Retention-Ph Profiles of Acids and Bases in Hydrophilic Interaction Liquid Chromatography
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Electric Permittivity of Carbon Fiber
Carbon 143 (2019) 475e480 Contents lists available at ScienceDirect Carbon journal homepage: www.elsevier.com/locate/carbon Electric permittivity of carbon fiber * Asma A. Eddib, D.D.L. Chung Composite Materials Research Laboratory, Department of Mechanical and Aerospace Engineering, University at Buffalo, The State University of New York, Buffalo, NY, 14260-4400, USA article info abstract Article history: The electric permittivity is a fundamental material property that affects electrical, electromagnetic and Received 19 July 2018 electrochemical applications. This work provides the first determination of the permittivity of contin- Received in revised form uous carbon fibers. The measurement is conducted along the fiber axis by capacitance measurement at 25 October 2018 2 kHz using an LCR meter, with a dielectric film between specimen and electrode (necessary because an Accepted 11 November 2018 LCR meter is not designed to measure the capacitance of an electrical conductor), and with decoupling of Available online 19 November 2018 the contributions of the specimen volume and specimen-electrode interface to the measured capaci- tance. The relative permittivity is 4960 ± 662 and 3960 ± 450 for Thornel P-100 (more graphitic) and Thornel P-25 fibers (less graphitic), respectively. These values are high compared to those of discon- tinuous carbons, such as reduced graphite oxide (relative permittivity 1130), but are low compared to those of steels, which are more conductive than carbon fibers. The high permittivity of carbon fibers compared to discontinuous carbons is attributed to the continuity of the fibers and the consequent substantial distance that the electrons can move during polarization. The P-100/P-25 permittivity ratio is 1.3, whereas the P-100/P-25 conductivity ratio is 67. -
VELOCITY of PROPAGATION by RON HRANAC
Originally appeared in the March 2010 issue of Communications Technology. VELOCITY OF PROPAGATION By RON HRANAC If you’ve looked at a spec sheet for coaxial cable, you’ve no doubt seen a parameter called velocity of propagation. For instance, the published velocity of propagation for CommScope’s F59 HEC-2 headend cable is "84% nominal," and Times Fiber’s T10.500 feeder cable has a published value of "87% nominal." What do these numbers mean, and where do they come from? We know that the speed of light in free space is 299,792,458 meters per second, which works out to 299,792,458/0.3048 = 983,571,056.43 feet per second, or 983,571,056.43/5,280 = 186,282.4 miles per second. The reciprocal of the free space value of the speed of light in feet per second is the time it takes for light to travel 1 foot: 1/983,571,056.43 = 1.02E-9 second, or 1.02 nanosecond. In other words, light travels a foot in free space in about a billionth of a second. Light is part of the electromagnetic spectrum, as is RF. That means RF zips along at the same speed that light does. "The major culprit that slows the waves down is the dielectric — and it slows TEM waves down a bunch." Now let’s define velocity of propagation: It’s the speed at which an electromagnetic wave propagates through a medium such as coaxial cable, expressed as a percentage of the free space value of the speed of light. -
Importance of Varying Permittivity on the Conductivity of Polyelectrolyte Solutions
Importance of Varying Permittivity on the Conductivity of Polyelectrolyte Solutions Florian Fahrenberger, Owen A. Hickey, Jens Smiatek, and Christian Holm∗ Institut f¨urComputerphysik, Universit¨atStuttgart, Allmandring 3, Stuttgart 70569, Germany (Dated: September 8, 2018) Dissolved ions can alter the local permittivity of water, nevertheless most theories and simulations ignore this fact. We present a novel algorithm for treating spatial and temporal variations in the permittivity and use it to measure the equivalent conductivity of a salt-free polyelectrolyte solution. Our new approach quantitatively reproduces experimental results unlike simulations with a constant permittivity that even qualitatively fail to describe