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Chapter 10 Experimental Methods
Chapter 10 Experimental Methods 10.1Materials preparation 10.2 Magnetic fields 10.3 Atomic-scale magnetism 10.4 Domain-scale measurements 10.5 Bulk magnetization measurement 10.6 Excitations 10.7 Numerical methods TCD April 2007 1 10.1 Materials Preparation 10.1.1 Bulk material Metals: Melt in an arc furnaces or a rf induction furnace. Heat treat in a resistance furnace (controlled temperature or atmosphere. X-ray Diffractometer Arc A meltermorphous me Gloveboxtals are produced by rapid solidificaSQUIDtion magnetometer - melt spinning Insulators: Mill components e.g. CoO + Fe2O3 ! CoFe2O4 . Grind and fire nx Mix ions in solutions. Precipitate gel as a precusror. Crystals: seed temperature seed Bridgeman method Czochralski method TCD April 2007 2 10.1.2 Thin films Physical vapour deposition Substrate 400 - 1000 C source Evaporation: Thermal e-beam e.g. 10 kV, 1A Mean-free path " = 6/P "in mm, P in Pa. TCD April 2007 3 cap film substrate TCD April 2007 4 Pulsed-laser deposition (PLD) ns pulses of UV light ! 1 J cm2 on the target, ! 10 Hz. directed plume cos11# Growth rate ! 1 nm s-1 TCD April 2007 5 Molecular-beam epitaxy (MBE) Carried out in UHV 10-7 - 10-9 Pa Needed to avoid conamination of a slowly-growing film by residual gas. Time for a monolayer 1/2 2 $t = (12MkBT/M) /Pa e..g Oxygen a ! 0.2 nm, P = 10-5 Pa, $t ! 6 0s Growth rate < 0.2 nm s-1 • Franck-van der Merwe • Volmer-Weber • Strannsky-Krastanov TCD April 2007 6 10.1.3 Small particles TCD April 2007 7 TCD April 2007 8 Sputtering Use Ar gas, Ar+ ions are accelerated towards the cathode (target). -
08. Ampère and Faraday Darrigol (2000), Chap 1
08. Ampère and Faraday Darrigol (2000), Chap 1. A. Pre-1820. (1) Electrostatics (frictional electricity) • 1780s. Coulomb's description: ! Two electric fluids: positive and negative. ! Inverse square law: It follows therefore from these three tests, that the repulsive force that the two balls -- [which were] electrified with the same kind of electricity -- exert on each other, Charles-Augustin de Coulomb follows the inverse proportion of (1736-1806) the square of the distance."" (2) Magnetism: Coulomb's description: • Two fluids ("astral" and "boreal") obeying inverse square law. • No magnetic monopoles: fluids are imprisoned in molecules of magnetic bodies. (3) Galvanism • 1770s. Galvani's frog legs. "Animal electricity": phenomenon belongs to biology. • 1800. Volta's ("volatic") pile. Luigi Galvani (1737-1798) • Pile consists of alternating copper and • Charged rod connected zinc plates separated by to inner foil. brine-soaked cloth. • Outer foil grounded. • A "battery" of Leyden • Inner and outer jars that can surfaces store equal spontaeously recharge but opposite charges. themselves. 1745 Leyden jar. • Volta: Pile is an electric phenomenon and belongs to physics. • But: Nicholson and Carlisle use voltaic current to decompose Alessandro Volta water into hydrogen and oxygen. Pile belongs to chemistry! (1745-1827) • Are electricity and magnetism different phenomena? ! Electricity involves violent actions and effects: sparks, thunder, etc. ! Magnetism is more quiet... Hans Christian • 1820. Oersted's Experimenta circa effectum conflictus elecrici in Oersted (1777-1851) acum magneticam ("Experiments on the effect of an electric conflict on the magnetic needle"). ! Galvanic current = an "electric conflict" between decompositions and recompositions of positive and negative electricities. ! Experiments with a galvanic source, connecting wire, and rotating magnetic needle: Needle moves in presence of pile! "Otherwise one could not understand how Oersted's Claims the same portion of the wire drives the • Electric conflict acts on magnetic poles. -
The Faraday Effect
