Environmental Magnetic Susceptibility: Using the Bartington MS2 System, by John Dearing OM0409
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Magnetism, Magnetic Properties, Magnetochemistry
Magnetism, Magnetic Properties, Magnetochemistry 1 Magnetism All matter is electronic Positive/negative charges - bound by Coulombic forces Result of electric field E between charges, electric dipole Electric and magnetic fields = the electromagnetic interaction (Oersted, Maxwell) Electric field = electric +/ charges, electric dipole Magnetic field ??No source?? No magnetic charges, N-S No magnetic monopole Magnetic field = motion of electric charges (electric current, atomic motions) Magnetic dipole – magnetic moment = i A [A m2] 2 Electromagnetic Fields 3 Magnetism Magnetic field = motion of electric charges • Macro - electric current • Micro - spin + orbital momentum Ampère 1822 Poisson model Magnetic dipole – magnetic (dipole) moment [A m2] i A 4 Ampere model Magnetism Microscopic explanation of source of magnetism = Fundamental quantum magnets Unpaired electrons = spins (Bohr 1913) Atomic building blocks (protons, neutrons and electrons = fermions) possess an intrinsic magnetic moment Relativistic quantum theory (P. Dirac 1928) SPIN (quantum property ~ rotation of charged particles) Spin (½ for all fermions) gives rise to a magnetic moment 5 Atomic Motions of Electric Charges The origins for the magnetic moment of a free atom Motions of Electric Charges: 1) The spins of the electrons S. Unpaired spins give a paramagnetic contribution. Paired spins give a diamagnetic contribution. 2) The orbital angular momentum L of the electrons about the nucleus, degenerate orbitals, paramagnetic contribution. The change in the orbital moment -
(Public Pack)Agenda Document for Health & Wellbeing Board, 11/12/2018 17:30
Public Document Pack Health & Wellbeing Board Tuesday, 11th December, 2018 5.30 pm AGENDA 1. Welcome and Apologies 2. Minutes of the Meeting Held on 25th September 2018 Minutes 25th September 2018 3 - 8 3. Declarations of Interest 4. Public Questions To receive a Letter from Kate Davies OBE, Director of Health & Justice, Armed Forces and Sexual Assault services Commissioning, and Jackie Doyle-Price MP, Parliamentary Under Secretary FAO Chairs of Health and Wellbeing Boards 9 - 11 5. Start Well Annual Update (Jayne Ivory) 6. Pan Lancashire Health and Wellbeing Board (Dominic Harrison) 7. Joint Commissioning and Better Care Fund Update (Sayyed Osman) Joint Commissioning and Better Care Fund Update 12 - 17 8. Joint Strategic Needs Assessment Summary Review (Anne Cunningham) HWBB - JSNA Summary Review paper 18 - 73 Summary Review 2018 9. Action on Air Quality (Dominic Harrison) Air Quality for HWB 11th December 74 - 103 Air Quality and Public Health Report FINAL(2) Appendix 1 Appendix 2 L&C Air Quality Summit for HWB 10. Health and Wealth Report (Dominic Harrison) Health for Wealth (2018) NHSA-REPORT-7pages 104 - 110 Date Published: 4th December 2018 Harry Catherall, Chief Executive Agenda Item 2 BLACKBURN WITH DARWEN HEALTH AND WELLBEING BOARD MINUTES OF A MEETING HELD ON TUESDAY, 25TH SEPTEMBER 2018 PRESENT: Mohammed Khan (Chair) Councillors Maureen Bateson Brian Taylor Clinical Commissioning Group (CCG) Roger Parr Lay Members Joe Slater Vicky Shepherd Voluntary Sector Angela Allen Healthwatch Abdul Mulla Sayyed Osman Dominic Harrison Kenneth Barnsley Council Rabiya Gangreker Wendi Shepherd Jayne Ivory Council Officers Firoza Hafeji CCG Officers Dr Penny Morris Midland and Lancashire Commissioning Nicola Feeney Support Unit 1. -
Magnetism Some Basics: a Magnet Is Associated with Magnetic Lines of Force, and a North Pole and a South Pole
Materials 100A, Class 15, Magnetic Properties I Ram Seshadri MRL 2031, x6129 [email protected]; http://www.mrl.ucsb.edu/∼seshadri/teach.html Magnetism Some basics: A magnet is associated with magnetic lines of force, and a north pole and a south pole. The lines of force come out of the north pole (the source) and are pulled in to the south pole (the sink). A current in a ring or coil also produces magnetic lines of force. N S The magnetic dipole (a north-south pair) is usually represented by an arrow. Magnetic fields act on these dipoles and tend to align them. The magnetic field strength H generated by N closely spaced turns in a coil of wire carrying a current I, for a coil length of l is given by: NI H = l The units of H are amp`eres per meter (Am−1) in SI