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physics cos 2011-2012
physics cos 2011-2012

C:\exams\June\June_06\physics\final\Physics 3204 June 2006.wpd
C:\exams\June\June_06\physics\final\Physics 3204 June 2006.wpd

Modern Physics
Modern Physics

structure and properties of severe deformed nanocomposite
structure and properties of severe deformed nanocomposite

... mechanism of niobium fibers, is forming of knife-like boundaries that are the result of propagation of powerful disclinations. In that way on the defined stage of drawing structure with 10-20 0 fragment disorientation angle is formed in niobium fibers. At that time strong internal elastic deformatio ...
FB FB FB
FB FB FB

... 14. A rod of mass M and radius R rests on two parallel rails (see figure below) that are d apart and L long. The rod carries a current of I in the direction shown and rolls along the rails without slipping. A uniform magnetic field of magnitude B is directed perpendicular to the rod and the rails. ...
PPT
PPT

Name:
Name:

Chapter 5 - Magnetostatics
Chapter 5 - Magnetostatics

akdeniz university faculty of engineering 2013
akdeniz university faculty of engineering 2013

if on the Internet, Press  on your browser to
if on the Internet, Press on your browser to

Chapter 1: Matter, Measurement and Problem Solving
Chapter 1: Matter, Measurement and Problem Solving

... HOMEWORK: ...
Microwave near-field scanning
Microwave near-field scanning

... Microwave scanning probes for local characterization of conducting and insulating films attract considerable interest since they are contactless, versatile, and provide high spatial resolution. Recently several microwave scanning probes have been developed, namely coaxial tip [1], slot aperture [2], ...
Week 10 Thursday
Week 10 Thursday

... Note that the Earth’s “North Pole” is really a south magnetic pole, as the north ends of magnets are attracted to it. ...
OdyNOTESki E and M
OdyNOTESki E and M

... 1) Electromagnetic Induction – Production of electricity caused by motion between a Magnetic field and a conductor that cuts through the flux lines 2) Faraday’s Law – Changing magnetic fields create an electric potential in a conductor a) 3) Lenz’s Law – An induced emf in a wire loop or coil has a d ...
Carrier Concentrations
Carrier Concentrations

... Two-dimensional representation of an Individual Si atom. Elemental semiconductors Valence ...
tron vmk
tron vmk

... Here S1 1 = Qk + w 0 • When ~ « 1, this equation leads to the wellknown spin-wave spectrumC1J, which is hardly affected by the electric field, and to two strongly attenuated branches of oscillations. When ~ » 1 we obtain high-frequency oscillations ±Q 1 [ 1] and two low-frequency oscillations: ...
Slide 1
Slide 1

... can be expressed in small whole numbers ...
Document
Document

... edition. John Willey and Sons, Inc. Alonso M. and Finn E.J. (1992). Physics, AddisonWesley Publishing Company Hecht, E. (2000). Physics. Calculus, Second Edition. ...
Electromagnetic Induction
Electromagnetic Induction

... Therefore the change in magnetic flux per time is equal to, assuming the angle is zero: ...
RIGHT HAND RULE
RIGHT HAND RULE

SUGGESTED SOLUTIONS FOR TUTORIAL 6
SUGGESTED SOLUTIONS FOR TUTORIAL 6

... (a) An electric field, E is added to the magnetic field so that the proton can move in straight line without any deflection. Show the direction of E. (b) Derive an equation for the electric field, E. (c) If an electron with the same velocity, v enters the same magnetic field and electric field, wha ...
Universal Law of Gravitation Problems
Universal Law of Gravitation Problems

... (b) Calculate the gravitational force between them. (c) Which force is mainly responsible for the electron’s circular motion? (d) Calculate the speed and period of the electron in its orbit around the proton. 7. Two point charges, +4.0 x 10-5 C and –1.8 x 10-5 C, are placed 24 cm apart. What is the ...
10 ≥ t 137 ≈ e cħ He re − mp vm E 2 2 1
10 ≥ t 137 ≈ e cħ He re − mp vm E 2 2 1

... element has ninety two protons. Towards the end of 1945 all these ninety two elements were filled in Mendeleev’s periodic table. The first artificial radioactive element with atomic number (Z=93) was discovered by Edwin McMillan and Philip H. Abelson in the year 1940 in Berkeley, California. It was ...
CHAPTER 5
CHAPTER 5

Background 2
Background 2

... suitable to explain the structure of water and the interaction of magnetic fields with molecules in aqueous solutions. The first one - due to W.G. Armstrong (1898)– shows that a water bridge between containers of water can rise when a high electric field is applied. The second one – due to M.N. Zhad ...
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Condensed matter physics



Condensed matter physics is a branch of physics that deals with the physical properties of condensed phases of matter. Condensed matter physicists seek to understand the behavior of these phases by using physical laws. In particular, these include the laws of quantum mechanics, electromagnetism and statistical mechanics.The most familiar condensed phases are solids and liquids, while more exotic condensed phases include the superconducting phase exhibited by certain materials at low temperature, the ferromagnetic and antiferromagnetic phases of spins on atomic lattices, and the Bose–Einstein condensate found in cold atomic systems. The study of condensed matter physics involves measuring various material properties via experimental probes along with using techniques of theoretical physics to develop mathematical models that help in understanding physical behavior.The diversity of systems and phenomena available for study makes condensed matter physics the most active field of contemporary physics: one third of all American physicists identify themselves as condensed matter physicists, and the Division of Condensed Matter Physics is the largest division at the American Physical Society. The field overlaps with chemistry, materials science, and nanotechnology, and relates closely to atomic physics and biophysics. Theoretical condensed matter physics shares important concepts and techniques with theoretical particle and nuclear physics.A variety of topics in physics such as crystallography, metallurgy, elasticity, magnetism, etc., were treated as distinct areas, until the 1940s when they were grouped together as solid state physics. Around the 1960s, the study of physical properties of liquids was added to this list, forming the basis for the new, related specialty of condensed matter physics. According to physicist Phil Anderson, the term was coined by him and Volker Heine when they changed the name of their group at the Cavendish Laboratories, Cambridge from ""Solid state theory"" to ""Theory of Condensed Matter"" in 1967, as they felt it did not exclude their interests in the study of liquids, nuclear matter and so on. Although Anderson and Heine helped popularize the name ""condensed matter"", it had been present in Europe for some years, most prominently in the form of a journal published in English, French, and German by Springer-Verlag titled Physics of Condensed Matter, which was launched in 1963. The funding environment and Cold War politics of the 1960s and 1970s were also factors that lead some physicists to prefer the name ""condensed matter physics"", which emphasized the commonality of scientific problems encountered by physicists working on solids, liquids, plasmas, and other complex matter, over ""solid state physics"", which was often associated with the industrial applications of metals and semiconductors. The Bell Telephone Laboratories was one of the first institutes to conduct a research program in condensed matter physics.References to ""condensed"" state can be traced to earlier sources. For example, in the introduction to his 1947 ""Kinetic theory of liquids"" book, Yakov Frenkel proposed that ""The kinetic theory of liquids must accordingly be developed as a generalization and extension of the kinetic theory of solid bodies"". As a matter of fact, it would be more correct to unify them under the title of ""condensed bodies"".
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