The Thixotropy and Dilatancy of a Marine Soil
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Regulatory Guide 3.39 Standard Format & Content of License
NUREG-O010 USNRC REGULATORY J GUIDE SERIES REGULATORY GUIDE 3.39 STANDARD FORMAT AND CONTENT OF LICENSE APPLICATIONS FOR PLUTONIUM PROCESSING 2 AND FUEL FABRICATION PLANTS JANUARY 1976 UNITED STATES NUCLEAR REGULATORY COMMISSION Available from National Technical Information Service Springfield, Virginia 22161 Price: Printed Copy $5.50 ; Microfiche $2.25 U.S. NUCLEAR REGULATORY COMMISSION January 1976 REGULATORY GUIDE OFFICE OF STANDARDS DEVELOPMENT REGULATORY GUIDE 3.39 1 STANDARD FORMAT AND C KEN\ OF LICENSE APPLIC 0O1 .R PLUTONIUM PROCf$ L4('I AND FUEL FABRjATI XP lTS USNRC REGULATORY GUIDES Comments should be sent to the Secretary of the Commission. U.S. Nuclear Regulatory Guides are Issued to describe and make available to the public Regulatory Commission. Washington. D.C. 20555. Attention Docketing and methods ecceptable to the NRC staff of implementing specific parts of the Service Section Commission's regulations, to delineate techniques used by the staff in evelu eting specific problems or postulated accidents. or to provide guidance to appli The guides are issued In the following ten broed divisions cants Regulatory Guides are not substitutes for regulations. and compliance 1 wer Reactors 6. Products with them Is not required. Methods end solutions different from those set 2. out in Research and Test Reactors 7. Transponation the guides will be acceptable if they provide a basis for the findings requisite to 3. Fuels and Materiels Facilities I Occupational Health the issuance or continuance of apermit or license by the Commission 4. Evironmental andSiting 9.Antitrust Review Comments and suggestions for Improvements in these guides are encouraged 5. Materials and Plant Protection 10. -
Shear Thickening in Concentrated Suspensions: Phenomenology
Shear thickening in concentrated suspensions: phenomenology, mechanisms, and relations to jamming Eric Brown School of Natural Sciences, University of California, Merced, CA 95343 Heinrich M. Jaeger James Franck Institute, The University of Chicago, Chicago, IL 60637 (Dated: July 22, 2013) Shear thickening is a type of non-Newtonian behavior in which the stress required to shear a fluid increases faster than linearly with shear rate. Many concentrated suspensions of particles exhibit an especially dramatic version, known as Discontinuous Shear Thickening (DST), in which the stress suddenly jumps with increasing shear rate and produces solid-like behavior. The best known example of such counter-intuitive response to applied stresses occurs in mixtures of cornstarch in water. Over the last several years, this shear-induced solid-like behavior together with a variety of other unusual fluid phenomena has generated considerable interest in the physics of densely packed suspensions. In this review, we discuss the common physical properties of systems exhibiting shear thickening, and different mechanisms and models proposed to describe it. We then suggest how these mechanisms may be related and generalized, and propose a general phase diagram for shear thickening systems. We also discuss how recent work has related the physics of shear thickening to that of granular materials and jammed systems. Since DST is described by models that require only simple generic interactions between particles, we outline the broader context of other concentrated many-particle systems such as foams and emulsions, and explain why DST is restricted to the parameter regime of hard-particle suspensions. Finally, we discuss some of the outstanding problems and emerging opportunities. -
World Reference Base for Soil Resources 2014 International Soil Classification System for Naming Soils and Creating Legends for Soil Maps
