| Element name | Element symbol | Atomic number |
| Actinium | Ac | 89 |
| Aluminium | Al | 13 |
| Americium | Am | 95 |
| Antimony | Sb | 51 |
| Argon | Ar | 18 |
| Arsenic | As | 33 |
| Astatine | At | 85 |
| Barium | Ba | 56 |
| Berkelium | Bk | 97 |
| Beryllium | Be | 4 |
| Bismuth | Bi | 83 |
| Bohrium | Bh | 107 |
| Boron | B | 5 |
| Bromine | Br | 35 |
| Cadmium | Cd | 48 |
| Caesium | Cs | 55 |
| Calcium | Ca | 20 |
| Californium | Cf | 98 |
| Carbon | C | 6 |
| Cerium | Ce | 58 |
| Chlorine | Cl | 17 |
| Chromium | Cr | 24 |
| Cobalt | Co | 27 |
| Copernicium | Cn | 112 |
| Copper | Cu | 29 |
| Curium | Cm | 96 |
| Darmstadtium | Ds | 110 |
| Dubnium | Db | 105 |
| Dysprosium | Dy | 66 |
| Einsteinium | Es | 99 |
| Erbium | Er | 68 |
| Europium | Eu | 63 |
| Fermium | Fm | 100 |
| Flerovium | Fl | 114 |
| Fluorine | F | 9 |
| Francium | Fr | 87 |
| Gadolinium | Gd | 64 |
| Gallium | Ga | 31 |
| Germanium | Ge | 32 |
| Gold | Au | 79 |
| Hafnium | Hf | 72 |
| Hassium | Hs | 108 |
| Helium | He | 2 |
| Holmium | Ho | 67 |
| Hydrogen | H | 1 |
| Indium | In | 49 |
| Iodine | I | 53 |
| Iridium | Ir | 77 |
| Iron | Fe | 26 |
| Krypton | Kr | 36 |
| Lanthanum | La | 57 |
| Lawrencium | Lr | 103 |
| Lead | Pb | 82 |
| Lithium | Li | 3 |
| Livermorium | Lv | 116 |
| Lutetium | Lu | 71 |
| Magnesium | Mg | 12 |
| Manganese | Mn | 25 |
| Meitnerium | Mt | 109 |
| Mendelevium | Md | 101 |
| Mercury | Hg | 80 |
| Molybdenum | Mo | 42 |
| Neodymium | Nd | 60 |
| Neon | Ne | 10 |
| Neptunium | Np | 93 |
| Nickel | Ni | 28 |
| Niobium | Nb | 41 |
| Nitrogen | N | 7 |
| Nobelium | No | 102 |
| Osmium | Os | 76 |
| Oxygen | O | 8 |
| Palladium | Pd | 46 |
| Phosphorus | P | 15 |
| Platinum | Pt | 78 |
| Plutonium | Pu | 94 |
| Polonium | Po | 84 |
| Potassium | K | 19 |
| Praseodymium | Pr | 59 |
| Promethium | Pm | 61 |
| Protactinium | Pa | 91 |
| Radium | Ra | 88 |
| Radon | Rn | 86 |
| Rhenium | Re | 75 |
| Rhodium | Rh | 45 |
| Roentgenium | Rg | 111 |
| Rubidium | Rb | 37 |
| Ruthenium | Ru | 44 |
| Rutherfordium | Rf | 104 |
| Samarium | Sm | 62 |
| Scandium | Sc | 21 |
| Seaborgium | Sg | 106 |
| Selenium | Se | 34 |
| Silicon | Si | 14 |
| Silver | Ag | 47 |
| Sodium | Na | 11 |
| Strontium | Sr | 38 |
| Sulfur | S | 16 |
| Tantalum | Ta | 73 |
| Technetium | Tc | 43 |
| Tellurium | Te | 52 |
| Terbium | Tb | 65 |
| Thallium | Tl | 81 |
| Thorium | Th | 90 |
| Thulium | Tm | 69 |
| Tin | Sn | 50 |
| Titanium | Ti | 22 |
| Tungsten | W | 74 |
| Ununoctium | Uuo | 118 |
| Ununpentium | Uup | 115 |
| Ununseptium | Uus | 117 |
| Ununtrium | Uut | 113 |
| Uranium | U | 92 |
| Vanadium | V | 23 |
| Xenon | Xe | 54 |
| Ytterbium | Yb | 70 |
| Yttrium | Y | 39 |
| Zinc | Zn | 30 |
| Zirconium | Zr | 40 |
THE CHEMICAL ELEMENTS SORTED BY NAME IN AN ALPHABETICAL ORDER
CHARGE-COUPLED DEVICES (CCD)
A charge-coupled device (CCD) is a kind of device that is widely used for such
diverse applications as computer memories and image recording. The charge-coupled
device employs an array of metal-oxide contacts, as illustrated in Fig. 14.25. Assuming a
p-type semiconductor, each of them has a positive imposed potential to create an
inversion layer just inside the semiconductor.
