WIKA Handbook Pressure & Temperature
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11 Fluid Statics
CHAPTER 11 | FLUID STATICS 357 11 FLUID STATICS Figure 11.1 The fluid essential to all life has a beauty of its own. It also helps support the weight of this swimmer. (credit: Terren, Wikimedia Commons) Learning Objectives 11.1. What Is a Fluid? • State the common phases of matter. • Explain the physical characteristics of solids, liquids, and gases. • Describe the arrangement of atoms in solids, liquids, and gases. 11.2. Density • Define density. • Calculate the mass of a reservoir from its density. • Compare and contrast the densities of various substances. 11.3. Pressure • Define pressure. • Explain the relationship between pressure and force. • Calculate force given pressure and area. 11.4. Variation of Pressure with Depth in a Fluid • Define pressure in terms of weight. • Explain the variation of pressure with depth in a fluid. • Calculate density given pressure and altitude. 11.5. Pascal’s Principle • Define pressure. • State Pascal’s principle. • Understand applications of Pascal’s principle. • Derive relationships between forces in a hydraulic system. 11.6. Gauge Pressure, Absolute Pressure, and Pressure Measurement • Define gauge pressure and absolute pressure. • Understand the working of aneroid and open-tube barometers. 11.7. Archimedes’ Principle • Define buoyant force. • State Archimedes’ principle. • Understand why objects float or sink. • Understand the relationship between density and Archimedes’ principle. 11.8. Cohesion and Adhesion in Liquids: Surface Tension and Capillary Action • Understand cohesive and adhesive forces. • Define surface tension. • Understand capillary action. 11.9. Pressures in the Body • Explain the concept of pressure the in human body. • Explain systolic and diastolic blood pressures. • Describe pressures in the eye, lungs, spinal column, bladder, and skeletal system. -
Chapter 3. Second and Third Law of Thermodynamics
Chapter 3. Second and third law of thermodynamics Important Concepts Review Entropy; Gibbs Free Energy • Entropy (S) – definitions Law of Corresponding States (ch 1 notes) • Entropy changes in reversible and Reduced pressure, temperatures, volumes irreversible processes • Entropy of mixing of ideal gases • 2nd law of thermodynamics • 3rd law of thermodynamics Math • Free energy Numerical integration by computer • Maxwell relations (Trapezoidal integration • Dependence of free energy on P, V, T https://en.wikipedia.org/wiki/Trapezoidal_rule) • Thermodynamic functions of mixtures Properties of partial differential equations • Partial molar quantities and chemical Rules for inequalities potential Major Concept Review • Adiabats vs. isotherms p1V1 p2V2 • Sign convention for work and heat w done on c=C /R vm system, q supplied to system : + p1V1 p2V2 =Cp/CV w done by system, q removed from system : c c V1T1 V2T2 - • Joule-Thomson expansion (DH=0); • State variables depend on final & initial state; not Joule-Thomson coefficient, inversion path. temperature • Reversible change occurs in series of equilibrium V states T TT V P p • Adiabatic q = 0; Isothermal DT = 0 H CP • Equations of state for enthalpy, H and internal • Formation reaction; enthalpies of energy, U reaction, Hess’s Law; other changes D rxn H iD f Hi i T D rxn H Drxn Href DrxnCpdT Tref • Calorimetry Spontaneous and Nonspontaneous Changes First Law: when one form of energy is converted to another, the total energy in universe is conserved. • Does not give any other restriction on a process • But many processes have a natural direction Examples • gas expands into a vacuum; not the reverse • can burn paper; can't unburn paper • heat never flows spontaneously from cold to hot These changes are called nonspontaneous changes. -
Pressure, Its Units of Measure and Pressure References
