Torr Kolen 's An Experiment to Measure Relative Variations in the One-Way PDF

By Torr Kolen

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02xlO28 atoms/m 3 n 18X1028 „ Valence = — = =s- = 3 n' 6x10 28 / t M _3N_ 2/3 N . 4 MeV Eav=|EF=20MeV These energies are of the correct order of magnitude for nuclear particles. 8% probability. 6xl0- 5 eV/K)(300 K) .. 40xl0 17 . rz> e~''"' " B ) 3/2 where m is the mass of the O , molecule (2xkBT) in kg and — is 104 molecules per cm 3 . Rewrite the equation in the form n(v) = AA—-J u2e~/l31' where A^ = , A2 = ,andA3= . Use the exponential format for large and small numbers to avoid computer errors.

385)>. 015 . 000 717. These values are plotted below. One sees that this approximation is good for low energy. There is exact agreement for P(0) and P(1E) and small deviations for the next two values with percent deviations for the higher energy values. 0) T3 •J3 A3 (JO M OJ c c ••B a m C a •8 Energy 10-7 (a) Ev =-pe=-ecos0°=-pe ED = - p £ , = -fcosl80°=+p£ so AE = ED - Ev = 2pe. (b) Let n(2pe) be the number of molecules in the excited state. n(2pe) g{2pe)Ae-2ps/k<>T •n(0) g{0)Aeu 2e~2velk*T MODERN PHYSICS (c) L90 = n(2p£) = 2 e .

913 u. 6) = 1720 MeV AE = Ebf - £(,,- = 1720 MeV -1560 MeV = 160 MeV 19 (a) kq The potential at the surface of a sphere of charge a and radius r is V = —. If a thin shell of charge d<7 (thickness dr) is added to the sphere, the increase in electrostatic potential energy will be dU = Vdq = — \dq.

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An Experiment to Measure Relative Variations in the One-Way Velocity of light by Torr Kolen


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