Scattering of electromagnetic waves
The third important phenomenon that affects wave propagation is scattering.
Scattering results from what are, effectively, elastic collisions between the photons of the
incident beam and particles or heterogeneities in the material, causing the photons to be
deflected, or scattered, so that they propagate in some new direction. Scattering subtracts
intensity from the transmitted wave and contributes to its attenuation. The material
property that governs scattering is called the scattering coefficient, S. A wave that is
transmitted through a medium with scattering coefficient, S, is attenuated according to
the relation
Optical glass and gemstones
Optical glasses serve a number of different functions. Some, like window glass,
are intended to maximize transparency. Others, like "crystal" glassware, are intended
both to reveal what is contained and to add a certain luster to it. Still other glasses are
colored, often for cosmetic reasons, but sometimes to filter light, as in tinted sunglasses
and windshields.
Ferrimagnetism
Ferrimagnetism occurs in polyatomic compounds that contain ions with different
core magnetic moments. The core magnetic moments order in an antiferromagnetic
pattern, but, since alternate moments differ in magnitude, they do not cancel. The
material has a net ferromagnetic moment.
The most important of the ferrimagnetic materials are the ferrites , which have the composition MFe2O4, where M is a divalent metal ion. The most familiar of these is magnetite, Fe3O4, which is the historic lodestone that was the first known ferromagnetic material. The ferrites crystallize in the spinel structure. While I shall not attempt to draw it here, it is a relatively simple structure that has a close-packed, FCC arrangement of oxygen atoms with metal ions in 1/2 of the octahedral interstitial sites and 1/8 of the tetrahedral sites. Since there are 2 tetrahedral and 1 octahedral void per oxygen ion, there are 2 metal ions in octahedral sites for each ion in a tetrahedral site. The magnetic order is an antiferromagnetic order in which the moments of all of the octahedral ions are oriented in one direction, while those of all the tetrahedral ions are oriented in the opposite direction.
The most important of the ferrimagnetic materials are the ferrites , which have the composition MFe2O4, where M is a divalent metal ion. The most familiar of these is magnetite, Fe3O4, which is the historic lodestone that was the first known ferromagnetic material. The ferrites crystallize in the spinel structure. While I shall not attempt to draw it here, it is a relatively simple structure that has a close-packed, FCC arrangement of oxygen atoms with metal ions in 1/2 of the octahedral interstitial sites and 1/8 of the tetrahedral sites. Since there are 2 tetrahedral and 1 octahedral void per oxygen ion, there are 2 metal ions in octahedral sites for each ion in a tetrahedral site. The magnetic order is an antiferromagnetic order in which the moments of all of the octahedral ions are oriented in one direction, while those of all the tetrahedral ions are oriented in the opposite direction.
What is Magnetostriction
Almost all ferromagnetic materials exhibit the phenomenon of magnetostriction in
which the material spontaneously expands or contracts in response to a magnetic field.
The phenomenon is due to the fact that the material can ordinarily increase its local
magnetization slightly by expanding or contracting to optimize the separation of its ion
cores. The sign and magnitude of the magnetostriction depends on the material.
Magnetostriction is a useful property that permits a time-varying magnetic field to be converted to a mechanical signal, or vice versa. It is used in transducers and in small speakers for consumer electronics, among many other applications. While nickel was the principle material of choice for early magnetostrictive devices, ferrites are often preferred today since their high resistance minimizes losses due to induced electrical currents.
Magnetostriction is a useful property that permits a time-varying magnetic field to be converted to a mechanical signal, or vice versa. It is used in transducers and in small speakers for consumer electronics, among many other applications. While nickel was the principle material of choice for early magnetostrictive devices, ferrites are often preferred today since their high resistance minimizes losses due to induced electrical currents.
The magnetic behavior of a type II superconductor
The negative interfacial tension between the normal and superconducting phases
is responsible for the unique magnetic behavior of type II superconductors. When ß < 0
the material is driven to create as much interface as possible, and can do so by spontaneously
subdividing into a two-phase mixture. The two-phase mixture persists over a
range of conditions (in our case, a range of H to either side of Hc) since the subvolumes
of the high-energy phase can be made so small that the interfacial tension dominates the
free energy. There are, however, limits on how small the regions of normal metal can be.
These set upper and lower bounds on the magnetic field that produces the mixed state.
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