the data. We can relate this success to a change in the ion distribution close to the polymer due to the built-up of a permittivity gradient. The dielectric permittivity " measures the polarizabil- grained approach is necessary due to the excessive sys- ity of a medium subjected to an electric field and is one of tem size. Molecular Dynamics (MD) simulations of only two fundamental constants in Maxwell's equations. charged systems typically work with the restricted prim- The relative permittivity of pure water at room temper- itive model by simulating the ions as hard spheres while ature is roughly 78.5, but charged objects dissolved in accounting for the solvent implicitly through a con- the fluid significantly reduce the local dielectric constant stant background dielectric. Crucially, the solvent me- because water dipoles align with the local electric field diates hydrodynamic interactions and reduces the elec- created by the object rather than the external field [1{3]. trostatic interactions due to its polarizability. -
Measurement of Dielectric Material Properties Application Note
with examples examples with solutions testing practical to show written properties. dielectric to the s-parameters converting for methods shows Italso analyzer. a network using materials of properties dielectric the measure to methods the describes note The application | | | | Products: Note Application Properties Material of Dielectric Measurement R&S R&S R&S R&S ZNB ZNB ZVT ZVA ZNC ZNC Another application note will be will note application Another <Application Note> Kuek Chee Yaw 04.2012- RAC0607-0019_1_4E Table of Contents Table of Contents 1 Overview ................................................................................. 3 2 Measurement Methods .......................................................... 3 Transmission/Reflection Line method ....................................................... 5 Open ended coaxial probe method ............................................................ 7 Free space method ....................................................................................... 8 Resonant method ......................................................................................... 9 3 Measurement Procedure ..................................................... 11 4 Conversion Methods ............................................................ 11 Nicholson-Ross-Weir (NRW) .....................................................................12 NIST Iterative...............................................................................................13 New non-iterative .......................................................................................14 -
Product Information PA 2200
Product Information PA 2200 PA 2200 is a non-filled powder on basis of PA 12. General Properties Property Measurement Method Units Value DIN/ISO Water absorption ISO 62 / DIN 53495 100°C, saturation in water % 1.93 23°C, 96% RF % 1.33 23°C, 50% RF % 0.52 Property Measurement Method Unit Value DIN/ISO Coefficient of linear thermal ex- ISO 11359 / DIN 53752-A x10-4 /K 1.09 pansion Specific heat DIN 51005 J/gK 2.35 Thermal properties of sintered parts Property Measurement Method Unit Value DIN/ISO Thermal conductivity DIN 52616 vertical to sintered layers W/mK 0.144 parallel to sintered layers W/mK 0.127 EOS GmbH - Electro Optical Systems Robert-Stirling-Ring 1 D-82152 Krailling / München Telefon: +49 (0)89 / 893 36-0 AHO / 03.10 Telefax: +49 (0)89 / 893 36-285 PA2200_Product_information_03-10_en.doc 1 / 10 Internet: www.eos.info Product Information Short term influcence of temperature on mechanical properties An overview about the temperature dependence of mechanical properties of PA 12 can be re- trieved from the curves for dynamic shear modulus and loss factor as function of temperature according to ISO 537. PA 2200 dynamic mechanical analysis (torsion) Temp.: - 100 bis 188°C 1E+10 G' 1E+03 G" tan_delta 1E+02 1E+09 , 1E+01 1E+08 tan_delta 1E+00 1E+07 loss modulus G´´ [Pa] 1E-01 storage modulus G´ [Pa] modulus storage 1E+06 1E-02 1E+05 1E-03 -100 -50 0 50 100 150 200 Temperature [°C] In general parts made of PA 12 show high mechanical strength and elasticity under steady stress in a temperature range from - 40°C till + 80°C. -
