Analysis and Comparison of Wave Equation Prediction for Propagating Waves

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Initial analysis and comparison of the wave equation and asymptotic prediction of a receiver experiment at depth for one-way propagating waves. The study examines the amplitude and information derived from a wave equation migration algorithm and its asymptotic form. The focus is on the prediction of the receiver experiment at depth, including Green's theorem/FK prediction, the exact Cagniard-deHoop solution, and the asymptotic output. The theory, numerical tests, and a summary are outlined for wave equation prediction and its corresponding asymptotic form for one-way up-going waves. Various equations and formulas are discussed in detail, shedding light on the mathematical aspects of wave propagation in heterogeneous media.


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  1. Initial analysis and comparison of the wave equation and asymptotic prediction of a receiver experiment at depth for one- way propagating waves Chao Ma*, Jing Wu and Arthur B. Weglein 1 M-OSRP 2014 Annual Meeting, May, 2014 Austin, TX

  2. Motivation Qiang et al (2014) examine the amplitude information at the image that derives from a wave equation migration algorithm and its corresponding asymptotic form. The asymptotic form follows from a stationary phase approximation performed on the operator that predicts the receiver and source experiment at depth. We examine the prediction of the receiver experiment at depth: Green s theorem/FK prediction The exact Cagniard-deHoop (CdH) solution The asymptotic output. 2

  3. Outline Theory Wave equation prediction and its corresponding asymptotic form for one way waves Numerical test Summary 3

  4. Wave equation prediction for one way up-going waves Stolt (1978), Stolt and Benson (1986), Stolt and Weglein (2012) Assuming an up-going wave, and homogeneous medium ( , | , ; ) D x z x z t g g s s ( ) ik x i t , e dx e dt g g g , ; ) s x z ( , | D k z g g s 2 g 2 k c z z = ( ) ik 1 ; ) = ; ) k ( , | , ( , | , D k z x z D k z x z e z g z 2 g s s g g s s c 1 ik x ; ) = ; )e W ( , | x z x z , ( , | , D D k z x z dk g s s g s s g 2 4 1 i t = ; ) W W ( , | x z x z t , ; ) ( , | x z x z , D D e d s s s s 2

  5. Asymptotic form of the wave equation prediction for one way up-going waves 1 z z ( ) ik x ik ik x = W ( , | x z x z , ; ) s ( , | , ; ) s x z D D x z e dx e e dk g g z g g s g g s g g 2 1 z z + x x [ ( ) ( )] i k k = ( , | , ; ) s x z D x z dx e dk z g g g g g s g g 2 5

  6. Asymptotic form of the wave equation prediction for one way up-going waves 1 z z ( ) ik x ik ik x = W ( , | x z x z , ; ) s ( , | , ; ) s x z D D x z e dx e e dk g g z g g s g g s g g 2 1 z z + x x [ ( ) ( )] i k k = ( , | , ; ) s x z D x z dx e dk z g g g g g s g g 2 2 2 ( cr ) i z z 1 gr c ( , | x z x z / A g , ; ) D ( , | , ; ) s x z D x z dx e s s g g s g 3 g 2 ) ( 6 = + 2 2 ( ) ( ) r z z x x g g g

  7. Asymptotic form of the wave equation prediction for one way up-going waves 1 z z ( ) ik x ik ik x = W ( , | x z x z , ; ) s ( , | , ; ) s x z D D x z e dx e e dk g g z g g s g g s g g 2 1 z z + x x [ ( ) ( )] i k k = ( , | , ; ) s x z D x z dx e dk z g g g g g s g g 2 2 g 2 k c = 1 k z 2 c 2 2 ( cr ) i z z 1 gr c ( , | x z x z / A g , ; ) D ( , | , ; ) s x z D x z dx e s s g g s g 3 g 2 ) ( ( ) ( ) x x z z 7 g g = = = + 2 2 , , ( ) ( ) k k r z z x x g z g g g c r c r g g

  8. Asymptotic form of the wave equation prediction for one way up-going waves 1 z z ( ) ik x ik ik x = W ( , | x z x z , ; ) s ( , | , ; ) s x z D D x z e dx e e dk g g z g g s g g s g g 2 1 z z + x x [ ( ) ( )] i k k = ( , | , ; ) s x z D x z dx e dk z g g g g g s g g 2 2 g 2 k c Non-linear = 1 k z 2 c 2 2 ( cr ) i z z 1 gr c ( , | x z x z / A g , ; ) D ( , | , ; ) s x z D x z dx e s s g g s g 3 g 2 ) ( ( ) ( ) x x z z 8 g g = = = + 2 2 , , ( ) ( ) k k r z z x x Linear g z g g g c r c r g g