ISSN 0532-0488 WORLD SOIL RESOURCES REPORTS 106 World reference base for soil resources 2014 International soil classification system for naming soils and creating legends for soil maps Update 2015 Cover photographs (left to right): Ekranic Technosol – Austria (©Erika Michéli) Reductaquic Cryosol – Russia (©Maria Gerasimova) Ferralic Nitisol – Australia (©Ben Harms) Pellic Vertisol – Bulgaria (©Erika Michéli) Albic Podzol – Czech Republic (©Erika Michéli) Hypercalcic Kastanozem – Mexico (©Carlos Cruz Gaistardo) Stagnic Luvisol – South Africa (©Márta Fuchs) Copies of FAO publications can be requested from: SALES AND MARKETING GROUP Information Division Food and Agriculture Organization of the United Nations Viale delle Terme di Caracalla 00100 Rome, Italy E-mail: [email protected] Fax: (+39) 06 57053360 Web site: http://www.fao.org WORLD SOIL World reference base RESOURCES REPORTS for soil resources 2014 106 International soil classification system for naming soils and creating legends for soil maps Update 2015 FOOD AND AGRICULTURE ORGANIZATION OF THE UNITED NATIONS Rome, 2015 The designations employed and the presentation of material in this information product do not imply the expression of any opinion whatsoever on the part of the Food and Agriculture Organization of the United Nations (FAO) concerning the legal or development status of any country, territory, city or area or of its authorities, or concerning the delimitation of its frontiers or boundaries. The mention of specific companies or products of manufacturers, whether or not these have been patented, does not imply that these have been endorsed or recommended by FAO in preference to others of a similar nature that are not mentioned. The views expressed in this information product are those of the author(s) and do not necessarily reflect the views or policies of FAO. -
International Society for Soil Mechanics and Geotechnical Engineering
INTERNATIONAL SOCIETY FOR SOIL MECHANICS AND GEOTECHNICAL ENGINEERING This paper was downloaded from the Online Library of the International Society for Soil Mechanics and Geotechnical Engineering (ISSMGE). The library is available here: https://www.issmge.org/publications/online-library This is an open-access database that archives thousands of papers published under the Auspices of the ISSMGE and maintained by the Innovation and Development Committee of ISSMGE. 1/18 Liquefaction of Saturated Sandy Soils Liquéfaction de sols sableux saturés by V. A. F lorin , Professor, Doctor of Technical Sciences, Associate Member of the USSR Academy of Sciences, Institute of Mechanics of the USSR Academy of Sciences, and P. L. I vanov , Docent, Candidate of Technical Sciences, Leningrad Polytechnic Institute. Summary Sommaire The authors give results obtained from theoretical and Le présent rapport contient quelques résultats des études experimental research on the liquefaction of saturated sandy théoriques et expérimentales des phénomènes de liquéfaction soils undertaken by them, in the Laboratory of Soil Mechanics de sols sableux saturés qui ont été effectuées aux Laboratoires of the Institute of Mechanics of the U.S.S.R. Academy of Sciences de Mécanique des sols de l’institut de Mécanique de l’Académie and in the Leningrad Polytechnic Institute. des Sciences de l’U.R.S.S. et de l’institut Polytechnique de Laboratory investigations have been carried out on various Leningrad. kinds of disturbances affecting saturated sandy soils and causing Les auteurs décrivent des études de Laboratoire de la liqué their liquefaction. The authors also give the results of studies faction de sols sableux soumis à diverses influences. -
Permeability and Seepage -2
13 Prof. B V S Viswanadham, Department of Civil Engineering, IIT Bombay Permeability and Seepage -2 Prof. B V S Viswanadham, Department of Civil Engineering, IIT Bombay Conditions favourable for the formation quick sand Quick sand is not a type of sand but a flow condition occurring within a cohesion-less soil when its effective stress is reduced to zero due to upward flow of water. Quick sand occurs in nature when water is being forced upward under pressurized conditions. In this case, the pressure of the escaping water exceeds the weight of the soil and the sand grains are forced apart. The result is that the soil has no capability to support a load. Why does quick condition or boiling occurs mostly in fine sands or silts? Prof. B V S Viswanadham, Department of Civil Engineering, IIT Bombay Some practical examples of quick conditions Excavations in granular materials behind cofferdams alongside rivers Any place where artesian pressures exist (i.e. where head of water is greater than the usual static water pressure). -- When a pervious underground structure is continuous and connected to a place where head is higher. Behind river embankments to protect floods Prof. B V S Viswanadham, Department of Civil Engineering, IIT Bombay Some practical examples of quick conditions Contrary to popular belief, it is not possible to drown in quick sand, because the density of quick sand is much greater than that of water. ρquicksand >> ρwater Consequently, it is literally impossible for a person to be sucked into quicksand and disappear. So, a person walking into quicksand would sink to about waist depth and then float. -