Kémia Idegen Nyelven 147
Kémia idegen nyelven 147 KÉMIA IDEGEN NYELVEN Kémia németül Szerkesztő: Horváth Judit A 2014/4. számban megjelent szakszöveg helyes fordítása: Pigmentek és festékek1 Pigmentek és kötőanyagok2 A pigment a felhasználásra szánt közegben (lakk, festék) oldhatatlan festékanyag, mely legtöbbször nagyon finoman eloszlatott formában van jelen. Az oldható festékanyagokat ezzel szemben színezékeknek3 színezékeket inkább színezésre. A tiszta pigment nem tartalmaz adaléknevezzük.anyago Pigmenteketkat. főként festésnél hatása és mázolásnál a kémiai összetételhasználunk, 4 függ. Az optimális Egyrészecskeméret pigment színező egy ötszázad és egy kétezredtől, millimétera kristályszerkezettől, között van. a részecskemérettől és az egész belső felülettől Ahhoz, hogy egy festékpigment tapadjon egy felületre, kötőanyaggal kell összekeverni. A kötőanyagok olyan anyagok, melyek finom eloszlású egyéb anyagokat felragasztanak egy alapra. Festék megszilárdulása alapon 5. Felhasználásielőállításához aterület pigmentet és festékkötőanyaggal6 keverik össze, és annak alkalmatosak. Használatután a pigment a festendő rögzítődik fehérjék, a szerint különféle kötőanyagok lenolaj hozzákeverésévelosak a gumik, olajfestéket. gyanták, Aviaszok, vízfestékekben olajok, cellulóz vagy a mész. Így kapunk például az ultramarinkék pigmentből Az iskolákban gyakran használt gumiarábikumot, a kazeinfestékekben a kazein nevű tejfehérjét alkalmazzák kötőanyagnak. 148 Kémia idegen nyelven plakátfesték7 a Pelikan temperafesték enyv–olaj–víz emulziót tartalmaz a pigment megkötésére. Az -
The Impact of Ph on the Structure and Function of Neural Cadherin
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by eGrove (Univ. of Mississippi) University of Mississippi eGrove Electronic Theses and Dissertations Graduate School 1-1-2014 The Impact of pH on the Structure and Function of Neural Cadherin Jared Michael Jungles University of Mississippi Follow this and additional works at: https://egrove.olemiss.edu/etd Part of the Chemistry Commons Recommended Citation Jungles, Jared Michael, "The Impact of pH on the Structure and Function of Neural Cadherin" (2014). Electronic Theses and Dissertations. 1288. https://egrove.olemiss.edu/etd/1288 This Dissertation is brought to you for free and open access by the Graduate School at eGrove. It has been accepted for inclusion in Electronic Theses and Dissertations by an authorized administrator of eGrove. For more information, please contact [email protected]. THE IMPACT OF PH ON THE STRUCTURE AND FUNCTION OF NEURAL CADHERIN A Thesis presented in partial fulfillment of requirements for the degree of Master of Science in the Department of Chemistry and Biochemistry The University of Mississippi by JARED JUNGLES July 2014 Copyright Jared M. Jungles 2014 ALL RIGHTS RESERVED ABSTRACT Neural (N-) cadherin is a transmembrane protein within adherens junctions that mediates cell-cell adhesion. It has 5 modular extracellular domains (EC1-EC5) that bind 3 calcium ions between each of the modules. Calcium binding is required for dimerization. N-cadherin is involved in diverse processes including tissue morphogenesis, excitatory synapse formation and dynamics, and metastasis of cancer. During neurotransmission and tumorigenesis, fluctuations in extracellular pH occur, causing tissue acidosis with associated physiological consequences. -
Properties of Cryogenic Insulants J
Cryogenics 38 (1998) 1063–1081 1998 Elsevier Science Ltd. All rights reserved Printed in Great Britain PII: S0011-2275(98)00094-0 0011-2275/98/$ - see front matter Properties of cryogenic insulants J. Gerhold Technische Universitat Graz, Institut fur Electrische Maschinen und Antriebestechnik, Kopernikusgasse 24, A-8010 Graz, Austria Received 27 April 1998; revised 18 June 1998 High vacuum, cold gases and liquids, and solids are the principal insulating materials for superconducting apparatus. All these insulants have been claimed to show fairly good intrinsic dielectric performance under laboratory conditions where small scale experiments in the short term range are typical. However, the insulants must be inte- grated into