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Che 253M Experiment No. 2 COMPRESSIBLE GAS FLOW
Rev. 8/15 AD/GW ChE 253M Experiment No. 2 COMPRESSIBLE GAS FLOW The objective of this experiment is to familiarize the student with methods for measurement of compressible gas flow and to study gas flow under subsonic and supersonic flow conditions. The experiment is divided into three distinct parts: (1) Calibration and determination of the critical pressure ratio for a critical flow nozzle under supersonic flow conditions (2) Calculation of the discharge coefficient and Reynolds number for an orifice under subsonic (non- choked) flow conditions and (3) Determination of the orifice constants and mass discharge from a pressurized tank in a dynamic bleed down experiment under (choked) flow conditions. The experimental set up consists of a 100 psig air source branched into two manifolds: the first used for parts (1) and (2) and the second for part (3). The first manifold contains a critical flow nozzle, a NIST-calibrated in-line digital mass flow meter, and an orifice meter, all connected in series with copper piping. The second manifold contains a strain-gauge pressure transducer and a stainless steel tank, which can be pressurized and subsequently bled via a number of attached orifices. A number of NIST-calibrated digital hand held manometers are also used for measuring pressure in all 3 parts of this experiment. Assorted pressure regulators, manual valves, and pressure gauges are present on both manifolds and you are expected to familiarize yourself with the process flow, and know how to operate them to carry out the experiment. A process flow diagram plus handouts outlining the theory of operation of these devices are attached. -
In Physical Chemistry
INTERNATIONAL UNION OF PURE AND APPLIED CHEMISTRY Physical and Biophysical Chemistry Division IUPAC Vc^llclllul LICb . U 111 Lb cillCl Oy 111 DOlo in Physical Chemistry Third Edition Prepared for publication by E. Richard Cohen Tomislav Cvitas Jeremy G. Frey BcTt.il Holmstrom Kozo Kuchitsu R,oberto Marquardt Ian Mills Franco Pavese Martin Quack Jiirgen Stohner Herbert L. Strauss Michio Takanii Anders J Thor The first and second editions were prepared for publication by Ian Mills Tomislav Cvitas Klaus Homann Nikola Kallay Kozo Kuchitsu IUPAC 2007 RSC Publishing CONTENTS v PREFACE ix HISTORICAL INTRODUCTION xi 1 PHYSICAL QUANTITIES AND UNITS 1 1.1 Physical quantities and quantity calculus 3 1.2 Base quantities and derived quantities 4 1.3 Symbols for physical quantities and units 5 1.3.1 General rules for symbols for quantities 5 1.3.2 General rules for symbols for units 5 1.4 Use of the words "extensive", "intensive", "specific", and "molar" 6 1.5 Products and quotients of physical quantities and units 7 1.6 The use of italic and Roman fonts for symbols in scientific publications 7 2 TABLES OF PHYSICAL QUANTITIES 11 2.1 Space and time 13 2.2 Classical mechanics 14 2.3 Electricity and magnetism 16 2.4 Quantum mechanics and quantum chemistry 18 2.4.1 Ab initio Hartree-Fock self-consistent field theory (ab initio SCF) 20 2.4.2 Hartree-Fock-Roothaan SCF theory, using molecular orbitals expanded as linear combinations of atomic-orbital basis . functions (LCAO-MO theory) . 21 2.5 Atoms and molecules 22 2.6 Spectroscopy 25 2.6.1 Symbols for angular -
Aspects of Flow for Current, Flow Rate Is Directly Proportional to Potential
Vacuum technology Aspects of flow For current, flow rate is directly proportional to potential difference and inversely proportional to resistance. I = V/R or I = V/R For a fluid flow, Q = (P1-P2)/R or P/R Using reciprocal of resistance, called conductance, we have, Q = C (P1-P2) There are two kinds of flow, volumetric flow and mass flow Volume flow rate, S = vA v – the average bulk velocity, A the cross sectional area S = V/t, V is the volume and t is the time. Mass flow rate is S x density. G = vA or V/t Mass flow rate is measured in units of throughput, such as torr.L/s Throughput = volume flow rate x pressure Throughput is equivalent to power. Torr.L/s (g/cm2)cm3/s g.cm/s J/s W It works out that, 1W = 7.5 torr.L/s