units or oersted (Oe) in CGS. 1 Am−1 = 4π × 10−3 Oe. If a coil (or solenoid) encloses a vacuum, then the magnetic flux density B generated by a field strength H from the solenoid is given by B = µ0H −7 where µ0 is the vacuum permeability. In SI units, µ0 = 4π × 10 H/m. If the solenoid encloses a medium of permeability µ (instead of the vacuum), then the magnetic flux density is given by: B = µH and µ = µrµ0 µr is the relative permeability. Materials respond to a magnetic field by developing a magnetization M which is the number of magnetic dipoles per unit volume. The magnetization is obtained from: B = µ0H + µ0M The second term, µ0M is reflective of how certain materials can actually concentrate or repel the magnetic field lines. -
Diamagnetism of Bulk Graphite Revised
magnetochemistry Article Diamagnetism of Bulk Graphite Revised Bogdan Semenenko and Pablo D. Esquinazi * Division of Superconductivity and Magnetism, Felix-Bloch-Institute for Solid State Physics, Faculty of Physics and Earth Sciences, University of Leipzig, Linnéstraße 5, 04103 Leipzig, Germany; [email protected] * Correspondence: [email protected]; Tel.: +49-341-97-32-751 Received: 15 October 2018; Accepted: 16 November 2018; Published: 22 November 2018 Abstract: Recently published structural analysis and galvanomagnetic studies of a large number of different bulk and mesoscopic graphite samples of high quality and purity reveal that the common picture assuming graphite samples as a semimetal with a homogeneous carrier density of conduction electrons is misleading. These new studies indicate that the main electrical conduction path occurs within 2D interfaces embedded in semiconducting Bernal and/or rhombohedral stacking regions. This new knowledge incites us to revise experimentally and theoretically the diamagnetism of graphite samples. We found that the c-axis susceptibility of highly pure oriented graphite samples is not really constant, but can vary several tens of percent for bulk samples with thickness t & 30 µm, whereas by a much larger factor for samples with a smaller thickness. The observed decrease of the susceptibility with sample thickness qualitatively resembles the one reported for the electrical conductivity and indicates that the main part of the c-axis diamagnetic signal is not intrinsic to the ideal graphite structure, but it is due to the highly conducting 2D interfaces. The interpretation of the main diamagnetic signal of graphite agrees with the reported description of its galvanomagnetic properties and provides a hint to understand some magnetic peculiarities of thin graphite samples. -
Magnetic Susceptibility Artefact on MRI Mimicking Lymphadenopathy: Description of a Nasopharyngeal Carcinoma Patient
1161 Case Report on Focused Issue on Translational Imaging in Cancer Patient Care Magnetic susceptibility artefact on MRI mimicking lymphadenopathy: description of a nasopharyngeal carcinoma patient Feng Zhao1, Xiaokai Yu1, Jiayan Shen1, Xinke Li1, Guorong Yao1, Xiaoli Sun1, Fang Wang1, Hua Zhou2, Zhongjie Lu1, Senxiang Yan1 1Department of Radiation Oncology, 2Department of Radiology, the First Affiliated Hospital, College of Medicine, Zhejiang University, Hangzhou 310003, China Correspondence to: Zhongjie Lu. Department of Radiation Oncology, the First Affiliated Hospital, College of Medicine, Zhejiang University, Hangzhou, Zhejiang 310003, China. Email: [email protected]; Senxiang Yan. Department of Radiation Oncology, the First Affiliated Hospital, College of Medicine, Zhejiang University, Hangzhou, Zhejiang 310003, China. Email: [email protected]. Abstract: This report describes a case involving a 34-year-old male patient with nasopharyngeal carcinoma (NPC) who exhibited the manifestation of lymph node enlargement on magnetic resonance (MR) images due to a magnetic susceptibility artefact (MSA). Initial axial T1-weighted and T2-weighted images acquired before treatment showed a round nodule with hyperintensity in the left retropharyngeal space that mimicked an enlarged cervical lymph node. However, coronal T2-weighted images and subsequent computed tomography (CT) images indicated that this lymph node-like lesion was an MSA caused by the air-bone tissue interface rather than an actual lymph node or another artefact. In addition, for the subsequent MR imaging (MRI), which was performed after chemoradiotherapy (CRT) treatment for NPC, axial MR images also showed an enlarged lymph node-like lesion. This MSA was not observed in a follow-up MRI examination when different MR sequences were used. -