large scaled insulating systems which must withstand any particular stress- ing voltage seen by the actual apparatus over the full life period. Estimation of the amount of degradation needs a reliable extrapolation from small scale experimental data. The latter are reviewed in the light of new experimental data, and guidelines for extrapolation are discussed. No degradation may be seen in resistivity and permit- tivity. Dielectric losses in liquids, however, show some degradation, and breakdown as a statistical event must be scrutinized very critically. Although information for break- down strength degradation in large systems is still fragmentary, some thumb rules can be recommended for design. 1998 Elsevier Science Ltd. All rights reserved Keywords: dielectric properties; vacuum; fluids; solids; power applications; supercon- ductors The dielectric insulation design of any superconducting Of special interest for normal operation are the resis- power apparatus must be based on the available insulators. tivity, the permittivity, and the dielectric losses. -
Acid Dissociation Constant - Wikipedia, the Free Encyclopedia Page 1
Acid dissociation constant - Wikipedia, the free encyclopedia Page 1 Help us provide free content to the world by donating today ! Acid dissociation constant From Wikipedia, the free encyclopedia An acid dissociation constant (aka acidity constant, acid-ionization constant) is an equilibrium constant for the dissociation of an acid. It is denoted by Ka. For an equilibrium between a generic acid, HA, and − its conjugate base, A , The weak acid acetic acid donates a proton to water in an equilibrium reaction to give the acetate ion and − + HA A + H the hydronium ion. Key: Hydrogen is white, oxygen is red, carbon is gray. Lines are chemical bonds. K is defined, subject to certain conditions, as a where [HA], [A−] and [H+] are equilibrium concentrations of the reactants. The term acid dissociation constant is also used for pKa, which is equal to −log 10 Ka. The term pKb is used in relation to bases, though pKb has faded from modern use due to the easy relationship available between the strength of an acid and the strength of its conjugate base. Though discussions of this topic typically assume water as the solvent, particularly at introductory levels, the Brønsted–Lowry acid-base theory is versatile enough that acidic behavior can now be characterized even in non-aqueous solutions. The value of pK indicates the strength of an acid: the larger the value the weaker the acid. In aqueous a solution, simple acids are partially dissociated to an appreciable extent in in the pH range pK ± 2. The a actual extent of the dissociation can be calculated if the acid concentration and pH are known. -
A Comprehensive Self-Consistent Spectrophotometric Acidity Scale Of
A Comprehensive Self-Consistent Spectrophotometric Acidity Scale of Neutral Brønsted Acids in Acetonitrile Agnes Kütt †, Ivo Leito * †, Ivari Kaljurand †, Lilli Sooväli †, Vladislav M. Vlasov ‡, Lev M. Yagupolskii § and Ilmar A. Koppel † † Institute of Chemical Physics, Department of Chemistry, University of Tartu, Jakobi 2 Str., 51014 Tartu, Estonia. E-mail: [email protected]; Phone: +372 7 375 259; Fax: +372 7 375 264. ‡ Institute of Organic Chemistry, Siberian Branch of the Russian Academy of Sciences, Novosibirsk 630090, Russia § Institute of Organic Chemistry, Ukrainian National Academy of Sciences, Murmanskaya Str. 5, Kiev 02094, Ukraine. Abstract For the first time the self-consistent spectrophotometric acidity scale of neutral Brønsted acids in acetonitrile (AN) spanning 24 orders of magnitude of acidities is reported. The scale ranges from pKa value 3.7 to 28.1 in AN. The scale includes altogether 93 acids that are interconnected by 203 relative acidity measurements (∆pKa measurements). The scale 1 contains compounds with gradually changing acidities, including representatives from all the conventional families of OH (alcohols, phenols, carboxylic acids, sulfonic acids), NH (anilines, diphenylamines, disulfonimides) and CH acids (fluorenes, diphenylacetonitriles, phenylmalononitriles). The CH acids were particularly useful in constructing the scale because they do not undergo homo- or heteroconjugation processes and their acidities are rather insensitive to traces of water in the medium. The scale has been fully cross-validated: the relative acidity of any two acids on the scale can be found combining at least two independent sets of ∆pKa measurements. The consistency standard deviation of the scale is 0.03 pKa units. Comparison of acidities in many different media has been carried out and the structure-acidity relations are discussed. -