Nature and Effects of Earthquake Hazards A
Session 7: Nature and Effects of Earthquake Hazards Session No. 7 Course Title: Earthquake Hazard and Emergency Management Session Title: Nature and Effects of Earthquake Hazards Author: James R. Martin, II Time: 120 minutes ______________________________________________________________________________ Objectives: 7.1. Describe the nature of earthquake hazards, and especially, how these hazards differ from other hazards. 7.2. Describe the effects of earthquakes upon infrastructure (buildings, lifelines, etc.). 7.3. What are the general effects of earthquakes upon people and what is the nature of the casualties from earthquakes? 7.4. Describe the general effects of earthquakes upon the economy and the nature of earthquake losses. Scope: In this session, the students will learn about the general nature of earthquake hazards, specifically how earthquake hazards differ from other natural hazards, and the special challenges they pose. This section addresses a variety of effects of earthquakes and specifically the factors that produce damage and losses. The session covers the effects on people, the economy, and infrastructure. This section is closely linked with Section 9 in which mitigation will be discussed. This section is important because it provides a better understanding of earthquake hazards, and fosters improved communication with scientists, engineers, policy makers, the public, etc. ______________________________________________________________________________ Readings: Suggested student reading: Commission on Engineering and Technical Systems. 1990. “The Economic Consequences of a Catastrophic Earthquake,” Proceedings of a Forum, August 1 and 2, 1990, Overview of Economic Research on Earthquake Consequences, National Academies Press. Earthquake Hazard and Emergency Management 7-1 Session 7: Nature and Effects of Earthquake Hazards http://books.nap.edu/catalog/2027.html. -
Impact of Thixotropy on Flow Patterns Induced in a Stirred Tank
CORE Metadata, citation and similar papers at core.ac.uk Provided by Open Archive Toulouse Archive Ouverte Impact of thixotropy on flow patterns induced in a stirred tank: Numerical and experimental studies G. Couerbe a, D.F. Fletcher b, C. Xuereb a, M. Poux a,∗ a Universit e´ de Toulouse, Laboratoire de G enie´ Chimique, CNRS/INP/UPS, 5 rue Paulin Talabot, BP 1301, 31106 Toulouse Cedex, France b School of Chemical and Biomolecular Engineering, The University of Sydney, NSW 2006, Australia abstract Agitation of a thixotropic shear•thinning fluid exhibiting a yield stress is investigated both experimentally and via simulations. Steady•state experiments are conducted at three 1 impeller rotation rates (1, 2 and 8 s − ) for a tank stirred with an axial•impeller and flow•field measurements are made using particle image velocimetry (PIV) measurements. Three• dimensional numerical simulations are also performed using the commercial CFD code Keywords: ANSYS CFX10.0. The viscosity of the suspension is determined experimentally and is mod• Thixotropy elled using two shear•dependant laws, one of which takes into account the flow instabilities CFD of such fluids at low shear rates. At the highest impeller speed, the flow exhibits the famil• PIV iar outward pumping action associated with axial•flow impellers. However, as the impeller Stirred tank speed decreases, a cavern is formed around the impeller, the flow generated in the vicin• Impeller ity of the agitator reorganizes and its pumping capacity vanishes. An unusual flow pattern, Mixing where the radial velocity dominates, is observed experimentally at the lowest stirring speed. It is found to result from wall slip effects. -