_______________ White Paper Pressure, Its Units of Measure and Pressure References Viatran Phone: 1‐716‐629‐3800 3829 Forest Parkway Fax: 1‐716‐693‐9162 Suite 500 [email protected] Wheatfield, NY 14120 www.viatran.com This technical note is a summary reference on the nature of pressure, some common units of measure and pressure references. Read this and you won’t have to wait for the movie! PRESSURE Gas and liquid molecules are in constant, random motion called “Brownian” motion. The average speed of these molecules increases with increasing temperature. When a gas or liquid molecule collides with a surface, momentum is imparted into the surface. If the molecule is heavy or moving fast, more momentum is imparted. All of the collisions that occur over a given area combine to result in a force. The force per unit area defines the pressure of the gas or liquid. If we add more gas or liquid to a constant volume, then the number of collisions must increase, and therefore pressure must increase. If the gas inside the chamber is heated, the gas molecules will speed up, impact with more momentum and pressure increases. Pressure and temperature therefore are related (see table at right). The lowest pressure possible in nature occurs when there are no molecules at all. At this point, no collisions exist. This condition is known as a pure vacuum, or the absence of all matter. It is also possible to cool a liquid or gas until all molecular motion ceases. This extremely cold temperature is called “absolute zero”, which is -459.4° F. -
Pressure Measuring Instruments
testo-312-2-3-4-P01 21.08.2012 08:49 Seite 1 We measure it. Pressure measuring instruments For gas and water installers testo 312-2 HPA testo 312-3 testo 312-4 BAR °C www.testo.com testo-312-2-3-4-P02 23.11.2011 14:37 Seite 2 testo 312-2 / testo 312-3 We measure it. Pressure meters for gas and water fitters Use the testo 312-2 fine pressure measuring instrument to testo 312-2 check flue gas draught, differential pressure in the combustion chamber compared with ambient pressure testo 312-2, fine pressure measuring or gas flow pressure with high instrument up to 40/200 hPa, DVGW approval, incl. alarm display, battery and resolution. Fine pressures with a resolution of 0.01 hPa can calibration protocol be measured in the range from 0 to 40 hPa. Part no. 0632 0313 DVGW approval according to TRGI for pressure settings and pressure tests on a gas boiler. • Switchable precision range with a high resolution • Alarm display when user-defined limit values are • Compensation of measurement fluctuations caused by exceeded temperature • Clear display with time The versatile pressure measuring instrument testo 312-3 testo 312-3 supports load and gas-rightness tests on gas and water pipelines up to 6000 hPa (6 bar) quickly and reliably. testo 312-3 versatile pressure meter up to Everything you need to inspect gas and water pipe 300/600 hPa, DVGW approval, incl. alarm display, battery and calibration protocol installations: with the electronic pressure measuring instrument testo 312-3, pressure- and gas-tightness can be tested. -
Surface Tension Measurement." Copyright 2000 CRC Press LLC
David B. Thiessen, et. al.. "Surface Tension Measurement." Copyright 2000 CRC Press LLC. <http://www.engnetbase.com>. Surface Tension Measurement 31.1 Mechanics of Fluid Surfaces 31.2 Standard Methods and Instrumentation Capillary Rise Method • Wilhelmy Plate and du Noüy Ring Methods • Maximum Bubble Pressure Method • Pendant Drop and Sessile Drop Methods • Drop Weight or Volume David B. Thiessen Method • Spinning Drop Method California Institute of Technology 31.3 Specialized Methods Dynamic Surface Tension • Surface Viscoelasticity • Kin F. Man Measurements at Extremes of Temperature and Pressure • California Institute of Technology Interfacial Tension The effect of surface tension is observed in many everyday situations. For example, a slowly leaking faucet drips because the force of surface tension allows the water to cling to it until a sufficient mass of water is accumulated to break free. Surface tension can cause a steel needle to “float” on the surface of water although its density is much higher than that of water. The surface of a liquid can be thought of as having a skin that is under tension. A liquid droplet is somewhat analogous to a balloon filled with air. The elastic skin of the balloon contains the air inside at a slightly higher pressure than the surrounding air. The surface of a liquid droplet likewise contains the liquid in the droplet at a pressure that is slightly higher than ambient. A clean liquid surface, however, is not elastic like a rubber skin. The tension in a piece of rubber increases as it is stretched and will eventually rupture. A clean liquid surface can be expanded indefinitely without changing the surface tension. -