Faraday 1 The Faraday Effect Objective To observe the interaction of light and matter, as modified by the presence of a magnetic field, and to apply the classical theory of matter to the observations. You will measure the Verdet constant for several materials and obtain the value of e/m, the charge to mass ratio for the electron. Equipment Electromagnet (Atomic labs, 0028), magnet power supply (Cencocat. #79551, 50V-5A DC, 32 & 140 V AC, RU #00048664), gaussmeter (RFL Industries), High Intensity Tungsten Filament Lamp, three interference filters, volt-ammeter (DC), Nicol prisms (2), glass samples (extra dense flint (EDF), light flint (LF), Kigre), sample holder (PVC), HP 6235A Triple output power supply, HP 34401 Multimeter, Si photodiode detector. I. Introduction If any transparent solid or liquid is placed in a uniform magnetic field, and a beam of plane polarized light is passed through it in the direction parallel to the magnetic lines of force (through holes in the pole shoes of a strong electromagnet), it is found that the transmitted light is still plane polarized, but that the plane of polarization is rotated by an angle proportional to the field intensity. This "optical rotation" is called the Faraday rotation (or Farady effect) and differs in an important respect from a similar effect, called optical activity, occurring in sugar solutions. In a sugar solution, the optical rotation proceeds in the same direction, whichever way the light is directed. In particular, when a beam is reflected back through the solution it emerges with the same polarization as it entered before reflection. -
Arxiv:1603.08481V1 [Physics.Optics] 28 Mar 2016 Strong Localized Electromagnetic fields Associated with Plasmonic Resonances
Magneto-optical response in bimetallic metamaterials Evangelos Atmatzakis,1 Nikitas Papasimakis,1 Vassili Fedotov,1 Guillaume Vienne,2 and Nikolay I. Zheludev1, 3, ∗ 1Optoelectronics Research Centre and Centre for Photonic Metamaterials, University of Southampton, Southampton SO17 1BJ, United Kingdom 2School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore 639798 3The Photonics Institute and Centre for Disruptive Photonic Technologies, Nanyang Technological University, Singapore 637371 (Dated: October 15, 2018) We demonstrate resonant Faraday polarization rotation in plasmonic arrays of bimetallic nano- ring resonators consisting of Au and Ni sections. This metamaterial design allows to optimize the trade-off between the enhancement of magneto-optical effects and plasmonic dissipation. Although Ni sections correspond to as little as ∼ 6% of the total surface of the metamaterial, the resulting magneto-optically induced polarization rotation is equal to that of a continuous film. Such bimetallic metamaterials can be used in compact magnetic sensors, active plasmonic components and integrated photonic circuits. The ability to tailor light-matter interactions is equally important for the development of current and future tech- nologies (telecommunications, sensing, data storage), as well as for the study of the fundamental properties of matter (spectroscopy). A typical example involves the exploitation of magneto-optical (MO) effects, where quasistatic mag- netic fields can induce optical anisotropy in a material. This is a direct manifestation of the Zeeman effect, the splitting of electronic energy levels due to interactions between magnetic fields and the magnetic dipole moment associated with the orbital and spin angular momentum [1]. This energy splitting gives rise to numerous polarization phenomena, such as magnetically-induced birefringence and dichroism, which enable dynamic control over the polarization state of light. -
Energy Pioneers
Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Energy Pioneers The following pages will give an overview about famous people in history who studied energy and invented useful things we still use today. Read about these people then complete the matching activity on the last page. For more great energy resources visit: www.ConsumersEnergy.com/kids © 2015 Consumers Energy. All rights reserved. Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Thomas Edison (1847) Information comes from the Department of Energy, including sourced pictures. Source: Wikimedia Commons (Public Domain) Born in 1847. Not a very good student. Created many inventions including the phonograph (similar to a record player), the light bulb, the first power plant and the first movie camera. One of his most famous quotes is, “Invention is one percent inspiration and ninety-nine percent perspiration.” For more great energy resources visit: www.ConsumersEnergy.com/kids © 2015 Consumers Energy. All rights reserved. Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Marie Curie (1867) Information comes from the Department of Energy, including sourced pictures. Source: Nobel Foundation, Wikimedia Commons (Public Domain) Born in 1867. Learned to read at 4. There were no universities in her native Poland that accepted women, so she had to move to France to attend college. She, along with her husband, discovered the first radioactive element. In 1903, she was awarded the Nobel Prize in Physics for the discovery of radium. Marie Curie was the first woman to win a Nobel Prize in Physics. -
