Measurements of the Thermal Conductivity and Electrical Resistivity of Platinum from 373 to 1373° K

Total Page:16

File Type:pdf, Size:1020Kb

Measurements of the Thermal Conductivity and Electrical Resistivity of Platinum from 373 to 1373° K NATIONAL BUREAU OF STANDARDS REPORT 9387 MEASUREMENTS OF THE THERMAL CONDUCTIVITY AND ELECTRICAL RESISTIVITY OF PLATINUM FROM 373 TO 1373° K by D. R. Flynn Environmental Engineering Section Building Research Division Institute for Applied Technology National Bureau of Standards and M. E. O' Hagan School of Engineering and Applied Science The George Washington University DO NOT REFERENCE THIS DOCUMENT U. S. DEPARTMENT OF COMMERCE NATIONAL BUREAU OF STANDARDS — THE NATIONAL BUREAU OF STANDARDS The National Bureau of Standards 1 provides measurement and technical information services essential to the efficiency and effectiveness of the work of the Nation’s scientists and engineers. The Bureau serves also as a focal point in the Federal Government for assuring maximum application of the physical and engineering sciences to the advancement of technology in industry and commerce. To accomplish this mission, the Bureau is organized into three institutes covering broad program areas of research and services: THE INSTITUTE FOR BASIC STANDARDS . provides the central basis within the United States for a complete and consistent system of physical measurements, coordinates that system with the measurement systems of other nations, and furnishes essential services leading to accurate and uniform physical measurements throughout the Nation’s scientific community, industry, and commerce. This Institute comprises a series of divisions, each serving a classical subject matter area: —Applied Mathematics—Electricity—Metrology—Mechanics—Heat—Atomic Physics—Physical 2 - 2 Chemistry—Radiation Physics—Laboratory Astrophysics —Radio Standards Laboratory , which includes Radio Standards Physics and Radio Standards Engineering—Office of Standard Refer- ence Data. THE INSTITUTE FOR MATERIALS RESEARCH . conducts materials research and provides associated materials services including mainly reference materials and data on the properties of ma- terials. Beyond its direct interest to the Nation’s scientists and engineers, this Institute yields services which are essential to the advancement of technology in industry and commerce. This Institute is or- ganized primarily by technical fields: —Analytical Chemistry—Metallurgy—Reactor Radiations—Polymers—Inorganic Materials—Cry- ogenics 2—Materials Evaluation Laboratory-—Office of Standard Reference Materials. APPLIED . provides technical services to promote the THE INSTITUTE FOR TECHNOLOGY . use of available technology and to facilitate technological innovation in industry and government. The principal elements of this Institute are: —Building Research—Electronic Instrumentation—Textile and Apparel Technology Center Technical Analysis—Center for Computer Sciences and Technology—Office of Weights and Meas- ures—Office of Engineering Standards Services—Office of Invention and Innovation—Clearing- 3 house for Federal Scientific and Technical Information . 1 Headquarters and Laboratories at Gaithersburg, Maryland, unless otherwise noted; mailing address Washington, D. C., 20234. 2 Located at Boulder, Colorado, 80302. 3 Located at 5285 Port Royal Road, Springfield, Virginia, 22151. NATIONAL BUREAU OF STANDARDS REPORT NBS PROJECT NBS REPORT 421.03-40-4212231 9387 August 22, 1966 MEASUREMENTS OF THE THERMAL CONDUCTIVITY AND ELECTRICAL RESISTIVITY OF PLATINUM FROM 373 TO 1373 °K by D. R. Flynn Environmental Engineering Section Building Research Division Institute for Applied Technology National Bureau of Standards and M. E. O' Hagan School of Engineering and Applied Science The George Washington University DO NOT REFERENCE THIS DOCUMENT IMPORTANT NOTICE NATIONAL BUREAU OF ST l s accounting documents intended for use within the Government, Approved for public release by the subjected to additional evaluation and review. For this reason, the Director of the National Institute of listing of this Report, either in whole or in part, is not author! Office of the Director, National (NIST) Bureau of Standards, Washingto