Lecture # 04 Pressure Measurement Techniques and Instrumentation
AerE 344 class notes LectureLecture ## 0404 PressurePressure MeasurementMeasurement TechniquesTechniques andand InstrumentationInstrumentation Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 50011, U.S.A Copyright © by Dr. Hui Hu @ Iowa State University. All Rights Reserved! MeasurementMeasurement TechniquesTechniques forfor ThermalThermal--FluidsFluids StudiesStudies Velocity, temperature, density (concentration), etc.. • Pitot probe • hotwire, hot film Intrusive • thermocouples techniques • etc ... Thermal-Fluids measurement techniques • Laser Doppler Velocimetry (LDV) particle-based • Planar Doppler Velocimetry (PDV) techniques • Particle Image Velocimetry (PIV) • etc… Non-intrusive techniques • Laser Induced Fluorescence (LIF) • Molecular Tagging Velocimetry (MTV) molecule-based • Molecular Tagging Therometry (MTT) techniques • Pressure Sensitive Paint (PSP) • Temperature Sensitive Paint (TSP) • Quantum Dot Imaging • etc … Copyright © by Dr. Hui Hu @ Iowa State University. All Rights Reserved! Pressure measurements • Pressure is defined as the amount of force that presses on a certain area. – The pressure on the surface will increase if you make the force on an area bigger. – Making the area smaller and keeping the force the same also increase the pressure. – Pressure is a scalar F dF P = n = n A dA nˆ dFn dA τˆ Copyright © by Dr. Hui Hu @ Iowa State University. All Rights Reserved! Pressure measurements Pgauge = Pabsolute − Pamb Manometer Copyright © by Dr. Hui Hu @ Iowa State University. All Rights Reserved! -
Operations of the Geometric and Military Compass
OPERATIONS OF THE GEOMETRIC AND MILITARY COMPASS OF GALILEO GALILEI FLORENTINE PATRICIAN AND TEACHER OF MATHEMATICS in the University of Padua Dedicated to THE MOST SERENE PRINCE DON COSIMO DE’ MEDICI. PRINTED AT PADUA in the Author’s House, By Pietro Marinelli. 1606 With license of the Superiors Translated by Stillman Drake, Florence 1977 CONTENTS Dedication............................................................................................................................ 5 Prologue .............................................................................................................................. 6 Operation I Division of a line .................................................................................................................. 7 Operation II How in any given line we can take as many parts as may be required .............................. 8 Operation III How these same lines give us two, and even infinitely many, scales for altering one map into another larger or smaller ............................................................................... 8 Operation IV The rule-of-three solved by means of a compass and these same Arithmetic Lines .................................................................................................................................... 9 Operation V The inverse rule-of-three resolved by means of the same lines ......................................... 10 Operation VI Rule for monetary exchange .............................................................................................. -
Sources: Galileo's Correspondence