Types of low 1. Laminar: Occurs when the ratio of mass flow to viscosity (Reynolds number) is low for a given diameter. This happens when Reynolds number is approximately below 2000. Q ~ P12-P22 2. Above 3000, flow becomes turbulent Q ~ (P12-P22)0.5 3. Choked flow occurs when there is a flow restriction between two pressure regions. Assume an orifice and the pressure difference between the two sections, such as 2:1. Assume that the pressure in the inlet chamber is constant. The flow relation is, Q ~ P1 4. Molecular flow: When pressure reduces, MFP becomes larger than the dimensions of the duct, collisions occur between the walls of the vessel. -
An Independent Assessment of the Sinking of the MV DERBYSHIRE
SNAME Transactions, Vol. 106, 1998, pp. 59-103 An Independent Assessment of the Sinking of the MV DERBYSHIRE Douglas Faulkner, Fellow, Emeritus Professor of Naval Architecture, University of Glasgow, Scotland The author was appointed by the UK Department of Tranq~ort as a fellow Assessor with R.A. Williams during Lord Donaldson's Assessment (1995) of the loss of the OBO ship DERBYSHIRE and throughout the planning and conduct of the two final surveys of the wreck. This paper is drawn from the independ- ent report (b~udknel; 1998a) and may be considered complementary to those of the UK and EC Asses- sors (Williams and Torchio, 1998a and 1998b). The paper deals with the history and loss of the ship, in- cluding the concept developed in 1995 of 13 possible loss scenarios in a Jormal safety Risk Matrix" of probability and seriousness. It analyses abnormal wave effects on hatch cover collapse, on ship bending, and on flooding of bow spaces and no. 1 hold. The implosion-explosion mechanics during sinking is out- lined to explain the devastation of the wreck. The 1996 and 1997 underwater surveys are outlined as are the findings of.fact. Each of the final 14 loss scenarios is analysed in the light of the firm and circum- stantial survey evidence, plus many other factotw of service experience, analyses and experiments. The updated Risk Matrix speaks for itself and leads to the prime conclusions and major recommendations. Nomenclature ~ Register, 1987) which also depicts the oil fuel, fresh water and minimal ballast water distribution. Her estimated displacement as she approached Japan was about A = 194,000 te and hence 1. -
Mass Flow Rate and Isolation Characteristics of Injectors for Use with Self-Pressurizing Oxidizers in Hybrid Rockets
49th AIAA/ASME/SAE/ASEE Joint PropulsionConference AIAA 2013-3636 July 14 - 17, 2013, San Jose, CA Mass Flow Rate and Isolation Characteristics of Injectors for Use with Self-Pressurizing Oxidizers in Hybrid Rockets Benjamin S. Waxman*, Jonah E. Zimmerman†, Brian J. Cantwell‡ Stanford University, Stanford, CA 94305 and Gregory G. Zilliac§ NASA Ames Research Center, Moffet Field, CA 94035 Self-pressurizing rocket propellants are currently gaining popularity in the propulsion community, partic- ularly in hybrid rocket applications. Due to their high vapor pressure, these propellants can be driven out of a storage tank without the need for complicated pressurization systems or turbopumps, greatly minimizing the overall system complexity and mass. Nitrous oxide (N2O) is the most commonly used self pressurizing oxidizer in hybrid rockets because it has a vapor pressure of approximately 730 psi (5.03 MPa) at room temperature and is highly storable. However, it can be difficult to model the feed system with these propellants due to the presence of two-phase flow, especially in the injector. An experimental test apparatus was developed in order to study the performance of nitrous oxide injectors over a wide range of operating conditions. Mass flow rate characterization has been performed to determine the effects of injector geometry and propellant sub-cooling (pressurization). It has been shown that rounded and chamfered inlets provide nearly identical mass flow rate improvement in comparison to square edged orifices. A particular emphasis has been placed on identifying the critical flow regime, where the flow rate is independent of backpressure (similar to choking). For a simple orifice style injector, it has been demonstrated that critical flow occurs when the downstream pressure falls sufficiently below the vapor pressure, ensuring bulk vapor formation within the injector element. -