Faraday Rotation Measurement Using a Lock-In Amplifier Sidney Malak, Itsuko S
Faraday rotation measurement using a lock-in amplifier Sidney Malak, Itsuko S. Suzuki, and Masatsugu Sei Suzuki Department of Physics, State University of New York at Binghamton (Date: May 14, 2011) Abstract: This experiment is designed to measure the Verdet constant v through Faraday effect rotation of a polarized laser beam as it passes through different mediums, flint Glass and water, parallel to the magnetic field B. As the B varies, the plane of polarization rotates and the transmitted beam intensity is observed. The angle through which it rotates is proportional to B and the proportionality constant is the Verdet constant times the optical path length. The optical rotation of the polarized light can be understood circular birefringence, the existence of different indices of refraction for the left-circularly and right-circularly polarized light components. The linearly polarized light is equivalent to a combination of the right- and left circularly polarized components. Each component is affected differently by the applied magnetic field and traverse the system with a different velocity, since the refractive index is different for the two components. The end result consists of left- and right-circular components that are out of phase and whose superposition, upon emerging from the Faraday rotation, is linearly polarized light with its plane of polarization rotated relative to its original orientation. ________________________________________________________________________ Michael Faraday, FRS (22 September 1791 – 25 August 1867) was an English chemist and physicist (or natural philosopher, in the terminology of the time) who contributed to the fields of electromagnetism and electrochemistry. Faraday studied the magnetic field around a conductor carrying a DC electric current. -
Notes on Corona-Resistant Antennas for High-Voltage Sensing Applications
Notes on Corona-Resistant Antennas for High-Voltage Sensing Applications Prof. Gregory D. Durgin, Marcin Morys August 13, 2018 1 Introduction Within emerging smart grid technologies, there is a gaping hole in scientific knowledge regarding design, modeling, and characterization of radio antennas in high-voltage environments. Specifically, useful quantitative models do not exist for describing the dynamic physics of high-voltage AC corona plasmas and their influence on radiating structures; as a result, little guidance is available for the design and measurement of communication antennas that resist this phenomenon. It has long been understood that high-voltages produce severe compatibility and noise issues for radio communications [Juh08]. Only recently, however, has the effect of corona shielding been measured and shown to impair UHF and microwave communication devices that operate at high- voltage line potentials [Val10]. Valenta, et. al. measured a 10 dB drop in the 5.8 GHz received power from an antenna operating at 100 kV line-to-ground AC potential [Val10]. This drop in received power was due to the surrounding corona plasma, an invisible Faraday cage that reflects and attenuates radio signals as well as de-tunes and distorts the antenna that it encapsulates. Antenna designs that resist this corona shielding are critical for wireless sensors that monitor and protect the national power grid. 2 Review of High-Voltage Corona In this section, we review the basic physics of AC corona plasmas and preliminary results on their influence on radio communications using line-potential antennas. 2.1 Plasma Effects on Communications The influence of plasmas on radio communications has been extensively studied for ionospheric propagation. -
Quantum Faraday Effect