Magnetism in Transition Metal Complexes
Magnetism for Chemists I. Introduction to Magnetism II. Survey of Magnetic Behavior III. Van Vleck’s Equation III. Applications A. Complexed ions and SOC B. Inter-Atomic Magnetic “Exchange” Interactions © 2012, K.S. Suslick Magnetism Intro 1. Magnetic properties depend on # of unpaired e- and how they interact with one another. 2. Magnetic susceptibility measures ease of alignment of electron spins in an external magnetic field . 3. Magnetic response of e- to an external magnetic field ~ 1000 times that of even the most magnetic nuclei. 4. Best definition of a magnet: a solid in which more electrons point in one direction than in any other direction © 2012, K.S. Suslick 1 Uses of Magnetic Susceptibility 1. Determine # of unpaired e- 2. Magnitude of Spin-Orbit Coupling. 3. Thermal populations of low lying excited states (e.g., spin-crossover complexes). 4. Intra- and Inter- Molecular magnetic exchange interactions. © 2012, K.S. Suslick Response to a Magnetic Field • For a given Hexternal, the magnetic field in the material is B B = Magnetic Induction (tesla) inside the material current I • Magnetic susceptibility, (dimensionless) B > 0 measures the vacuum = 0 material response < 0 relative to a vacuum. H © 2012, K.S. Suslick 2 Magnetic field definitions B – magnetic induction Two quantities H – magnetic intensity describing a magnetic field (Système Internationale, SI) In vacuum: B = µ0H -7 -2 µ0 = 4π · 10 N A - the permeability of free space (the permeability constant) B = H (cgs: centimeter, gram, second) © 2012, K.S. Suslick Magnetism: Definitions The magnetic field inside a substance differs from the free- space value of the applied field: → → → H = H0 + ∆H inside sample applied field shielding/deshielding due to induced internal field Usually, this equation is rewritten as (physicists use B for H): → → → B = H0 + 4 π M magnetic induction magnetization (mag. -
The Effects of Ultrafine Air Pollution Particles on Health” Session with Barbara Maher
11/19 RAPPORTEURSHIPS “FACING CLIMATE CHANGE” “THE EFFECTS OF ULTRAFINE AIR POLLUTION PARTICLES ON HEALTH” SESSION WITH BARBARA MAHER. 7th November 2019- Barbara Maher 11th session – Re-City: Facing Climate Change The effects of ultrafine air pollution particles on health Invited speaker: Barbara Maher, Lancaster University ______________________________________________________________________________ CONTENTS Biography 3 Summary 5 Nanoparticles are a threat to public health 5 Air pollution nanoparticles contribute to neurodegenerative diseases 5 Electric cars and green barriers to reduce pollution. 6 The effects of ultrafine air pollution particles on health 7 Airborne Particulate Matter 7 Ultrafine air pollution and the human brain 8 Location affects exposure 10 Potential solutions for reducing exposure to air pollution 11 You cannot manage what you do not measure 11 Roadside tree lines for reducing exposure to PM - The silver-birch tree experiment 13 Public transport 14 Filters to reduce air pollution 14 Raising awareness 14 Concluding remarks 15 References 15 1 7th November 2019- Barbara Maher 11th session – Re-City: Facing Climate Change This report is a synthesis of the debate with Dr. Barbara Maher in the conference series “Facing climate change”, organised by the Catalunya Europa Foundation as part of the Re-City project, in collaboration with BBVA. This session, entitled "The effects of ultrafine air pollution particles on health” consisted of a public lecture, a lunch-debate that brought together actors from the economic, social, political and business sector of Catalonia, and a meeting with academics. The activities were held in Barcelona at the Antoni Tàpies Foundation in November 2019. The content order along this report is thematic and does not represent the order in which it was presented by Dr. -
Condensed Matter Option MAGNETISM Handout 1