Homework 1: Exercise 1 Metric - English Conversion [Based on the Chauffe & Jefferies (2007)]
MAR 110 HW 1: Exercise 1 – Conversions p. 1 Homework 1: Exercise 1 Metric - English Conversion [based on the Chauffe & Jefferies (2007)] 1-1. THE METRIC SYSTEM The French developed the metric system during the 1790s. Unlike the "English" system, in which the difference between smaller and larger units is irregular and has no scientific foundation, the metric system is based on multiples of 10. Smaller and larger units can be obtained simply by moving the decimal point - that is multiplying or dividing by 10. For example, in the "English" system there are 12 inches to a foot (ft), but 3 ft to a yard, and 1760 yards in a mile. By contrast, in the metric system there are 10 m to a decameter (dm), 10 dm to a hectometer (hm), and 10 hm to a kilometer (km). The convenience and regularity of the metric system make it the standard system used in scientific research The basic units of the metric system are the meter for length, gram for mass (weight), liter for volume, and degree Celsius (OC) for temperature. These terms have been defined in terms of practical considerations. For example, one meter is equal to one ten millionth of the distance between the North Pole and the Equator. The gram is the mass of one cubic centimeter (or one millionth of a cubic meter) of water at a temperature of 4°C. The liter is the volume of a cubic decimeter (or one thousandth of a cubic meter). A degree Celsius is one-hundredth of the change in temperature between the freezing and boiling points of water. -
Yiddish and Relation to the German Dialects Bryan Witmore University of South Carolina
University of South Carolina Scholar Commons Theses and Dissertations 6-30-2016 Yiddish and Relation To The German Dialects Bryan Witmore University of South Carolina Follow this and additional works at: https://scholarcommons.sc.edu/etd Part of the German Language and Literature Commons Recommended Citation Witmore, B.(2016). Yiddish and Relation To The German Dialects. (Master's thesis). Retrieved from https://scholarcommons.sc.edu/ etd/3522 This Open Access Thesis is brought to you by Scholar Commons. It has been accepted for inclusion in Theses and Dissertations by an authorized administrator of Scholar Commons. For more information, please contact [email protected]. YIDDISH AND ITS RELATION TO THE GERMAN DIALECTS by Bryan Witmore Bachelor of Arts University of South Carolina, 2006 Submitted in Partial Fulfillment of the Requirements For the Degree of Master of Arts in German College of Arts and Sciences University of South Carolina 2016 Accepted by: Kurt Goblirsch, Director of Thesis Lara Ducate, Reader Lacy Ford, Senior Vice Provost and Dean of Graduate Studies © Copyright by Bryan Witmore, 2016 All Rights Reserved. ii ACKNOWLEDGEMENTS This thesis project was made possible in large part by the German program at the University of South Carolina. The technical assistance that propelled this project was contributed by the staff at the Ted Mimms Foreign Language Learning Center. My family was decisive in keeping me physically functional and emotionally buoyant through the writing process. Many thanks to you all. iii ABSTRACT In an attempt to balance the complex, multi-component nature of Yiddish with its more homogenous speech community – Ashekenazic Jews –Yiddishists have proposed definitions for the Yiddish language that cannot be considered linguistic in nature. -
Physics 101: Lecture 18 Fluids II