Sources: Galileo’s Correspondence Notes on the Translations The following collection of letters is the result of a selection made by the author from the correspondence of Galileo published by Antonio Favaro in his Le opere di Galileo Galilei,theEdizione Nazionale (EN), the second edition of which was published in 1968. These letters have been selected for their relevance to the inves- tigation of Galileo’s practical activities.1 The information they contain, moreover, often refers to subjects that are completely absent in Galileo’s publications. All of the letters selected are quoted in the work. The passages of the letters, which are quoted in the work, are set in italics here. Given the particular relevance of these letters, they have been translated into English for the first time by the author. This will provide the international reader with the opportunity to achieve a deeper comprehension of the work on the basis of the sources. The translation in itself, however, does not aim to produce a text that is easily read by a modern reader. The aim is to present an understandable English text that remains as close as possible to the original. The hope is that the evident disadvantage of having, for example, long and involute sentences using obsolete words is compensated by the fact that this sort of translation reduces to a minimum the integration of the interpretation of the translator into the English text. 1Another series of letters selected from Galileo’s correspondence and relevant to Galileo’s practical activities and, in particular, as a bell caster is published appended to Valleriani (2008). -
Here from the Main Rings to Enceladus M.K
Block Schedule Wednesday 7/27 Thursday 7/28 Friday 7/29 8:30 Introduction 8:40 Ring Objects 9:00 Dense Ring Ring 9:20 Structure Composition 9:40 10:00 10:20 10:40 Dense Ring Ring F ring 11:00 Structure Particle 11:20 (continued) Properties 11:40 12:00 12:20 12:40 Lunch Lunch 13:00 Lunch 13:20 13:40 14:00 Ring Particle Ring Origins 14:20 Sizes 14:40 Dusty Rings 15:00 OPUS 15:20 15:40 Intro to Posters Ring 16:00 Dusty Rings Evolution 16:20 and 16:40 Ring Environments Poster 17:00 Session 17:20 Discussion Discussion 17:40 18:00 18:30 19:00 Dinner on Campus BBQ at Treman Park Open 19:30 2 Wedsneday Morning, July 27 8:30-8:40 Welcome, Introduction 8:40-9:00 Revisiting the Self-Gravity Wakes Granola Bar Model: More Data, More Parameters J. E. Colwell, R. G. Jerousek, J. H. Cooney 9:00-9:20 Self-Gravity Wakes and the Viscosity of Dense Planetary Rings G. R. Stewart 9:20-9:40 B Ring Gray Ghosts in Cassini UVIS Occultations M. Sremˇcevi´c L.W. Esposito, J.E. Colwell, N. Albers 9:40-10:00 Simulating the B ring M. Lewis 10:00-10:20 Break 10:20-10:40 Noncircular Features in Saturn's Rings: I. The Cassini Division R. G. French, P. D. Nicholson, J. Colwell, E. A. Marouf, N. J. Rappaport, M. Hedman, K. Lonergan, C. McGhee-French, and T. Sepersky 10:40-11:00 Noncircular Features in Saturn's Rings: II. -
POLITECNICO DI TORINO Repository ISTITUZIONALE
POLITECNICO DI TORINO Repository ISTITUZIONALE Body temperature measurement from the 17th century to the present days Original Body temperature measurement from the 17th century to the present days / Angelini, Emma; Grassini, Sabrina; Parvis, Marco; Parvis, Luca; Gori, Andrea. - ELETTRONICO. - (2020), pp. 1-6. ((Intervento presentato al convegno 15th IEEE International Symposium on Medical Measurements and Applications - MeMeA2020 tenutosi a Bari, Italy nel 1-3 June 2020 [10.1109/MeMeA49120.2020.9137339]. Availability: This version is available at: 11583/2841349 since: 2020-08-25T14:41:07Z Publisher: IEEE Published DOI:10.1109/MeMeA49120.2020.9137339 Terms of use: openAccess This article is made available under terms and conditions as specified in the corresponding bibliographic description in the repository Publisher copyright IEEE postprint/Author's Accepted Manuscript ©2020 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future media, including reprinting/republishing this material for advertising or promotional purposes, creating new collecting works, for resale or lists, or reuse of any copyrighted component of this work in other works. (Article begins on next page) 07 October 2021 Body temperature measurement from the 17th century to the present days Emma Angelini Sabrina Grassini Department of Applied Science and Technology Department of Applied Science and Technology Politecnico di Torino Politecnico di Torino Torino, Italy Torino, Italy [email protected] -