Condensed Matter Option MAGNETISM Handout 1 Hilary 2014 Radu Coldea http://www2.physics.ox.ac.uk/students/course-materials/c3-condensed-matter-major-option Syllabus The lecture course on Magnetism in Condensed Matter Physics will be given in 7 lectures broken up into three parts as follows: 1. Isolated Ions Magnetic properties become particularly simple if we are able to ignore the interactions between ions. In this case we are able to treat the ions as effectively \isolated" and can discuss diamagnetism and paramagnetism. For the latter phenomenon we revise the derivation of the Brillouin function outlined in the third-year course. Ions in a solid interact with the crystal field and this strongly affects their properties, which can be probed experimentally using magnetic resonance (in particular ESR and NMR). 2. Interactions Now we turn on the interactions! I will discuss what sort of magnetic interactions there might be, including dipolar interactions and the different types of exchange interaction. The interactions lead to various types of ordered magnetic structures which can be measured using neutron diffraction. I will then discuss the mean-field Weiss model of ferromagnetism, antiferromagnetism and ferrimagnetism and also consider the magnetism of metals. 3. Symmetry breaking The concept of broken symmetry is at the heart of condensed matter physics. These lectures aim to explain how the existence of the crystalline order in solids, ferromagnetism and ferroelectricity, are all the result of symmetry breaking. The consequences of breaking symmetry are that systems show some kind of rigidity (in the case of ferromagnetism this is permanent magnetism), low temperature elementary excitations (in the case of ferromagnetism these are spin waves, also known as magnons), and defects (in the case of ferromagnetism these are domain walls). -
Magnetic Susceptibility Artifacts in Gradient-Recalled Echo MR Imaging
1149 Magnetic Susceptibility Artifacts in Gradient-Recalled Echo MR Imaging Leo F. Czervionke1 Artifacts related to magnetic susceptibility differences between bone and soft tissue David L. Daniels 1 are prevalent on gradient-recalled echo images, particularly when long echo delay times Felix W . Wehrli2 are used. These susceptibility artifacts spatially distort and artifactually enlarge bone Leighton P. Mark1 contours. This can alter the apparent shape of the spinal canal and exaggerate the Lloyd E. Hendrix1 degree of spinal stenosis seen in patients with cervical spondylosis. The effects of magnetic susceptibility artifacts in gradient echo imaging were studied Julie A. Strandt1 1 in a phantom model and the results were correlated with MR images obtained in patients Alan L. Williams with cervical spondylosis. Victor M. Haughton1 Magnetic susceptibility is the ratio of the intensity of magnetization produced in a substance to the intensity of the applied magnetic field [1]. In other words, magnetic susceptibility is a measure of the extent a substance can be magnetized when placed in an external magnetic field . In spin echo imaging, ferromagnetic materials have high magnetic susceptibility, which alters the homogeneity of the field and results in geometric distortion of the image [2] . To a lesser extent such geometric distortion has been observed near air/tissue interfaces when gradient recalled echoes (GRE) are used [3]. Spatial variations in magnetic or diamagnetic susceptibility cause intrinsic magnetic field gradients across the imaging voxel. Spins subjected to these gradients lose phase coherence with a concomitant attenuation in signal intensity, leading to the well-known artifactual loss of signal intensity near air-containing sinus cavities. -
Divergent Drivers of Carbon Dioxide and Methane Dynamics in an Agricultural Coastal Floodplain: Post-Flood Hydrological and Biological Drivers
ResearchOnline@JCU This is the author-created version of the following work: Webb, Jackie R., Santos, Isaac R., Tait, Douglas R., Sippo, James Z., Macdonald, Ben C.T., Robson, Barbara, Maher, Damien T., and UNSPECIFIED (2016) Divergent drivers of carbon dioxide and methane dynamics in an agricultural coastal floodplain: post-flood hydrological and biological drivers. Chemical Geology, 440 pp. 313-325. Access to this file is available from: https://researchonline.jcu.edu.au/58052/ © 2016 Elsevier B.V. All rights reserved. Accepted Version: © 2016 Elsevier B.V. All rights reserved. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/ Please refer to the original source for the final version of this work: https://doi.org/10.1016/j.chemgeo.2016.07.025 ÔØ ÅÒÙ×Ö ÔØ Divergent drivers of carbon dioxide and methane dynamics in an agricultural coastal floodplain: post-flood hydrological and biological drivers Jackie R. Webb, Isaac R. Santos, Douglas R. Tait, James Z. Sippo, Ben C.T. Macdonald, Barbara Robson, Damien T. Maher PII: S0009-2541(16)30377-1 DOI: doi: 10.1016/j.chemgeo.2016.07.025 Reference: CHEMGE 18014 To appear in: Chemical Geology Received date: 24 March 2016 Revised date: 22 July 2016 Accepted date: 31 July 2016 Please cite this article as: Webb, Jackie R., Santos, Isaac R., Tait, Douglas R., Sippo, James Z., Macdonald, Ben C.T., Robson, Barbara, Maher, Damien T., Diver- gent drivers of carbon dioxide and methane dynamics in an agricultural coastal flood- plain: post-flood hydrological and biological drivers, Chemical Geology (2016), doi: 10.1016/j.chemgeo.2016.07.025 This is a PDF file of an unedited manuscript that has been accepted for publication. -
