engineering, Faculty of Agriculture,
PRESENTATION OF CFD ACTIVITIES IN CV GROUP Daniel Gasser.
Surface Acoustics Wave Sensors. Outline Introduction Piezoelectricity effect Fabrication of acoustic waves devices Wave propagation modes Bulk Wave sensor.
Bulatom Confernce June 2007
Ultrasound. History: Available in 19th century. Available in 19th century. Was for sonar (SONAR  Sound Navigation and Ranging) Was for sonar (SONAR 
McNeese State University Department of Engineering.
Date of download: 6/2/2016 Copyright © ASME. All rights reserved. From: Experimental Research on Velocity Distribution and Attenuation Characteristic of.
EKT 451 CHAPTER 6 Sensor & Transducers.
Date of download: 9/19/2016 Copyright © ASME. All rights reserved. From: A Reduced-Order Model of the Mean Properties of a Turbulent Wall Boundary Layer.
Measuring principles Introduction 1.
Portland State University Ali Hafiz and Thomas Schumacher
By ASST. Prof. DR. ASEEL BASIM
Reynolds Number (Re) Viscosity: resistance of a liquid to change of form. Inertia: resistance of an object (body) to a change in its state of motion.
Kessler-Ellis Products
Bhabha Atomic Research Centre
Titolo presentazione sottotitolo
Internal Incompressible
Date of download: 10/22/2017 Copyright © ASME. All rights reserved.
Date of download: 10/26/2017 Copyright © ASME. All rights reserved.
Fig. 4 Block diagram of system
Date of download: 11/5/2017 Copyright © ASME. All rights reserved.
Ultrasound.
Date of download: 11/9/2017 Copyright © ASME. All rights reserved.
Date of download: 12/16/2017 Copyright © ASME. All rights reserved.
TEKNIK MESIN FAKULTAS TEKNOLOGI INDUSTRI UNIVERSITAS MERCU BUANA
Date of download: 12/23/2017 Copyright © ASME. All rights reserved.
Date of download: 12/25/2017 Copyright © ASME. All rights reserved.
Spatially Varying Frequency Compounding of Ultrasound Images
Food Quality Evaluation Methods (FQEM)
Wave Properties.
PD Detection on Metal Enclosed Switchgear Panels
Review of Ultrasonic Imaging
CFD – Fluid Dynamics Equations
Numerical Study of the Wall Slip Reduction Effects for a Double Concentric Cylinder Rheometer with Slotted Rotor D. De Kee, Department of Chemical and.
Exp. 1- Viscosity.
Control System Instrumentation
REAL FLUIDS SECTION 4.
HYDRAULICS of steady and pulsatile flow in systemic circulation
Topic 6 NavierStokes Equations
Finite element Analysis study of P-U based Acoustic Vector Sensor for Underwater Application in COMSOL Bipin Kumar1, Arun Kumar1, Rajendar Bahl1 1Centre.
Fig. 4 Block diagram of system
Ultrasonic Rangefinder
KROHNE Ultrasonic Flowmeters
Understanding Network Analysis
Priyabrata Mandal, Priya Goel, Anusha Chandra, Dr. Sujay Chattopadhyay
Presentation transcript:

Studies on Attenuation in Ultrasonic Flow Meter Shalini1, G. J Studies on Attenuation in Ultrasonic Flow Meter Shalini1, G.J.Gorade1, Rohini Datar1, S.K.Sinha1 1. Reactor Engineering Division, Bhabha Atomic Research Centre, Mumbai, India Introduction: Ultrasonic technology is used for various crucial measurements in the industry. Like every other energy waveform the ultrasonic waveforms also suffers attenuation while travelling through a medium. This attenuation is a function of the square of resonant frequency of the ultrasonic waveform, thermal coefficient of the medium, bulk and shear viscosity of the medium. If the attenuation is high the received signal becomes almost undetectable. Results: Figure 3: Pressure signal at transmitter and the Receiver when 1MHz transducer is used Figure 4: Variation in pressure ratio (Received versus Transmitted) with frequency of the transducer Computational Methods: Turbulent flow k-ℇ model in Computational Fluid Dynamics module has been used to simulate various flow rates. The thermos-viscous model under pressure acoustics was utilised to study the waveform attenuation Figure 1 : Velocity magnitude via CFD computation Conclusions It can be seen that as the frequency of the ultrasonic transducer increases the ratio of pressure magnitude at the Receiver to that at the transmitter decreases exponentially. Studies done till now are for ultrasonic flowmeter with water as a medium, however the same approach can be effectively used to do attenuation studies for other mediums too. The model for Non-destructive testing and level measurement can also be made on similar lines. Figure 2 : Acoustic pressure on the surface via Thermo-Viscous Module