Standards and Technology the Government agency for which the Report has been specifically on October 9, 2015 pies for its own use. U. S. DEPARTMENT OF COMMERCE NATIONAL BUREAU Of STANDARDS ABSTRACT Measurements have been made of the thermal conductivity and the electri- cal resistivity of commercial grade platinum (99.98% pure) in the temperature range 373 to 1373 °K. The measurements have been made with a view to providing accurate data on the thermal conductivity of platinum to serve as a basis for establishing platinum as a thermal conductivity standard reference material. Two methods of measuring the thermal conductivity have been employed, one an electrical method and the other a non-electrical method. In the electri- cal method, a direct current passed through a necked-down portion of the speci- men and the thermal conductivity was determined in terms of the temperature and electrical potential distribution in the necked-down region. The second method was of the absolute guarded longitudinal heat flow type. The experiment was designed to permit measurements by both methods in the same apparatus and on the same specimen thereby providing as direct a comparison as possible between the methods. The data given by the two methods agree within experimental error and show the thermal conductivity of platinum to be a smoothly increasing function of temperature in the measured range. The data are considered to be accurate to better than 1% and indicate that platinum could be adopted as a thermal conductivity standard reference material. ii TABLE OF CONTENTS Page ACKNOWLEDGMENTS v LIST OF TABLES . ....... V £ LIST OF ILLUSTRATIONS vii INTRODUCTION .................. 1 Chapter I. PREVIOUS INVESTIGATIONS 4 II. DESCRIPTION OF THE APPARATUS ....... 24 Mechanical Configuration 27 Specimen 27 Furnace 34 Environmental System 36 Thermal Configuration 37 Specimen 37 Guard 42 Instrumentation 45 Temperature Control 45 Temperature Measurement 46 Power Measurement 46 Resistance Measurement 46 III. THEORY OF THE INDIRECT METHOD 50 IV. CALCULATION PROCEDURES 63 Indirect Method 63 Direct Method 73 V. SPECIMEN CHARACTERIZATION 85 Source 85 Fabrication and Thermal History 85 Hardness 88 Spectrographic Analysis . 88 Metallography 89 Density 89 Residual Resistance 91 Ice-Point Resistivity 92 EMF vs Pt 27 93 - iii - VI. TEST PROCEDURES 94 Direct Method 95 Resistivity 97 Indirect Method 98 VII. RESULTS 101 Electrical Resistivity 101 Thermal Conductivity ....... ....... 106 VIII. DISCUSSION OF RESULTS 116 Accuracy ....... ..... 116 Electrical Resistivity . 116 Thermal Conductivity ....... 117 Comparison with Other Investigations . 130 Electrical Resistivity ..... ..... 130 Thermal Conductivity 131 Appendix A. Machining the Neck and Wiring the Specimen . 138 B. Potential Perturbations . ..... 141 C. The Thomson Effect . 148 D. Alternative Calculation Procedure for the Indirect Method . 150 E. A Simplified Expression for the Maximum Temperature Rise in the Neck in the Presence of Heat Losses 152 F. Derivation of the Equation for Heat Flow in the Current Leads of the Specimen Heater 154 G. Errors in Temperature Measurements Due to Heat Conduction along Thermocouple Wires 157 H. Departures from One -Dimensional Heat Flow in the Direct Method 160 I. Tempering of the Heater Current Leads 162 References 164 - iv - ACKNOWLEDGMENTS This research was the subject of a dissertation submitted by Malcolm O'Hagan to the Faculty of The School of Engineering and Applied Science, The George Washington University, in partial satisfaction of the requirements for the degree of Doctor of Science. This work was supported in part by Engelhard Industries, Inc., Newark, New Jersey, who supplied the platinum and financial assistance in the form of a Grant to the National Bureau of Standards. We thank Henry G. Albert and A. V. Lincoln, both of Engelhard Industries, Inc., for their support and advice. Malcolm E. O'Hagan was supported in part by Grant AFOSR-1025-66 from the Air Force Office of Scientific Research and in part by the Institute for Industrial Research and Standards, Dublin, Ireland. We thank Henry E„ Robinson, Chief, Environmental Engineering Section, NBS, and Adjunct Professor of Engineering, The George Washington University for his advice and support. The intricate and difficult machining required for this project was done by Raymond Chidester, Section 145.01 NBS. Much good advice in matters of fabrication came from John Hettenhouser , Section 145.01 NBS. - v - LIST OF TABLES Table Page 1. Sample characterization of platinum samples used by various investigators 17 2. Thermal conductivity of platinum in the temperature range 273-373 °K as reported by several investigators ... 