One dimensional harmonic oscillator

    • [DOC File]2

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      The energies (eigenvalues) of the one-dimensional harmonic oscillator may be found from the relations. Combining these, we obtain. Unlike the corresponding classical result, we find that the quantum mechanical energy is quantized, in units of , where ω is the classical frequency ω2 = k/m. v is called the vibrational quantum number.

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    • [DOC File]PH 426/526, Thermodynamics and statistical mechanics

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      K force constant, ∆x displacement in an harmonic oscillation . So a one dimensional harmonic oscillator has . even better, equipartition theorem is even valid for non-mechanical systems such as thermal fluctuations in electrical circuits. 2.2. Application of Maxwell-Boltzmann statistics: ideal gas

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    • [DOC File]EXAM I, PHYSICS 4304 - Texas Tech Physics & Astronomy

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      Consider a one-dimensional, damped, driven harmonic oscillator with a driving force given by . F(t), above. Use the known solution for the . steady state displacement. xs(t) of a damped oscillator with a sinusoidal driving force, along with the results of part . a), to find the steady state solution for . x(t) for this driven oscillator as a ...

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    • [DOC File]Information and Statistical Physics 1

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      This vibration simulates a one-dimensional harmonic oscillator contributing two more degrees of freedom (one from p2 and one from x2 terms) to produce a heat capacity of . 7 The energy of a rigid rotating molecule has the form where the p’s represent momenta and a, b, and c are constants.

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    • [DOC File]SCHEME - Punjabi University

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      Particle in a one dimensional box with finite walls. Two dimensional square with infinite walls. Three dimensional rectangular box with infinite walls and three dimensional square well potential. Isotropic Harmonic oscillator. Degeneracy. Matrix Mechanics: Postulates of quantum mechanics. Hilbert space.

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    • [DOC File]Physics 406 - St. Bonaventure University

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      The one-dimensional wave equation is . a. Solution. The wave equation has solutions of the form , , and . These are all traveling harmonic waves, where the wave number is and the angular frequency is . (f is the frequency in Hz.) We’ll concentrate on the complex exponential form: . Then the derivatives are. and . Evidently, Whence we can ...

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    • [DOC File]ch 9 - THE HELIUM ATOM - probs

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      9.1 Two identical, non-interacting spin-1/2 particles of mass m are in the one-dimensional harmonic oscillator for which the Hamiltonian is. a) Determine the ground state and first excited state kets and corresponding energies when the two particles are in a total spin-0 state. What are the lowest energy states and corresponding kets for the particles if they are in a total spin-1 state?

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    • [DOC File]Physics 201 2009

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      2. Harmonic Oscillator. a. isotropic harmonic oscillator. In the Second “Law”, . Separate the variables. We have three one-dimensional problems, which we solved already. All have the same angular frequency, . To obtain a trajectory, we eliminate t to get, for instance, Step one: _____ Solve for . …

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    • [DOC File]3. Simple Harmonic Oscillator

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      3. Simple Harmonic Oscillator. NOTES: We have already discussed the solution of the quantum mechanical simple harmonic oscillator (s.h.o.) in class by direct substitution of the potential energy (3.1) into the one-dimensional, time-independent Schroedinger equation. Recall that C is the spring constant of the spring attached to a mass m .

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    • [DOC File]Simple harmonic motion-

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      A simple harmonic oscillator is simply an oscillator that is neither damped nor driven. So the equation to describe one is: Physically, the above never actually exists, since there will always be friction or some other resistance, but two approximate examples are a mass on a spring and an LC circuit.

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