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Second-Order Differential Equations
Second-Order Differential Equations

CHAPTER 17 - The Sine and Cosine Function
CHAPTER 17 - The Sine and Cosine Function

... remember being presented with a circle, called the Unit Circle for reasons soon to be seen. In this circle any point on it had the co-ordinates ( Cos Ø, Sin Ø) where x= Cos Ø and y= Sin Ø. Often times the circle added more confusion to your understanding of Sines and Cosines. At such a point your mi ...
Section 13.10 Interference of Waves
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... interferes with a second wave of amplitude 0.20 m traveling in the same direction. What are (a) the largest and (b) the smallest resultant amplitudes that can occur, and under what conditions will these maxima and minima arise? Additional Problems ...
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Statistical Physics
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... In this module we are focusing on the system of macroscopic particles and we study the statistical description of systems in terms of probability and the behavior of the density of state which help to measure the macroscopic parameters like heat, absolute temperature and entropy. As a result of this ...
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... will be dealt with in the lectures. Furthermore, there will be demonstration experiments during the  lectures.   We cannot cover everything you need to know for the final test in the lectures. We can only give  summaries of the concepts covered. Lectures should therefore be regarded as a starting po ...
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... In large atoms (e.g., Uranium), the nucleus can be unstable to the emission of an alpha particle (a He nucleus). This form of radioactivity is a tunneling process, involving transmission of the alpha particle from a low-energy valley through a barrier to a lower energy outside. ...
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... A long-standing problem in the kinetic theory is how to effectively describe, within the framework of the Boltzmann equation, the evolution of a system of particles interacting with long range forces, especially with Coulomb forces. Many interesting methods (see [9, 10] and cited references therein) ...
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The interpretation of the Einstein-Rupp experiments and their

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Wave packet



In physics, a wave packet (or wave train) is a short ""burst"" or ""envelope"" of localized wave action that travels as a unit. A wave packet can be analyzed into, or can be synthesized from, an infinite set of component sinusoidal waves of different wavenumbers, with phases and amplitudes such that they interfere constructively only over a small region of space, and destructively elsewhere. Each component wave function, and hence the wave packet, are solutions of a wave equation. Depending on the wave equation, the wave packet's profile may remain constant (no dispersion, see figure) or it may change (dispersion) while propagating.Quantum mechanics ascribes a special significance to the wave packet; it is interpreted as a probability amplitude, its norm squared describing the probability density that a particle or particles in a particular state will be measured to have a given position or momentum. The wave equation is in this case the Schrödinger equation. It is possible to deduce the time evolution of a quantum mechanical system, similar to the process of the Hamiltonian formalism in classical mechanics. The dispersive character of solutions of the Schrödinger equation has played an important role in rejecting Schrödinger's original interpretation, and accepting the Born rule.In the coordinate representation of the wave (such as the Cartesian coordinate system), the position of the physical object's localized probability is specified by the position of the packet solution. Moreover, the narrower the spatial wave packet, and therefore the better localized the position of the wave packet, the larger the spread in the momentum of the wave. This trade-off between spread in position and spread in momentum is a characteristic feature of the Heisenberg uncertainty principle,and will be illustrated below.
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