Determination of the Relative Permittivity, E′, of Methylbenzene
1056 J. Chem. Eng. Data 2008, 53, 1056–1065 Determination of the Relative Permittivity, E′, of Methylbenzene at Temperatures between (290 and 406) K and Pressures below 20 MPa with a Radio Frequency Re-Entrant Cavity and Evaluation of a MEMS Capacitor for the Measurement of E′ Mohamed E. Kandil and Kenneth N. Marsh Department of Chemical and Process Engineering, University of Canterbury, Christchurch, New Zealand Anthony R. H. Goodwin* Schlumberger Technology Corporation, 125 Industrial Boulevard, Sugar Land, Texas 77478 The relative electric permittivity of liquid methylbenzene has been determined with an uncertainty of 0.01 % from measurements of the resonance frequency of the lowest order inductive-capacitance mode of a re-entrant cavity (J. Chem. Thermodyn. 2005, 37, 684–691) at temperatures between (290 and 406) K and pressures below 20 MPa and at T ) 297 K with a MicroElectricalMechanical System (MEMS) interdigitated comb capacitor. For the re-entrant cavity, the working equations were a combination of the expressions reported by Hamelin et al. (ReV. Sci. Instrum. 1998, 69, 255-260) and a function to account for dilation of the resonator vessel walls with pressure that was determined by calibration with methane (J. Chem. Eng. Data 2007, 52, 1660–1671). The results were represented by an empirical equation reported by Owen and Brinkley (Liq. Phys. ReV. 1943, 64, 32–36) analogous to the Tait equation (Br. J. Appl. Phys. 1967, 18, 965–977) with a standard (k ) 1) uncertainty of 0.33 %. The values reported by Mospik (J. Chem. Phys. 1969, 50, 2559–2569) differed from the interpolating equation by <( 0.2 % at temperatures that overlap ours; extrapolating the smoothing expression to T ) 223 K, a temperature of 40 K below the lowest used for the measurements, provided values within ( 0.6 % of the data reported by Mospik. -
Electrical Properties of Polyethylene/Polypropylene Compounds for High-Voltage Insulation
energies Article Electrical Properties of Polyethylene/Polypropylene Compounds for High-Voltage Insulation Sameh Ziad Ahmed Dabbak 1, Hazlee Azil Illias 1,* ID , Bee Chin Ang 2, Nurul Ain Abdul Latiff 1 and Mohamad Zul Hilmey Makmud 1,3,* ID 1 Department of Electrical Engineering, Faculty of Engineering, University of Malaya, Kuala Lumpur 50603, Malaysia; [email protected] (S.Z.A.D.); [email protected] (N.A.A.L.) 2 Department of Chemical Engineering, Faculty of Engineering, University of Malaya, Kuala Lumpur 50603, Malaysia; [email protected] 3 Complex of Science and Technology, Faculty of Science and Natural Resources, University Malaysia Sabah, Kota Kinabalu 88400, Malaysia * Correspondence: [email protected] (H.A.I.); [email protected] (M.Z.H.M.); Tel.: +60-3-7967-4483 (H.A.I.) Received: 12 April 2018; Accepted: 30 May 2018; Published: 4 June 2018 Abstract: In high-voltage insulation systems, the most commonly used material is polymeric material because of its high dielectric strength, high resistivity, and low dielectric loss in addition to good chemical and mechanical properties. In this work, various polymer compounds were prepared, consisting of low-density polyethylene (LDPE), high-density polyethylene (HDPE), polypropylene (PP), HDPE/PP, and LDPE/PP polymer blends. The relative permittivity and breakdown strength of each sample types were evaluated. In order to determine the physical properties of the prepared samples, the samples were also characterized using differential scanning calorimetry (DSC). The results showed that the dielectric constant of PP increased with the increase of HDPE and LDPE content. The breakdown measurement data for all samples were analyzed using the cumulative probability plot of Weibull distribution.