Basic Theoretical Physics: A Concise Overview P19 ppt

Basic Theoretical Physics: A Concise Overview P19 ppt

Basic Theoretical Physics: A Concise Overview P19 ppt

... (This exhausts all crystal classes). In the first case one is dealing with so-called optically uniaxial crystals, in the latter case with optically biaxial crystals. We have now arrived at the phenomenon ... c (s) long. .) 2 In some (mainly artificial) materials both ε and μ are negative, i.e., also n.These so-called left-handed materials have unusual optical properties. 3 To avoid any misunder...

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Basic Theoretical Physics: A Concise Overview P2 pptx

Basic Theoretical Physics: A Concise Overview P2 pptx

... Experiment; LiquefactionofAir 319 41.7 Adiabatic ExpansionofanIdealGas 324 42 Phase Changes, van der Waals Theory and Related Topics 327 42.1 VanderWaals Theory 327 42.2 Magnetic Phase Changes; The Arrott Equation. ... Quantum Mechanics: Retrospect and Prospect 293 38 Appendix: “Mutual Preparation Algorithm” for Quantum Cryptography 297 Part I Mechanics and Basic Relativity 4 1 Space and Ti...

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Basic Theoretical Physics: A Concise Overview P8 ppt

Basic Theoretical Physics: A Concise Overview P8 ppt

... considerably, as follows: Assume that all parameters reflect this left-right symmetry, i.e., the La- grangian L shall be invariant against permutation of the indices j =1and j = 3, such that the ... re- striction, because ω is a so-called axial vector 1 : For example, a right-handed rotation around the unit vector n with positive angular velocity ˙ϕ is identical to a rotation, also right...

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Basic Theoretical Physics: A Concise Overview P10 pptx

Basic Theoretical Physics: A Concise Overview P10 pptx

... ·(x 2 1 x 2 − x 3 2 3 ),whichservesasatypicalexampleofnon-integrability and “chaos” in a simple two-dimensional system; for ε = 0 the potential is no longer rotationally invariant, but has only discrete triangular symmetry. 92 ... have seen above, always simple, at least in principle. In contrast, for non-linear non-integrable systems chaotic behavior occurs. In most cases this behavior is...

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Basic Theoretical Physics: A Concise Overview P11 pptx

Basic Theoretical Physics: A Concise Overview P11 pptx

... which are measured and mapped by geophysicists, e.g., in mineral prospecting. As usual, for didactical reasons we distinguish between the inertial mass m t and the gravitational mass m s , although m s = ... the earth had the form of an exact sphere, and if the mass distribution were exactly spherical, then G 1 and G 2 would vanish, and G 3 ≡−g.The deviations correspond to gravitational anoma...

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Basic Theoretical Physics: A Concise Overview P13 ppt

Basic Theoretical Physics: A Concise Overview P13 ppt

... problem and on another important statement, which is that a harmonic function cannot have a local maximum or local minimum in the interior of an open region. For example, in the case of a local maximum ... Electrostatics and Magnetostatics 17.1.6 General Curvilinear, Spherical and Cylindrical Coordinates At this point it makes sense to include a short mathematical section on polar coo...

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Basic Theoretical Physics: A Concise Overview P15 pptx

Basic Theoretical Physics: A Concise Overview P15 pptx

... an infinity of different vector potentials A, but essentially they are all identical. If one adds an arbitrary gradient field to A, then curlA is not changed at all. A so-called gauge transformation: A ... dielectric constant ε between the plates. Let us transport an infinitesimal amount of charge 14 , δQ,fromthemetal plate at lower potential to that with the higher potential, where a cap...

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Basic Theoretical Physics: A Concise Overview P18 pptx

Basic Theoretical Physics: A Concise Overview P18 pptx

... Leiden had already established before Einstein that Maxwell’s equations, which are not invariant under a Galilean transformation, are invariant w.r.t. a Lorentz transformation –asitwaslater called ... results are similar. 20.8 Relativistic Invariance of Electrodynamics We have already seen in Part I that classical mechanics had to be amended as a result of Einstein’s theory of special r...

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Basic Theoretical Physics: A Concise Overview P21 pptx

Basic Theoretical Physics: A Concise Overview P21 pptx

... ε T of a classical harmonic oscillator at a Kelvin temperature T and k B is Boltz- mann’s constant. Rayleigh and Jeans’ law thus predicts that the energy of the radiation should increase indefinitely ... consider- able direct and indirect contact between many people at various places, are indeed equivalent, as we shall see below. Nowadays the standard way to present the subject – which w...

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Basic Theoretical Physics: A Concise Overview P24 pptx

Basic Theoretical Physics: A Concise Overview P24 pptx

... 244 28 Abstract Quantum Mechanics (Algebraic Methods) a) The operators ˆ J 2 and ˆ J z commute with each other, and are thus simul- taneously diagonalizable. b) The orthonormalized abstract eigenvectors ... that a generalized Fourier expansion of an arbitrary function f(ϑ, ϕ)is possible. Important spherical harmonics are listed in the following table (we repeat that the normalization facto...

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