Chapter 3: FLUID FLOW CHAPTER THREE FLUID FLOW 3.1 3.2 3.3 3.4 3.5 Fluid Flow Unit Pump Test Unit Hydraulics bench and accessories Flow Curve Determination for Non-Newtonian Fluids Fixed and Fluidized Bed Facts which at first seem improbable will‚ even in scant explanation‚ drop the cloak which has hidden them and stand forth in naked and simple beauty. GALILEO GALILEI 1 3.1. FLUID FLOW UNIT Keywords: Pressure loss‚ straight pipe‚ pipe bend‚ orifice meter‚ venturi meter
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CBE 6333‚ R. Levicky 1 Potential Flow Part I. Theoretical Background. Potential Flow. Potential flow is frictionless‚ irrotational flow. Even though all real fluids are viscous to some degree‚ if the effects of viscosity are sufficiently small then the accompanying frictional effects may be negligible. Viscous effects become negligible‚ for example‚ for flows at high Reynolds number that are dominated by convective transport of momentum. Thus potential flow is often useful for analyzing external
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The objective : 1. To determine the head loss and friction factor for laminar & turbulent flow in a smooth pipe over a range of Reynolds’s number . 2. To obtain the following relationships : a. Head loss as a function of the velocity of flow . b. Friction factor as a function of Reynolds number . Theory : The friction resistance to the flow of fluid through a pipe results in a loss of pressure energy for a given fluid flowing a long a given pipe‚ experiments show that for laminar flow
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Abstract This experiment of the friction loss along a smooth pipe shows that there are existence of laminar and transitional flows as stated in Graph 2.0 and Graph 2.1. It is proven that the higher velocity along the smooth bore pipe‚ the higher is the head loss of water. As shown in Table 3.0‚ when the Reynolds’ number increases‚ the value of pipe coefficient friction‚ f decreases along the decreasing stead laminar line. On top of that‚ there are energy loss from the water to the surface of the
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Should you fail to attend either one you will be asked to complete some extra work. This will involve a detailed report and further questions. The simplest strategy is to do the lab.] Notes For the First Year Lecture Course: An Introduction to Fluid Mechanics School of Civil Engineering‚ University of Leeds. Homework: Example sheets: These will be given for each section of the course. Doing these will greatly improve your exam mark. They are course work but do not have credits toward the
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A Coefficient of Friction Estimation Monitoring System for Autonomous Off-Road Vehicles Using Wide Area Augme- ntation Systems (WAAS) and a Magnetic Pulse Generator Shaft Encoder Abstract: The proposed work introduces a means of developing a friction measurement system that has many applications in vehicle safety systems such as Anti-lock Braking System (ABS) and Traction Control System (TCS). Rapid weather and road conditions would change the behavior of the vehicle and a need of a system to
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point in a fluid has the same magnitude in all directions. (Pressure is a scalar) Variation of Pressure with Depth It will come as no surprise to you that pressure in a fluid at rest does not change in the horizontal direction. This can be shown easily by considering a thin horizontal layer of fluid and doing a force balance in any horizontal direction. However‚ this is not the case in the vertical direction in a gravity field. Pressure in a fluid increases with depth because more fluid rests on
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A Manual for the MECHANICS of FLUIDS LABORATORY William S. Janna Department of Mechanical Engineering Memphis State University ©1997 William S. Janna All Rights Reserved. No part of this manual may be reproduced‚ stored in a retrieval system‚ or transcribed in any form or by any means—electronic‚ magnetic‚ mechanical‚ photocopying‚ recording‚ or otherwise— without the prior written consent of William S. Janna 2 TABLE OF CONTENTS Item Page Report Writing............
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EN 1029 Laboratory Laboratory FM Declaration: In submitting this report‚ I hereby declare that‚ except where I have made clear and full reference to the work of others‚ this submission‚ and all the material (e.g. text‚ pictures‚ diagrams) contained in it‚ is my own work‚ has not previously been submitted for assessment‚ and I have not knowingly allowed it to be copied by another student. In the case of group projects‚ the contribution of group members has been appropriately quantified. I understand
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Id Question The fluid property‚ due to which‚ mercury does not wet the glass is A surface tension B viscosity C cohesion D adhesion Answer A Marks 1 Unit A1 Id Question The dimension of dynamic viscosity is A ML-1T-1 B L2T-1 C LT-2 D ML-1T-2 Answer A Marks 2 Unit A1 Id Question The fluid‚ in which the shearing stress within it is proportional to the velocity gradient across the sheared section‚ is called a __________ fluid. A Bingham B Newtonian
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