18 3. Hardness values as measured on the platinum bar .... 88 4. Spectrographic analysis as determined on platinum wire No. 175105 89 5. Resistance values for three samples of platinum at ice- point and helium-point temperatures and the computed re- sistance ratios at zero current 92 6. EMF vs Pt 27 as determined on 20-mil platinum wire. 93 7. Experimental values for the thermal conductivity of platinum as determined by the direct method 107 8. Typical set of data from measurements of the thermal con- ductivity by the direct method 108 9. Experimental values for the thermal conductivity of platinum as determined by the indirect method .... 113 10. Comparison of smoothed resistivity values for platinum with those of other investigators 130 11. Thermal conductivity of platinum 132 12. Values for the relative magnitude of the Thomson Term . 149 U(T) 13. Values of o 0 m) for
Recommended publications
  • Effect of Glass Transition: Density and Thermal Conductivity Measurements of B2O3
    High Temperatures-High Pressures, Vol. 49, pp. 125–142 ©2020 Old City Publishing, Inc. Reprints available directly from the publisher Published by license under the OCP Science imprint, Photocopying permitted by license only a member of the Old City Publishing Group DOI: 10.32908/hthp.v49.801 Effect of glass transition: density and thermal conductivity measurements of B2O3 DMITRY CHEBYKIN1*, HANS-PETER HELLER1, IVAN SAENKO2, GERT BARTZSCH1, RIE ENDO3 AND OLENA VOLKOVA1 1Institute of Iron and Steel Technology, TU Bergakademie Freiberg, Leipziger Straße 34, 09599 Freiberg, Germany 2Institute of Materials Science, TU Bergakademie Freiberg, Gustav-Zeuner-Straße 5, 09599 Freiberg, Germany 3Department of Materials Science and Engineering, Tokyo Institute of Technology, 152–8552 Tokyo, Japan Received: May 28, 2019; Accepted: October 11, 2019. The role of B2O3 as a fluxing agent for developing fluoride free fluxes has been accentuated in the recent years. Therefore, knowledge about thermo- physical properties of the oxide are essential to find the optimal chemical composition of the mold fluxes. In the present study, the density and ther- mal conductivity of B2O3 were measured by means of the buoyancy method, the maximal bubble pressure (MBP) method and the hot-wire method in the temperature range of 295–1573 K. The results are discussed in the context of the chemical stability of the B2O3 as well as the effect of glass transition on the thermal conductivity. The density of the B2O3 decreases non-linearly with increasing temperature in the temperature range of 973–1573 K. The MBP method was successfully applied for the density measurements with a viscosity up to 91 Pa.s.
    [Show full text]
  • R09 SI: Thermal Properties of Foods
    Related Commercial Resources CHAPTER 9 THERMAL PROPERTIES OF FOODS Thermal Properties of Food Constituents ................................. 9.1 Enthalpy .................................................................................... 9.7 Thermal Properties of Foods ..................................................... 9.1 Thermal Conductivity ................................................................ 9.9 Water Content ........................................................................... 9.2 Thermal Diffusivity .................................................................. 9.17 Initial Freezing Point ................................................................. 9.2 Heat of Respiration ................................................................. 9.18 Ice Fraction ............................................................................... 9.2 Transpiration of Fresh Fruits and Vegetables ......................... 9.19 Density ...................................................................................... 9.6 Surface Heat Transfer Coefficient ........................................... 9.25 Specific Heat ............................................................................. 9.6 Symbols ................................................................................... 9.28 HERMAL properties of foods and beverages must be known rizes prediction methods for estimating these thermophysical proper- Tto perform the various heat transfer calculations involved in de- ties and includes examples on the