Propagation of photons along the direction of the magnetic field. Quantum Faraday Effect. MsC. Lidice Cruz Rodríguez * Dra. Aurora Pérez Martínez ** Dra. Elizabeth Rodríguez Querts ** Dr. Hugo Pérez Rojas ** * Physics Faculty, Havana University ** Institute of Cybernetic, Mathematics and Physics STARS2015-SMFNS2015 Outline 1. Introduction, Faraday rotation angle. 2. Propagation of photons along the direction of the magnetic field . Quantum Faraday Effect, initial results . Solution of the dispersion equation near the thresholds. 3. Diluted gas: magnetosphere of neutron stars. Quantum Faraday Effect. Solution of the dispersion equation near the thresholds. 4. Summary. 5. Work in progress. Faraday Effect, our initial motivation It is well known that an electromagnetic wave propagating through a medium in an ambient magnetic field suffers Faraday rotation. Classical explanation of the phenomenon: birefringence of the medium Astrophysical applications!!!!!! . Measurements of the magnetic field in the interstellar medium. Particle density in the ionosphere . Difference between the amount of matter and antimatter However, in most of papers the amount of Faraday rotation is derived in a non relativistic regime and for a non degenerated medium. Faraday Effect, our initial motivation However, in most of papers the amount of Faraday rotation is derived in a non relativistic regime and for a non degenerated medium. But in the magnetosphere of neutron stars degenerate plasma Faraday Effect, our initial motivation However, in most of papers the amount of Faraday rotation is derived in a non relativistic regime and for a non degenerated medium. But in the magnetosphere of neutron stars degenerate plasma Faraday rotation in graphene-like systems. J. Appl. Phys. 113, 17B529 (2013) Faraday rotation has been reported in graphene, we use QFT, to describe the astrophysical background and also, graphene-like systems. -
Lab on Faraday Rotation
Faraday Rotation Tatsuya Akiba∗ Truman State University Department of Physics (Dated: March 6, 2019) This paper reports the results of analyzing the Faraday rotation effect of SF-59 glass subject to a magnetic field generated by current through a solenoid. We verify Malus' Law to determine the orientation of the first polarizer. We set the nominal angle at an optimal φ = 45◦ to make relative intensity measurements at various magnetic field strengths. The relative intensity is measured using a photo diode and a simple circuit that allows for voltage readout. The exact magnetic field strength generated by a current through a solenoid of finite length is calculated and used to compute magnetic field strengths at various currents. A plot of the magnetic field strength integrated over the length of the optical material against the Faraday rotation angle is produced and a linear fit is obtained. The experimental value of the Verdet constant was obtained from the slope of the linear fit, and compared to two theoretical values: one provided by the manufacturer and one predicted by the dispersion relation. I. INTRODUCTION of known polarization state through an optical material in a magnetic field to obtain an experimental value of Faraday rotation is a magneto-optic effect that causes the Verdet constant. The magnetic field is generated by the polarization vector of light to rotate as it passes a solenoid, and we control the magnetic field strength by through an optical material in an external magnetic field controlling the current passing through the solenoid. The [1]. First discovered by Michael Faraday in 1845, it was laser passes through an initial polarizer to set the light the first experimental evidence linking light to magnetic to a particular linear polarization, then goes through the phenomena [2]. -
Historical Perspective of Electricity
B - Circuit Lab rev.1.04 - December 19 SO Practice - 12-19-2020 Just remember, this test is supposed to be hard because everyone taking this test is really smart. Historical Perspective of Electricity 1. (1.00 pts) The first evidence of electricity in recorded human history was… A) in 1752 when Ben Franklin flew his kite in a lightning storm. B) in 1600 when William Gilbert published his book on magnetism. C) in 1708 when Charles-Augustin de Coulomb held a lecture stating that two bodies electrified of the same kind of Electricity exert force on each other. D) in 1799 when Alessandro Volta invented the voltaic pile which proved that electricity could be generated chemically. E) in 1776 when André-Marie Ampère invented the electric telegraph. F) about 2500 years ago when Thales of Miletus noticed that a piece of amber attracted straw or feathers when he rubbed it with cloth. 