Rheology in Pharmaceutical Formulations-A Perspective
evelo f D pin l o g a D Mastropietro et al., J Develop Drugs 2013, 2:2 n r r u u g o s J Journal of Developing Drugs DOI: 10.4172/2329-6631.1000108 ISSN: 2329-6631 Review Article Open Access Rheology in Pharmaceutical Formulations-A Perspective David J Mastropietro1, Rashel Nimroozi2 and Hossein Omidian1* 1Department of Pharmaceutical Sciences, College of Pharmacy, Nova Southeastern University, Fort Lauderdale, Florida, USA 2Westside Regional Medical Center, Pharmacy Department, Plantation, Florida, USA Abstract Medications produced as semi-solids type product such as creams, ointments and lotions are based on emulsion or suspension type systems consisting of two or more incompatible materials. In order to be manufactured, these dosage forms need specific flow properties so they can be placed into a container, remain stable over time, dispensed, handled and properly applied to the affected area by patients. Rheology is therefore crucially important as it will directly affect the way a drug is formulated and developed, the quality of the raw and finished product, the drug efficacy, the way a patient adheres to the prescribed drug, and the overall healthcare cost. It can be concluded that there are inherent and independent factors that affect the flow property of a medicated material during every stage of its manufacturing all the way to its use. Keywords: Pharmaceutical formulation; Rheology; Viscosity; dampened as the particles easily slide over one another to maintain a Suspensions; Rheology modifiers; Hydrophilic polymers steady viscosity, or Newtonian behavior. If stress is applied at a faster rate, the spherical particles slide faster over each other to maintain Introduction their history of viscosity. -
Thixotropy Vs Wall Slip in Suspensions
Thixotropy vs wall slip in suspensions Wonjae Choi Papers : Dullaert, Mewis : Thixotropy : Build-up and breakdown curves during flow ( JoR, 2005 ) Claimed the first robust stress measurement of the thixotropic system Introduced de-embedding of rheometer’s transfer function from the output data Dullaert, Mewis : A model system for thixotropy studies ( Rheol Acta, 2005 ) Detailed description on the previous ‘robust thixotropic system’ Covered various issues which was problematic for previous researches and was reduced with their new compound Covered wall-slip phenomenon and remedy for it Experiments about thixotropy Difficulties in experiments While there are various models & theories about thixotropy, there are few reliable experimental datasets Primary reason for this is the difficulties involved in measuring thixotropic system with enough accuracy Main objective of this paper Building robust thixotropic system which supports repeatible & reliable measurements Recall : Definition of thixotropy in this paper Change of floc structure resulting in varying viscosity Does not necessarily include viselasticity Why is measurement difficult? Implemental artifacts Wall slip Heterogeneous shear rates Gap size effect Rheometer’s transfer function Memory of floc’s microstructure Evaporation of solvents Particle sedimentation, change in particle’s wetting property, adsorption Plan Wall slip Interparticle attraction & PIB Viscosity control Sedimentation Memory Steady-state Enough pre-treatment Evaporation Non volatile suspension -
Pharmaceutics I صيدالنيات 1
Pharmaceutics I صيدﻻنيات 1 Unit 6 1 Rheology of suspensions • Rheology, the study of flow, addresses the viscosity characteristics of powders, fluids, and semisolids. • Materials are divided into two general categories, Newtonian and non-Newtonian, depending on their flow characteristics. • The unit of viscosity is the poise, the shearing force required to produce a velocity of 1 cm per second between two parallel planes of liquid, each 1 cm2 in area and separated by a distance of 1 cm. • The most convenient unit to use is the centipoise, or cP (equivalent to 0.01 poise). Newton’s law of flow • Newton law of flow relates parallel layers of liquid, with the bottom layer fixed, when a force is placed on the top layer, the top plane moves at constant velocity, each lower layer moves with a velocity directly proportional