    [Show full text]
  • THERMAL CONDUCTIVITY of CONTINUOUS CARBON FIBRE REINFORCED COPPER MATRIX COMPOSITES J.Koráb1, P.Šebo1, P.Štefánik 1, S.Kavecký 1 and G.Korb 2
    1. THERMAL CONDUCTIVITY OF CONTINUOUS CARBON FIBRE REINFORCED COPPER MATRIX COMPOSITES J.Koráb1, P.Šebo1, P.Štefánik 1, S.Kavecký 1 and G.Korb 2 1 Institute of Materials and Machine Mechanics of the Slovak Academy of Sciences, Racianska 75, 836 06 Bratislava, Slovak Republic 2 Austrian Research Centre Seibersdorf, A-2444 Seibersdorf, Austria SUMMARY: The paper deals with thermal conductivity of the continuous carbon fibre reinforced - copper matrix composite that can be applied in the field of electric and electronic industry as a heat sink material. The copper matrix - carbon fibre composite with different fibre orientation and fibre content was produced by diffusion bonding of copper-coated carbon fibres. Laser flash technique was used for thermal conductivity characterisation in direction parallel and transverse to fibre orientation. The results revealed decreasing thermal conductivity as the volume content of fibre increased and independence of through thickness conductivity on fibre orientation. Achieved results were compared with the materials that are currently used as heat sinks and possibility of the copper- based composite application was analysed. KEYWORDS: thermal conductivity, copper matrix, carbon fibre, metal matrix composite, heat sink, thermal management, heat dissipation INTRODUCTION Carbon fibre reinforced - copper matrix composite (Cu-Cf MMC) offer thermomechanical properties (TMP) which are now required in electronic and electric industry. Their advantages are low density, very good thermal conductivity and tailorable coefficient of thermal expansion (CTE). These properties are important in the applications where especially thermal conductivity plays large role to solve the problems of heat dissipation due to the usage of increasingly powerful electronic components. In devices, where high density mounting technology is applied thermal management is crucial for the reliability and long life performance.
    [Show full text]
  • Carbon Epoxy Composites Thermal Conductivity at 77 K and 300 K Jean-Luc Battaglia, Manal Saboul, Jérôme Pailhes, Abdelhak Saci, Andrzej Kusiak, Olivier Fudym
    Carbon epoxy composites thermal conductivity at 77 K and 300 K Jean-Luc Battaglia, Manal Saboul, Jérôme Pailhes, Abdelhak Saci, Andrzej Kusiak, Olivier Fudym To cite this version: Jean-Luc Battaglia, Manal Saboul, Jérôme Pailhes, Abdelhak Saci, Andrzej Kusiak, et al.. Carbon epoxy composites thermal conductivity at 77 K and 300 K. Journal of Applied Physics, American Institute of Physics, 2014, 115 (22), pp.223516-1 - 223516-4. 10.1063/1.4882300. hal-01063420 HAL Id: hal-01063420 https://hal.archives-ouvertes.fr/hal-01063420 Submitted on 12 Sep 2014 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Science Arts & Métiers (SAM) is an open access repository that collects the work of Arts et Métiers ParisTech researchers and makes it freely available over the web where possible. This is an author-deposited version published in: http://sam.ensam.eu Handle ID: .http://hdl.handle.net/10985/8502 To cite this version : Jean-Luc BATTAGLIA, Manal SABOUL, Jérôme PAILHES, Abdelhak SACI, Andrzej KUSIAK, Olivier FUDYM - Carbon epoxy composites thermal conductivity at 80 K and 300 K - Journal of Applied Physics - Vol. 115, n°22, p.223516-1 - 223516-4 - 2014 Any correspondence concerning this service should be sent to the repository Administrator : [email protected] Carbon epoxy composites thermal conductivity at 80 K and 300 K J.-L.