PhysicsPhysics 101:101: LectureLecture 1818 FluidsFluids IIII Today’s lecture will cover Textbook Chapter 9 Physics 101: Lecture 18, Pg 1 ReviewReview StaticStatic FluidsFluids Pressure is force exerted by molecules “bouncing” off container P = F/A Gravity affects pressure P = P 0 + ρgd Archimedes’ principle: Buoyant force is “weight” of displaced fluid. F = ρ g V Today include moving fluids! A1v1 = A 2 v2 – continuity equation 2 2 P1+ρgy 1 + ½ ρv1 = P 2+ρgy 2 + ½ρv2 – Bernoulli’s equation Physics 101: Lecture 18, Pg 2 08 ArchimedesArchimedes ’’ PrinciplePrinciple Buoyant Force (F B) weight of fluid displaced FB = ρfluid Vdisplaced g Fg = mg = ρobject Vobject g object sinks if ρobject > ρfluid object floats if ρobject < ρfluid If object floats… FB = F g Therefore: ρfluid g Vdispl. = ρobject g Vobject Therefore: Vdispl./ Vobject = ρobject / ρfluid Physics 101: Lecture 18, Pg 3 10 PreflightPreflight 11 Suppose you float a large ice-cube in a glass of water, and that after you place the ice in the glass the level of the water is at the very brim. When the ice melts, the level of the water in the glass will: 1. Go up, causing the water to spill out of the glass. 2. Go down. 3. Stay the same. Physics 101: Lecture 18, Pg 4 12 PreflightPreflight 22 Which weighs more: 1. A large bathtub filled to the brim with water. 2. A large bathtub filled to the brim with water with a battle-ship floating in it. 3. They will weigh the same. Tub of water + ship Tub of water Overflowed water Physics 101: Lecture 18, Pg 5 15 ContinuityContinuity A four-lane highway merges down to a two-lane highway. -
THERMODYNAMICS, HEAT TRANSFER, and FLUID FLOW, Module 3 Fluid Flow Blank Fluid Flow TABLE of CONTENTS
Department of Energy Fundamentals Handbook THERMODYNAMICS, HEAT TRANSFER, AND FLUID FLOW, Module 3 Fluid Flow blank Fluid Flow TABLE OF CONTENTS TABLE OF CONTENTS LIST OF FIGURES .................................................. iv LIST OF TABLES ................................................... v REFERENCES ..................................................... vi OBJECTIVES ..................................................... vii CONTINUITY EQUATION ............................................ 1 Introduction .................................................. 1 Properties of Fluids ............................................. 2 Buoyancy .................................................... 2 Compressibility ................................................ 3 Relationship Between Depth and Pressure ............................. 3 Pascal’s Law .................................................. 7 Control Volume ............................................... 8 Volumetric Flow Rate ........................................... 9 Mass Flow Rate ............................................... 9 Conservation of Mass ........................................... 10 Steady-State Flow ............................................. 10 Continuity Equation ............................................ 11 Summary ................................................... 16 LAMINAR AND TURBULENT FLOW ................................... 17 Flow Regimes ................................................ 17 Laminar Flow ............................................... -
Vowel Change in English and German: a Comparative Analysis
Vowel change in English and German: a comparative analysis Miriam Calvo Fernández Degree in English Studies Academic Year: 2017/2018 Supervisor: Reinhard Bruno Stempel Department of English and German Philology and Translation Abstract English and German descend from the same parent language: West-Germanic, from which other languages, such as Dutch, Afrikaans, Flemish, or Frisian come as well. These would, therefore, be called “sister” languages, since they share a number of features in syntax, morphology or phonology, among others. The history of English and German as sister languages dates back to the Late antiquity, when they were dialects of a Proto-West-Germanic language. After their split, more than 1,400 years ago, they developed their own language systems, which were almost identical at their earlier stages. However, this is not the case anymore, as can be seen in their current vowel systems: the German vowel system is composed of 23 monophthongs and 8 diphthongs, while that of English has only 12 monophthongs and 8 diphthongs. The present paper analyses how the English and German vowels have gradually changed over time in an attempt to understand the differences and similarities found in their current vowel