Estimation of Internal Pressure of Liquids and Liquid Mixtures
Available online at www.ilcpa.pl International Letters of Chemistry, Physics and Astronomy 5 (2012) 1-7 ISSN 2299-3843 Estimation of internal pressure of liquids and liquid mixtures N. Santhi 1, P. Sabarathinam 2, G. Alamelumangai 1, J. Madhumitha 1, M. Emayavaramban 1 1Department of Chemistry, Government Arts College, C.Mutlur, Chidambaram-608102, India 2Retd. Registrar & Head of the Department of Technology, Annamalai University, Annamalainagar-608002, India E-mail address: [email protected] ABSTRACT By combining the van der Waals’ equation of state and the Free Length Theory of Jacobson, a new theoretical model is developed for the prediction of internal pressure of pure liquids and liquid mixtures. It requires only the molar volume data in addition to the ratio of heat capacities and critical temperature. The proposed model is simple, reliably accurate and capable of predicting internal pressure of pure liquids with an average absolute deviation of 4.24% in the predicted internal pressure values compared to those given in literature. The average absolute deviation in the predicted internal pressure values through the proposed model for the five binary liquid mixtures tested varies from 0.29% to 1.9% when compared to those of literature values. Keywords: van der Waals, pressure of liquids, theory of Jacobson, capacity of heat liquids, equation of Srivastava and Berkowitz 1. INTRODUTION The importance of internal pressure in understanding the properties of liquids and the full potential of internal pressure as a structural probe did become apparent with the pioneering work of Hildebrand 1, 2 and the first review of the subject by Richards 3 appeared in 1925. -
Solutions for Primary & Secondary Laboratories
1 üThe Source for Calibration Professionals Solutions for Primary & Secondary Laboratories Temperature Calibration Equipment & Services - Required calibration point for range Copper Freeze 1084.62ºC Point Cells COPPER FREEZES 1064.180ºC GOLD FREEZES Silver Freeze Point Cells 961.7800ºC Aluminium Freeze Point Cells 660.3230ºC ITL 17705 or 17702C or 17705 ITL hermometer 962 & 96178 & 962 hermometer T Zinc Freeze Point Cells 419.5270ºC ITL 17702B or ITL 17706 ITL or 17702B ITL Tin Freeze Point Cells 231.9280ºC 465 Indium Freeze 156.5985ºC hermocouple Point Cells ITL 17707 or 17702A or 17707 ITL T hermometer 909 & 670 & 909 hermometer T ITL 17701 ITL ITL 17703 ITL emperature Standard Platinum Resistance Resistance Platinum Standard emperature T Gallium Melt Point Cell & Apparatus 29.76460ºC Gold / Platinum Platinum / Gold High Triple Point Water Cell & Apparatus 0.010000ºC Mercury Triple Point Cell & Apparatus -38.83440ºC Boiling Point -189.3442ºC Standard Platinum Resistance Resistance Platinum Standard Comparator for TRIPLE POINT OF ARGON Argon, Nitrogen or Oxygen -218.7916ºC TRIPLE POINT OF OXYGEN -248.5939ºC TRIPLE POINT OF NEON -259.3467ºC TRIPLE POINT OF HYDROGEN -273.1500ºC Isotech ITS-90 ABSOLUTE ZERO ITS-90 Metrology Temperature Acceptable Furnaces Scale Thermometer Ranges For full details, contact Isothermal Technology Limited, Pine Grove, Southport, Merseyside PR9 9AG England Telephone +44 (0)1704 543830 Fax +44 (0)1704 544799 Email [email protected] Web www.isotech.co.uk Contents Metrology Instruments .........................................Inside Front The Best Comparison Calibration Equipment ........... 54 - 55 Introduction .................................................................. 4 - 5 Nitrogen Boiling Point Apparatus .................................. 57 Model 461 Simple Liquid N2 Apparatus ........................ 58 Primary ITS-90 Standards Model 459 Cryostat ....................................................