    [Show full text]
  • The Viscosity and Thermal Conductivity Coefficients of Dilute Nitrogen and Oxygen
    jras : .<; : .:' '.: » l\l 1 ^rf' ' » * ^ 1 350 The Viscosity and Thermal Conductivity Coefficients of Dilute Nitrogen and Oxygen G. E. CHI LDS AND H. J. M. HANLEY F *** ° Cf »* U.S. DEPARTMENT OF COMMERCE ,&': Z (A National Bureau of Standards \ n ' *"*C A U O? — THE NATIONAL BUREAU OF STANDARDS The National Bureau of Standards 1 provides measurement and technical information services essential to the efficiency and effectiveness of the work of the Nation's scientists and engineers. The Bureau serves also as a focal point in the Federal Government for assuring maximum application of the physical and engineering sciences to the advancement of technology in industry and commerce. To accomplish this mission, the Bureau is organized into three institutes covering broad program areas of research and services: THE INSTITUTE FOR BASIC STANDARDS . provides the central basis within the United States for a complete and consistent system of physical measurements, coordinates that system with the measurement systems of other nations, and furnishes essential services leading to accurate and uniform physical measurements throughout the Nation's scientific community, industry, and commerce. This Institute comprises a series of divisions, each serving a classical subject matter area: —Applied Mathematics—Electricity—Metrology—Mechanics —Heat—Atomic Physics—Physical Chemistry—Radiation Physics—Laboratory Astrophysics 2—Radio Standards Laboratory, 2 which includes Radio Standards Physics and Radio Standards Engineering—Office of Standard Refer- ence Data. THE INSTITUTE FOR MATERIALS RESEARCH . conducts materials research and provides associated materials services including mainly reference materials and data on the properties of ma- terials. Beyond its direct interest to the Nation's scientists and engineers, this Institute yields services which are essential to the advancement of technology in industry and commerce.
    [Show full text]
  • Thermodynamic Temperature
    Thermodynamic temperature Thermodynamic temperature is the absolute measure 1 Overview of temperature and is one of the principal parameters of thermodynamics. Temperature is a measure of the random submicroscopic Thermodynamic temperature is defined by the third law motions and vibrations of the particle constituents of of thermodynamics in which the theoretically lowest tem- matter. These motions comprise the internal energy of perature is the null or zero point. At this point, absolute a substance. More specifically, the thermodynamic tem- zero, the particle constituents of matter have minimal perature of any bulk quantity of matter is the measure motion and can become no colder.[1][2] In the quantum- of the average kinetic energy per classical (i.e., non- mechanical description, matter at absolute zero is in its quantum) degree of freedom of its constituent particles. ground state, which is its state of lowest energy. Thermo- “Translational motions” are almost always in the classical dynamic temperature is often also called absolute tem- regime. Translational motions are ordinary, whole-body perature, for two reasons: one, proposed by Kelvin, that movements in three-dimensional space in which particles it does not depend on the properties of a particular mate- move about and exchange energy in collisions. Figure 1 rial; two that it refers to an absolute zero according to the below shows translational motion in gases; Figure 4 be- properties of the ideal gas. low shows translational motion in solids. Thermodynamic temperature’s null point, absolute zero, is the temperature The International System of Units specifies a particular at which the particle constituents of matter are as close as scale for thermodynamic temperature.
    [Show full text]
  • Determination of Thermal Conductivity, Specific Heat and Thermal
    Biosystems Engineering (2002) 82 (2), 169–176 doi:10.1006/bioe.2002.0066, available online at http://www.idealibrary.com on PH}Postharvest Technology Determination of Thermal Conductivity, Specific Heat and Thermal Diffusivity of Borage Seeds W. Yang1; S. Sokhansanj2; J. Tang3; P. Winter4 1 Department of Food Science, University of Arkansas, 2650 N. Young Ave., Fayetteville, AR 72704, USA; e-mail of corresponding author: [email protected] 2 Oak Ridge National Lab, Bioenergy Feedstock Development Program, Oak Ridge, TN 37831-6422, USA; e-mail: [email protected] 3 Food Engineering Program, Department of Biological Systems Engineering, Washington State University, Pullman, WA 99164-6120, USA; e-mail: [email protected] 4 Hinz Automation, Inc., 410 Jessop Ave., Saskatoon, SK, Canada S7N 2S5; e-mail: [email protected] (Received 16 March 1999; accepted in revised form 15 February 2002; published online 11 June 2002) Thermal conductivity, specific heat capacity and thermal diffusivity of borage (Borago officinalis) seeds were determined at temperatures ranging from 6 to 208C and moisture contents from 1Á2to30Á3% w.b. The thermal conductivity was measured by the transient technique using a line heat source. The maximum slope method was used to analyse the line source heating data for thermal conductivity determination. The specific heat capacity was measured by different scanning calorimetry and ranged from 0Á77 to 1Á99 kJ kgÀ1KÀ1. The thermal conductivity of borage seeds ranged from 0Á11 to 0Á28 W mÀ1 KÀ1 and increased with moisture content in the range of 1Á2–30Á3% w.b. The thermal diffusivity ranged from 2Á32 Â 10À7 to 3Á18 Â 10À7 m2 sÀ1.