to its distance from the stationary bottom layer. • The velocity gradient, or rate of shear (dv/dr), is the difference of velocity dv between two planes of liquid separated by the distance dr. • The force (F´/A) applied to the top layer that is required to result in flow (rate of shear, G) is called the shearing stress (F). NEWTONIAN’S LOW OF FLOW Let us consider a block of liquid consisting of parallel plates of molecules as shown in the figure. The bottom layer is considered to be fixed in place. If the top plane of liquid is moved at constant velocity, each lower layer will move with a velocity directly proportional to its distance from the stationary bottom layer Representation of shearing force acting on a block of material ☻Rate of Shear dv/dr = G Is the velocity difference dv between two planes of liquid separated by an infinite distance dr. -
State Highway Department Extension Service And
Public Access Copy DO NOT REMOVE STATE OF DELAWARE from room 208. DELAWARE GEOLOGICAL SURVEY Bulletin No. 1 GROUNDWATER PROBLEMS IN HIGHWAY CONSTRUCTION AND MAINTENANCE WILLIAM C. RASMUSSEN Geologirt United States Geological Swey and LEON B. HAIGLER Hydraulic Engineer United States Geological Smey PREPARED BY THE UN~TEDSTATES GEOLOGICAL SURVEY IN COOPEMTION WITH THE DELAWARESTATE HIGHWAYDEPARTMENT AGRICULTURALEXTENSION SERVICE AND EXPERIMENTSTATION AND THE DELAWAREGEOLOGICAL SURVEY Published for !be DELAWARE GEOLOGICAL SURVEY Newark, 1953 STATE OF DELAWARE Contents DELAWARE GEOLOGICAL SURVEY Bulletin No. 1 Introduction ................................................. 4 Purpose and scope ......................................... 4 GROUND-WATER PROBLEMS IN HIGHWAY 4 CONSTRUCTION AND MAINTENANCE the State ............................................... 5 Cooperation and acknowIedgments ............................ 6 7 WILLIAM C. RASMUSSEN Road subdrainage 7 Geologist Quicksand ............................................. 8 United States Geological Survey and LEON B. HAIGLER Hydraulic Engineer United States Geological Survey PREPARED BY THE Figure 1. Map of the State of Delaware, showing the physiographic provinces and the localities discussed ................... 18 UNITEDSTATES GEOLOGICAL SURVEY 2. Map of subdrainage robIem, roadway near Portsville, IN COOPERATION WITH THE between Laurel an 1Bethel, Sussex County, Del. .......... 19 DELAWARESTATE HIGHWAY DEPARTMENT 3. Cross sections showing high water table beneath road shown in figure -
Dilatancy in the Flow and Fracture of Stretched Colloidal Suspensions
Dilatancy in the flow and fracture of stretched colloidal suspensions M.I. Smith School of Engineering, University of Edinburgh, Kings Buildings, Mayfield Rd, Edinburgh, EH9 3JL, UK School of Physics and Astronomy, University of Nottingham, University Park, Nottingham, NG7 2RD e-mail: [email protected] R. Besseling SUPA, School of Physics and Astronomy, University of Edinburgh, Kings Buildings, Mayfield Rd, Edinburgh EH9 3JZ e-mail: [email protected] M.E. Cates SUPA, School of Physics and Astronomy, University of Edinburgh, Kings Buildings, Mayfield Rd, Edinburgh, EH9 3JZ, UK e-mail: m.e.cates@ ed.ac.uk V. Bertola* School of Engineering, University of Edinburgh, Kings Buildings, Mayfield Rd, Edinburgh, EH9 3JL, UK e-mail: [email protected] contacting author* 1 Dilatancy in the flow and fracture of stretched colloidal suspensions. Concentrated particulate suspensions, commonplace in the pharmaceutical, cosmetic and food industries, display intriguing rheology. In particular, the dramatic increase in viscosity with strain rate (shear thickening and jamming) which is often observed at high volume fractions, is of strong practical and fundamental importance. Yet manufacture of these products and their subsequent dispensing often involves flow geometries substantially different from that of simple shear flow experiments. Here we show that the elongation and breakage of a filament of a colloidal fluid under tensile loading is closely related to the jamming transition seen in its shear rheology. However, the modified flow geometry reveals important additional effects. Using a model system with nearly hard-core interactions, we provide evidence of surprisingly strong viscoelasticity in such a colloidal fluid under tension.