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Tuesday, June 13, 2006
Tuesday, June 13, 2006

Consider a rod BC of length L and uniform cross-sectional... x which is characteristics of the rod BC.
Consider a rod BC of length L and uniform cross-sectional... x which is characteristics of the rod BC.

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... Again by superposition, U = U1 + U2 + U3 + U4. Since all the masses are the same, the only difference between the Ui’s is the distance from the mass Mi to the test mass m. For the two righthand masses, r1 = a/2. For the two left-hand masses, r22 = (a/2)2 + a2 = 5a2/4, and so r2 = 5a/2. U = –2 G M m ...
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Chapter 4 - UniMAP Portal

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5th Homework Due: 7 November 2008 1. In spherical

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... 130. A metal tool is sharpen by being held against the rim of a wheel on a grinding machine by a force of 180N. The frictional forces between the rim and the tool grind small pieces of the tool. The wheel has a radius of 20cm and rotates at 2.5 rev/s. The coefficient of kinetic friction between the ...
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Chapter 7 Energy

... • When we lift a load against Earth’s gravity, work is done. – The heavier the load or the higher we lift the load, the more work is done. – Two things enter the picture whenever work is done: • (1) application of a force, and • (2) the movement of something by that force. ...
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Energy and Energy Resources

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1. A weightlifter is raising a 100 kg barbell above his head at

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Energy and Energy Resources

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Eigenstate thermalization hypothesis

The Eigenstate Thermalization Hypothesis (or ETH) is a set of ideas which purports to explain when and why an isolated quantum mechanical system can be accurately described using equilibrium statistical mechanics. In particular, it is devoted to understanding how systems which are initially prepared in far-from-equilibrium states can evolve in time to a state which appears to be in thermal equilibrium. The phrase ""eigenstate thermalization"" was first coined by Mark Srednicki in 1994, after similar ideas had been introduced by Josh Deutsch in 1991. The principal philosophy underlying the eigenstate thermalization hypothesis is that instead of explaining the ergodicity of a thermodynamic system through the mechanism of dynamical chaos, as is done in classical mechanics, one should instead examine the properties of matrix elements of observable quantities in individual energy eigenstates of the system.
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