    [Show full text]
  • Thermal Properties of Water
    Forschungszentrum Karlsruhe Technik und Umwelt issenscnatiiK FZKA 5588 Thermal Properties of Water K. Thurnay Institut für Neutronenphysik und Reaktortechnik Projekt Nukleare Sicherheitsforschung Juni 1995 Forschungszentrum Karlsruhe Technik und Umwelt Wissenschaftliche Berichte FZKA 5588 Thermal Properties of Water K.Thurnay Institut für Neutronenphysik und Reaktortechnik Projekt Nukleare Sicherheitsforschung Forschungszentrum Karlsruhe GmbH, Karlsruhe 1995 Als Manuskript gedruckt Für diesen Bericht behalten wir uns alle Rechte vor Forschungszentrum Karlsruhe GmbH Postfach 3640, 76021 Karlsruhe ISSN 0947-8620 Abstract The report describes AQUA, a code developed in the Forschungszentrum Karlsruhe to calculate thermal properties of the water in steam explosions. AQUA bases on the H.G.K, water code, yet supplies - besides of the pressure and heat capacity functions - also the thermal conductivity, viscosity and the surface tension. AQUA calculates in a new way the thermal properties in the two phase region, which is more realistic as the one used in the H.G.K, code. AQUA is equipped with new, fast runnig routines to convert temperature-density dependent states into temperature-pressure ones. AQUA has a version to be used on line and versions adapted for batch calculations. A complete description of the code is included. Thermische Eigenschaften des Wassers. Zusammenfassung. Der Bericht befaßt sich mit dem Code AQUA. AQUA wurde im Forschungszentrum Karlsruhe entwickelt um bei der Untersuchung von Dampfexplosionen die thermischen Eigenschaften des Wassers zu liefern. AQUA ist eine Fortentwicklung des H.G.K.-Wassercodes, aber er berechnet - neben Druck- und Wärmeeigenschaften - auch die Wärmeleitfähigket, die Viskosität und die Oberflächenspannung. Im Zweiphasenge• biet beschreibt AQUA die thermischen Eigenschaften mit einer neuen Methode, die real• istischer ist, als das in der H.G.K.-Code dargebotene Verfahren.
    [Show full text]
  • Thermal Conductivity 1 Thermal Conductivity
    Thermal conductivity 1 Thermal conductivity In physics, thermal conductivity, , is the property of a material's ability to conduct heat. It appears primarily in Fourier's Law for heat conduction. Thermal conductivity is measured in watts per kelvin-meter (W·K−1·m−1, i.e. W/(K·m) or in IP units (Btu·hr−1·ft−1·F−1, i.e. Btu/(hr·ft⋅F). Multiplied by a temperature difference (in kelvins, K) and an area (in square meters, m2), and divided by a thickness (in meters, m), the thermal conductivity predicts the rate of energy loss (in watts, W) through a piece of material. In the window building industry "thermal conductivity" is expressed as the U-Factor [1], which measures the rate of heat transfer and tells you how well the window insulates. U-factor values are generally recorded in IP units (Btu/(hr·ft⋅F)) and usually range from 0.15 to 1.25. The lower the U-factor, the better the window insulates. The reciprocal of thermal conductivity is thermal resistivity. Measurement There are a number of ways to measure thermal conductivity. Each of these is suitable for a limited range of materials, depending on the thermal properties and the medium temperature. There is a distinction between steady-state and transient techniques. In general, steady-state techniques are useful when the temperature of the material does not change with time. This makes the signal analysis straightforward (steady state implies constant signals). The disadvantage is that a well-engineered experimental setup is usually needed. The Divided Bar (various types) is the most common device used for consolidated rock samples.