Efficient Experimental Design for Measuring Magnetic Susceptibility of Arbitrarily Shaped Materials by MRI
pISSN 2384-1095 iMRI 2018;22:141-149 https://doi.org/10.13104/imri.2018.22.3.141 eISSN 2384-1109 Efficient Experimental Design for Measuring Magnetic Susceptibility of Arbitrarily Shaped Materials by MRI Seon-ha Hwang, Seung-Kyun Lee Department of Biomedical Engineering, Sungkyunkwan University, Suwon, Korea Magnetic resonance imaging Center of Neuroscience Imaging Research, Institute for Basic Science, Suwon, Korea Purpose: The purpose of this study is to develop a simple method to measure magnetic susceptibility of arbitrarily shaped materials through MR imaging and numerical modeling. Original Article Materials and Methods: Our 3D printed phantom consists of a lower compartment filled with a gel (gel part) and an upper compartment for placing a susceptibility object (object part). The B0 maps of the gel with and without the object were reconstructed from phase images obtained in a 3T MRI scanner. Then, their difference Received: April 5, 2018 Revised: July 25, 2018 was compared with a numerically modeled B0 map based on the geometry of the Accepted: August 17, 2018 object, obtained by a separate MRI scan of the object possibly immersed in an MR- visible liquid. The susceptibility of the object was determined by a least-squares fit. Correspondence to: Results: A total of 18 solid and liquid samples were tested, with measured suscepti- Seung-Kyun Lee, Ph.D. bility values in the range of -12.6 to 28.28 ppm. To confirm accuracy of the method, Department of Biomedical Engineering, Sungkyunkwan independently obtained reference values were compared with measured susceptibility University, 2066, Seobu-ro, when possible. The comparison revealed that our method can determine susceptibility Jangan-gu, Suwon-si, Gyeonggi- within approximately 5%, likely limited by the object shape modeling error. -
Electromagnetic Fields and Energy
MIT OpenCourseWare http://ocw.mit.edu Haus, Hermann A., and James R. Melcher. Electromagnetic Fields and Energy. Englewood Cliffs, NJ: Prentice-Hall, 1989. ISBN: 9780132490207. Please use the following citation format: Haus, Hermann A., and James R. Melcher, Electromagnetic Fields and Energy. (Massachusetts Institute of Technology: MIT OpenCourseWare). http://ocw.mit.edu (accessed [Date]). License: Creative Commons Attribution-NonCommercial-Share Alike. Also available from Prentice-Hall: Englewood Cliffs, NJ, 1989. ISBN: 9780132490207. Note: Please use the actual date you accessed this material in your citation. For more information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms 9 MAGNETIZATION 9.0 INTRODUCTION The sources of the magnetic fields considered in Chap. 8 were conduction currents associated with the motion of unpaired charge carriers through materials. Typically, the current was in a metal and the carriers were conduction electrons. In this chapter, we recognize that materials provide still other magnetic field sources. These account for the fields of permanent magnets and for the increase in inductance produced in a coil by insertion of a magnetizable material. Magnetization effects are due to the propensity of the atomic constituents of matter to behave as magnetic dipoles. It is natural to think of electrons circulating around a nucleus as comprising a circulating current, and hence giving rise to a magnetic moment similar to that for a current loop, as discussed in Example 8.3.2. More surprising is the magnetic dipole moment found for individual electrons. This moment, associated with the electronic property of spin, is defined as the Bohr magneton e 1 m = ± ¯h (1) e m 2 11 where e/m is the electronic chargetomass ratio, 1.76 × 10 coulomb/kg, and 2π¯h −34 2 is Planck’s constant, ¯h = 1.05 × 10 joulesec so that me has the units A − m .