The theory of wave poseable bends portable requires carrier/vm preservable acquires dimension\Δx probable can be measured Bends relative to the movement of objects or within moving matter. Requires carrier each new proton electron coupling is a new movement. Acquires dimension when it comes into contact with objects[see footnote[ Can be measured relative to the movement of the observer. Nick Harvey + Payman Sheriff It comes into contact with objects Prob. of absorption of two protons in the same state is equal to the prob. of spontaneous emission of a proton into that state. If the initial state consists of two protons in the same state, it will not be possible to distinguish them and the statistical weight of the initial state will be 1\2 ! , However, the amplitude for absorption will be more that of a proton. When there are three protons per initial proton state and one is absorbed, the statistical weight of the initial state is 1/3 !, the statistical weight of the final state is 1/2 ! .Thus the transition probability is (1/3!)1/2!(6)² times that if there were one proton per initial state. Richard Feynman Newman Stability Neumann method which is based on the decomposition of the errors into Fourier series gives us the stability of the implicit approximation to the wave equation using a fourier mode of the form φ n,m = En eimkΔx Formula to calculate the amplitude for absorption E E =-B/A Δx=π A=mv[cos(kΔx(-1[-1 B=2(1-mv(cos(kΔx(-1[+2
Posted on: Thu, 02 Oct 2014 08:26:15 +0000
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