systems. In order to do so, I explain in detail the previous stages through which both English and German went, giving special attention to the vowel changes from a phonological perspective. Not only do I describe such processes, but I also contrast the paths both languages took, which is key to understand all the differences and similarities present in modern English and German. The analysis shows that one of the main reasons for the differences between modern German and English is to be found in all the languages English has come into contact with in the course of its history, which have exerted a significant influence on its vowel system, making it simpler than that of German. -
A Middle High German Primer, with Grammar, Notes, and Glossary
> 1053 MIDDLE HIGH GERMAN PRIMER WITH GRAMMAR, NOTES, AND GLOSSARY BY JOSEPH WRIGHT M.A., PH.D., D.C.L., LL.D., L1TT.D. FELLOW OF THE BRITISH ACADEMY CORPUS CHRISTI PROFESSOR OF COMPARATIVE PHILOLOGY IN THE UNIVERSITY OF OXFORD THIRD EDITION RE-WRITTEN AND ENLARGED AT THE CLARENDON PRESS 1917 OXFORD UNIVERSITY PRESS LONDON EDINBURGH GLASGOW NEW YORK TORONTO MELBOURNE BOMBAY HUMPHREY MILFORD PUBLISHER TO THE UNIVERSITY pr EXTRACTS FROM THE PREFACES TO THE FIRST AND SECOND EDITIONS THE present book has been written in the hope that it will serve as an elementary introduction to the larger German works on the subject from which I have appro- priated whatever seemed necessary for the purpose. In the grammar much aid has been derived from Paul's Mittelhochdeutsche Grammatik, second edition, Halle, 1884, and Weinhold's Mittelhochdeutsche Grammatik, second edition, Paderborn, 1883. The former work, besides con- taining by far the most complete syntax, is also the only Middle High German Grammar which is based on the present state of German Philology. ... I believe that the day is not far distant when English students will take a much more lively interest in the study of their own and the other Germanic languages (especially German and Old Norse) than has hitherto been the case. And if this little book should contribute anything towards furthering the cause, it will have amply fulfilled its purpose. LONDON : January, 1888. WHEN I wrote the preface to the first edition of this primer in 1888, I ventured to predict that the interest of English students in the subject would grow and develop as time went on, but I hardly expected that it would grow so much that a second edition of the book would be required within iv Preface to the Second Edition so short a period. -
Online Companion to a Historical Phonology of English
A Historical Phonology of English Donka Minkova © Donka Minkova, 2014 Edinburgh University Press Ltd 22 George Square, Edinburgh EH8 9LF www.euppublishing.com Typeset in 10.5/12 Janson by Servis Filmsetting Ltd, Stockport, Cheshire, printed and bound in Great Britain by CPI Group (UK) Ltd, Croydon CR0 4YY A CIP record for this book is available from the British Library ISBN 978 0 7486 3467 5 (hardback) ISBN 978 0 7486 3468 2 (paperback) ISBN 978 0 7486 3469 9 (webready PDF) ISBN 978 0 7486 7755 9 (epub) The right of Donka Minkova to be identifi ed as author of this work has been asserted in accordance with the Copyright, Designs and Patents Act 1988. Contents Acknowledgements x List of abbreviations and symbols xii A note on the Companion to A Historical Phonology of English xv 1 Periods in the history of English 1 1.1 Periods in the history of English 2 1.2 Old English (450–1066) 2 1.3 Middle English (1066–1476) 9 1.4 Early Modern English (1476–1776) 15 1.5 English after 1776 17 1.6 The evidence for early pronunciation 20 2 The sounds of English 24 2.1 The consonants of PDE 24 2.1.1 Voicing 26 2.1.2 Place of articulation 27 2.1.3 Manner of articulation 29 2.1.4 Short and long consonants 31 2.2 The vowels of PDE 32 2.2.1 Short and long vowels 35 2.2.2 Complexity: monophthongs and diphthongs 37 2.3 The syllable: some basics 39 2.3.1 Syllable structure 39 2.3.2 Syllabifi cation 40 2.3.3 Syllable weight 43 2.4 Notes on vowel representation 45 2.5 Phonological change: some types and causes 46 3 Discovering the earliest links: Indo- European