    [Show full text]
  • The Properties of Helium: Density, Specific Heats, Viscosity, and Thermal Conductivity at Pressures from 1 to 100 Bar and from Room Temperature to About 1800 K
    View metadata,Downloaded citation and from similar orbit.dtu.dk papers on:at core.ac.uk Dec 20, 2017 brought to you by CORE provided by Online Research Database In Technology The properties of helium: Density, specific heats, viscosity, and thermal conductivity at pressures from 1 to 100 bar and from room temperature to about 1800 K Forskningscenter Risø, Roskilde Publication date: 1970 Document Version Publisher's PDF, also known as Version of record Link back to DTU Orbit Citation (APA): Petersen, H. (1970). The properties of helium: Density, specific heats, viscosity, and thermal conductivity at pressures from 1 to 100 bar and from room temperature to about 1800 K. (Denmark. Forskningscenter Risoe. Risoe-R; No. 224). General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. • Users may download and print one copy of any publication from the public portal for the purpose of private study or research. • You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. « Riso Report No. 224 5 o, « Danish Atomic Energy Commission .1 * Research Establishment Ris6 The Properties of Helium: Density, Specific Heats, Viscosity, and Thermal Conductivity at Pressures from 1 to 100 bar and from Room Temperature to about 1800 K by Helge Petersen September, 1970 Sain dUiributort: JUL GjiUtrap, 17, »Wpdt, DK-U07 Capubaftn K, Dnaurk U.D.C m»!:62U34.3t September, 1 970 Rise Report No.
    [Show full text]
  • The Properties of Helium: Density, Specific Heats, Viscosity, and Thermal Conductivity at Pressures from 1 to 100 Bar and from Room Temperature to About 1800 K
    Downloaded from orbit.dtu.dk on: Oct 04, 2021 The properties of helium: Density, specific heats, viscosity, and thermal conductivity at pressures from 1 to 100 bar and from room temperature to about 1800 K Petersen, H. Publication date: 1970 Document Version Publisher's PDF, also known as Version of record Link back to DTU Orbit Citation (APA): Petersen, H. (1970). The properties of helium: Density, specific heats, viscosity, and thermal conductivity at pressures from 1 to 100 bar and from room temperature to about 1800 K. Risø National Laboratory. Denmark. Forskningscenter Risoe. Risoe-R No. 224 General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Users may download and print one copy of any publication from the public portal for the purpose of private study or research. You may not further distribute the material or use it for any profit-making activity or commercial gain You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. « Riso Report No. 224 5 o, « Danish Atomic Energy Commission .1 * Research Establishment Ris6 The Properties of Helium: Density, Specific Heats, Viscosity, and Thermal Conductivity at Pressures from 1 to 100 bar and from Room Temperature to about 1800 K by Helge Petersen September, 1970 Sain dUiributort: JUL GjiUtrap, 17, »Wpdt, DK-U07 Capubaftn K, Dnaurk U.D.C m»!:62U34.3t September, 1 970 Rise Report No.
    [Show full text]
  • Modeling the Thermal Conductivity of Concrete Based on Its Measured Density and Porosity
    Modeling the Thermal Conductivity of Concrete Based on Its Measured Density and Porosity .loA. Tinker J.G. Cabrera ABSTRACT material. In order to satisfactorily model the thennal conductivity of the composites from the properties of the The relationship between density and conductive heat individual components, it is necessary to choose a model transfer through mulliphase, porous materials is reasonably whose theoretical assumptions represent the distribution and well understood and can be evaluated using simple em­ shape of the component phases within the mixture as closely pirical relations. However, the complex effects ofporosity, as possible. However, in view of the complexity of the particularly pore size and volume, on heat transfer are structure of real materials, there are comparatively few mechanisms far less understood. To date, very few formulae cases where such theoretical assumptions can be applied are available that assess the effect that these variables have rigorously. The limiting factor in most models is the on heat conduction properties of a multiphase material. agreement between the theoretical assumptions and the This paper presents the results ofan experimental study structure of the actual material. designed to evaluate the influence ofpore characteristics on A small number of models have been reported that the thermal conductivity of concrete, a composite widely specifically calculate the conductive heat transfer of con­ used as a construction material. cretes (Pratt 1962; Valore 1980; Campbell-Allen and Twenty-one different concretes were made with densities Thome 1963). These models express the conductive heat that variedfrom 97to 146lbljii (1,550 to 2,350kg/m3) and transfer in terms of the conductivities and the fractional porosities from 10% to 39%.
    [Show full text]