Waves in fluids and solids Part 2 pot

...    2 3 22 322 2 2 22 2 2 22 2 2 2 2 2 2 22 231311 122 11 11641 121 1 mEee ggu e gu e gu g g eg eg eug nuE eggueguegEgeeug                              . ( 122 ) ... 1 and 2) is also Waves in Fluids and Solids 30 0 100 20 0 300 400 500 600 700 -2 -1 0 1 2 Frequency [Hz] -2 -1 0 1 2 -2 -1 0 1 2 -2 -1 0...

Ngày tải lên: 19/06/2014, 12:20

... 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 1 2 1 det( )det 2det1 D D cc cc cc cc cccc cccc cc ... 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...

Ngày tải lên: 19/06/2014, 12:20

... This opens the possibility to engineer a novel and useful method for investigating the complex response 128 Waves in Fluids and Solids Waves in Fluids and Solids 116 Kr matrix behaves almost ... propagates from one grain to its neighbors only through their mutual contacts and not via air, we have 130 Waves in Fluids and Solids Waves in Fluids and...

Ngày tải lên: 19/06/2014, 12:20

...       , (27 a) (27 b) in the water, and   22 22 11 1 1 111 1 22 2 22 2 111 11 22 22 22 11 1 1 111 1 22 2 22 2 22 xx xz zz xz xz z xz xz xz xz x           ... 55–86 1 52 Waves in Fluids and Solids Waves in Fluids and Solids 160 22 000 0 .   ( 32) in the water, and 22 111 0 , p...

Ngày tải lên: 19/06/2014, 12:20

... of 2 A , 2 B and C are given as follows: 22 2 11 2 222 222 3 2 111 2( 4) (2) 16 (4) (2 8 /) mm mm m m Ne A Rc λμ ωω ρω λμ ωηωω ωδω   +− =−   ++ −++    , 3 2 11 1 2 2 22 222 3 2 111 4 (28 /) (2) 16 ... Eqs. (4 .29 ) and (4.30) in Eq. (4 .28 ) yields 2 22 1 111 2 1 ()0 g d V dx ρω Φ +Λ+ Φ=  , (4.31a) 2 22 2 42 2 22 2 1 2 1 (4 ) g d VV dx ρω ρ...

Ngày tải lên: 19/06/2014, 12:20

... ultra-thin layered reservoirs taking into account the interbedded multiples. 2, 22 2 ,21 2, 20 2, 19 2, 18 2, 17 2, 16 2, 15 2, 14 2, 13 0,00,10 ,20 ,30,4  Depth, km 2, 22 2 ,21 2, 20 2, 19 2, 18 2, 17 2, 16 2, 15 2, 14 2, 13 0,5 ... m 420 0 422 0 424 0 426 0 428 0 4300 4 320 1,8 1,9 2, 0 2, 1 2, 2 2, 3 2, 4 2, 5 2, 6 2, 7  420 0 422 0 424 0 426 0 428 0 4300...

Ngày tải lên: 19/06/2014, 12:20

... determinant coincides with (29 ) completely. (30) Waves in Fluids and Solids 88 11 12 13 11 12 13 21 22 23 21 22 23 31 32 33 31 32 33 11 12 13 11 12 13 21 22 23 21 22 23 31 32 33 31 32 33 00 00 00 00 00 00 000000 uu ... the metal layer has the simplest form: 11 12 13 11 12 13 21 22 23 21 22 23 31 32 33 31 32 33 11 12 13 11 12 13 21...

Ngày tải lên: 19/06/2014, 12:20

... the transfer matrix M FE1QE2G by the following expression: (2) 11 12 13 11 12 13 1 1 1 (2) 21 22 23 21 22 23 2 2 2 (2) 31 32 33 31 32 33 3 3 3 11 12 13 11 12 13 1 (2) 0 0 0 0 uu uu uu uT uT ... most general form: 11 12 13 11 12 13 1 1 21 22 23 21 22 23 2 2 31 32 33 31 32 33 3 3 11 12 13 11 12 13 1 1 12 21 22 23 21 22 23 2 2 uu uu uu uT uT u...

Ngày tải lên: 19/06/2014, 12:20

... formula: 12 12 22 12 2 2 2 322 222 1 5,667 10 1,7 32 10 2, 096 10 1, 125 10 1 5,084 10 1,818 10 2, 625 10 1,074 10 n λλλλ λλλλ −−−− −−− ⋅⋅⋅⋅ −= + + + −⋅ −⋅ −⋅ −⋅ Waves in Fluids and Solids 176 ...    (11) The matrix elements in this equation are: () () () () 21 21 12 2 1 2 12 12 21 21 121 2 12 12 11 exp cos sin , exp sin , 22 11 exp sin...

Ngày tải lên: 19/06/2014, 12:20

... Waves in Fluids and Solids 20 0 vibrating molecules. The standing waves are induced in each globule of the crystal. The pulsating modes arising in the PNC globules are ... Scattering (SGS) in the PTC were first described in [6]. The schematic of experimental setup for observing this scattering in the “forward” and “backward” geometry is illustrated in Figs. 2...

Ngày tải lên: 19/06/2014, 12:20