Electromagnetic Waves Part 1 pot

... 2 010 ) The force of light is the operative mechanism behind “space sails” which are now being employed on Electromagnetic Waves 12 5 -15 3 4 10 4 4 47.31x10 7.031x10 er g /cm de g 3x10 ... IX Part 1 The Physics of Electromagnetic Fields 1 Chapter 1 The Fundamental Physics of Electromagnetic Waves 3 Juliana H. J. Mortenson Chapter 2 Modern Classical Electrodynami...

Ngày tải lên: 19/06/2014, 21:20

... Modern Phys., 19 45, 17 , N 2-3, p. 15 7 -18 1 [10 0] Pegg D.T. Rep. Prog. Phys. 19 75. V. 38. P. 13 39 [10 1] Rohrlich F. Classical Charged Particles. Reading, Mass.: Addison-Wesley, 19 65 - [10 2] Bolotovskii ... Physics Reports, 12 3/ (1 and 2), 1- 116 , 19 85 [48] Moffat H.K. The degree of knottedness of tangled vortex lines. Journal of Fluid Mechanics, 35 /1, 11 7 -12 9.,...

Ngày tải lên: 19/06/2014, 21:20

... lenses in electromagnetic beams considering that the incident beam has plane wavefronts (Saleh & Teich, 19 91) z  r   1 1 z r / f P  2  z r , w  0  1 1 z r / f P  2 w 0 , (10 9) where ... fields in cavities R 1 and R 2 , the interference fringes can be seen (Raimond et al., 20 01; Ramsey, 19 85; Nogues et al., 19 99). 88 Electromagnetic Waves Electromagnetic...

Ngày tải lên: 19/06/2014, 21:20

... ' 11 12 6 1 21 22 6 1 '' ' 11 12 6 1 21 22 6 ()() ()() Det mmqqmmq RF mmqqmmq    (30) where m ij are the entries of matrix M and F 1 is given by 2 212 1 2 22 1 4coscos (cos ... al., 19 94). Prism ZrO2 Glass  5 ’ (Ag)  5 ’’ (Ag) d 5 - 17 . 41 0 .10 0.2 ±0 .1 615 15 Å -18 .1 ±0 .1 1. 36 ±0.08 14 6 ±5Å   ’ ( Pi...

Ngày tải lên: 19/06/2014, 21:20

... linearised non-linear problem (α =+0. 01, right figure): |U(κ (NL) 1 ; z)| with κ (NL) 1 = 0.370 511 0 −i 0. 010 49 613 ( #1) , |U(κ (NL) 3 ; z)| with κ (NL) 3 = 1. 1 214 73 −i 0.00 919 4824 (#2) 337 Resonance Properties ... (18 )) ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩ ∇ 2 E 1 (r, κ)+κ 2 ε κ (z, α(z), E 1 (r, κ) , E 1 (r,2κ), E 1 (r,3κ)) E 1 (r, κ) = − α(z)κ 2 E 2 1 (r,2κ)E 1 (r...

Ngày tải lên: 19/06/2014, 21:20

... () () () 2 2 *22222 12 1 11 1 11 1 2 2 12 12 11 1 12 2 z y xz x y ee e ee ee ηη η ⎡ ⎤ ⎛⎞ ⎛⎞ −− ⎢ ⎥ =− ∂ +∂ + ∂ +∂ − ∂ ⎜⎟ ⎜⎟ ⎢ ⎥ −+ ⎝⎠ ⎝⎠ ⎣ ⎦ . (12 3) () () () 2 2 *22222 12 2 11 2 11 2 2 2 12 12 211 12 2 xz ... () () T 1 * 11 11 1 12 2 2 2 11 1 12 1 EeeE ee η η = ⋅⎡−+⎤ ⎣ ⎦ −+ EE= φ (12 0) () () T 1 * 22 12 211 2 2 2 211 12 1 EeeE ee η η = ⋅⎡+−⎤...

Ngày tải lên: 20/06/2014, 22:20

... second-order approximations         22 2 11 12 12 11 22 11 12 12 11 22 2 2 22 2 12 11 22 12 22 12 11 22 22 12 11 1 1 22 2 , 11 1 1 22 2 D D gg f f ggg ggf g fgg fggg ggf g fgg ggf   ... are given by     11 22 21 12 12 21 22 11 2 222 2 11 12 21 22 11 21 12 22 2 22 2 2 11 21 12 22 11 12 21 22 det det 2 det det det( )det det...

Ngày tải lên: 19/06/2014, 12:20

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Ngày tải lên: 26/02/2014, 11:20

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Ngày tải lên: 25/03/2014, 09:20

... corresponding to n 1 if (n = 1) 1 return 1 2 else 1 return g(n – 1) + 1 End g n^3*log2(n) 40*2 ^10 24 *10 ^-9 U n = U +1 U = 1 O(n) n -1 1 Faculty of Computer Science and Engineering Department of ... program segment: 1 i = 1 2 loop (i <= n) 1 j = 1 2 loop (j < n) 1 k = 1 2 loop (k <= n) 1 doIt(…) 2 k = k *2 3 end loop 4 j = j + 1 3 en...

Ngày tải lên: 28/03/2014, 15:20