2. (3.00 pts) The word electric… (Mark ALL correct answers) A) was first used in printed text when it was published in William Gilber’s book on magnetism. B) comes from the Greek word ήλεκτρο (aka “electron”) meaning amber. C) adapted the meaning “charged with electricity” in the 1670s. D) was first used by Nicholas Callen in 1799 to describe mail transmitted over telegraph wires, “electric-mail” or “email”. E) was cast in stone by Greek emperor Julius Caesar when he knighted Archimedes for inventing the electric turning lathe. F) was first used by Michael Faraday when he described electromagnetic induction in 1791. 3. (5.00 pts) Which five people, who made scientific discoveries related to electricity, were alive at the same time? (Mark ALL correct answers) A) Charles-Augustin de Coulomb B) Alessandro Volta C) André-Marie Ampère D) Georg Simon Ohm E) Michael Faraday F) Gustav Robert Kirchhoff 4. -
Michael Faraday
Michael Faraday The credit for generating electric current on a practical scale goes to the famous English scientist, Michael Faraday. Faraday was greatly interested in the invention of the electro- magnet, but his brilliant mind took earlier experiments still further. If electricity could produce magnetism, why couldn’t magnetism produce electricity? In 1831, Faraday found the solution. Electricity could be produced through magnetism by motion. He discovered that when a magnet was moved inside a coil of copper wire, a tiny electric current flows through the wire. He discovered, in essence, the first method of generating electricity by means of motion in a magnetic field, yet Otto Von Guericke made the first electrical machine, the frictional machine, by which a glass ball of sulphur became electrified by rotating rubber. Davy, who had the greatest influence on Faraday’s thinking, had shown in 1807 that the metals sodium and potassium can be precipitated from their compounds by an electric current, a process known as ELECTROLYSIS. Faraday’s vigorous pursuit of these experiments led in 1834 to what became known as Faraday’s laws of electrolysis. Faraday’s research into electricity and electrolysis was guided by the belief that electricity is only one of the many manifestations of the unified forces of nature, which included heat, light, magnetism, and chemical affinity. Although this idea was erroneous, it led him into the field of electromagnetism (see MAGNETISM), which was still in its infancy. In 1785, Charles Coulomb had been the first to demonstrate the manner in which electric charges repel one another, and it was not until 1820 that Hans Christian OERSTED and Andre Marie AMPERE discovered that an electric current produces a magnetic field. -
Metamaterials with Magnetism and Chirality
1 Topical Review 2 Metamaterials with magnetism and chirality 1 2;3 4 3 Satoshi Tomita , Hiroyuki Kurosawa Tetsuya Ueda , Kei 5 4 Sawada 1 5 Graduate School of Materials Science, Nara Institute of Science and Technology, 6 8916-5 Takayama, Ikoma, Nara 630-0192, Japan 2 7 National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, 8 Japan 3 9 Advanced ICT Research Institute, National Institute of Information and 10 Communications Technology, Kobe, Hyogo 651-2492, Japan 4 11 Department of Electrical Engineering and Electronics, Kyoto Institute of 12 Technology, Matsugasaki, Sakyo, Kyoto 606-8585, Japan 5 13 RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan 14 E-mail: [email protected] 15 November 2017 16 Abstract. This review introduces and overviews electromagnetism in structured 17 metamaterials with simultaneous time-reversal and space-inversion symmetry breaking 18 by magnetism and chirality. Direct experimental observation of optical magnetochiral 19 effects by a single metamolecule with magnetism and chirality is demonstrated 20 at microwave frequencies. Numerical simulations based on a finite element 21 method reproduce well the experimental results and predict the emergence of giant 22 magnetochiral effects by combining resonances in the metamolecule. Toward the 23 magnetochiral effects at higher frequencies than microwaves, a metamolecule is 24 miniaturized in the presence of ferromagnetic resonance in a cavity and coplanar 25 waveguide. This work opens the door to the realization of a one-way mirror and 26 synthetic gauge fields for electromagnetic waves. 27 Keywords: metamaterials, symmetry breaking, magnetism, chirality, magneto-optical 28 effects, optical activity, magnetochiral effects, synthetic gauge fields 29 Submitted to: J.