  9. Outline Theory Wave equation prediction and its corresponding asymptotic form for one way waves; Numerical test Summary 9

  10. Numerical test comparing a wave equation prediction of a receiver experiment at depth and its asymptotic form Model: -20,000 m to 20,000 m (dx=4m) Input data at depth 400 m sz = (0, 0) x z = ( , 400) = CdH ( , 400|0, , ) D x z z t g g g g s = 2000 / c m s 0 Reflector depth 2000 m = 1000 / c m s 1 10 Tmax=5 s, dt=1 ms;

  11. Numerical test comparing a wave equation prediction of a receiver experiment at depth and its asymptotic form sz = (0, 0) Input data at depth 400 m Predicted depth 600 m x z = ( , 400) g g = CdH ( , 400|0, , ) D x z z t g g s = 2000 / c m s 0 Reflector depth 2000 m = 1000 / c m s 1 Input Calculate = = z W W ( , x z 600|0, , ) ( , x z 600|0, , ) D z t D 11 s s = CdH ( , 400|0, , ) D x z z t g g s = = z A A ( , x z 600|0, , ) ( , x z 600|0, , ) D z t D s s

  12. Numerical test comparing a wave equation prediction of a receiver experiment at depth and its asymptotic form Comparison (0m offset and 2000m offset) = = z CdH CdH ( , x z 600|0, , ) ( , x z 600|0, , ) D z t D s s = = z W W ( , x z 600|0, , ) ( , x z 600|0, , ) D z t D s s = = z A A ( , x z 600|0, , ) ( , x z 600|0, , ) D z t D s s 12

  13. Compare (0 m) Zero-offset space-time = CdH ( , x z 600|0, , ) D z t s = W ( , x z 600|0, , ) D z t s = A ( , x z 600|0, , ) D z t s 13

  14. Compare (0 m) Zero-offset space-time (zoom-in of the plot in the last slide) = CdH ( , x z 600|0, , ) D z t s = W ( , x z 600|0, , ) D z t s = A ( , x z 600|0, , ) D z t s 14

  15. Compare (0 m) Zero-offset space-frequency = z CdH ( , x z 600|0, , ) D s = z W ( , x z 600|0, , ) D s = z A ( , x z 600|0, , ) D s 0.04 CdH accurate data Asymptotic prediction Wave prediction 0.035 0.03 0.025 Amplitude 0.02 0.015 0.01 0.005 15 0 0 10 20 30 40 50 60 Frequency/Hz

  16. Compare (0 m) Zero-offset space-frequency (zoom-in of the plot in the last slide) = z CdH ( , x z 600|0, , ) D s = z W ( , x z 600|0, , ) D s = z A ( , x z 600|0, , ) D s 0.04 CdH accurate data Asymptotic prediction Wave prediction 0.035 0.03 0.025 Amplitude 0.02 0.015 0.01 0.005 16 0 0 2 4 6 8 10 12 14 16 18 20 Frequency/Hz

  17. Compare (2000 m) 2000 m-offset space-time = CdH ( , x z 600|0, , ) D z t s = W ( , x z 600|0, , ) D z t s = A ( , x z 600|0, , ) D z t s 17

  18. Compare (2000 m) 2000 m-offset space-time (zoom-in of the plot in the last slide) = CdH ( , x z 600|0, , ) D z t s = W ( , x z 600|0, , ) D z t s = A ( , x z 600|0, , ) D z t s 18

  19. Compare (2000 m) 2000 m-offset space-frequency (zoom-in of the plot in the last slide) = z CdH ( , x z 600|0, , ) D s = z W ( , x z 600|0, , ) D s = z A ( , x z 600|0, , ) D s 0.04 CdH accurate data Asymptotic prediction Wave prediction 0.035 0.03 0.025 Amplitude 0.02 0.015 0.01 0.005 19 0 0 10 20 30 40 50 60 Frequency/Hz

  20. Compare (2000 m) 2000 m-offset space-frequency (zoom-in of the plot in the last slide) = z CdH ( , x z 600|0, , ) D s = z W ( , x z 600|0, , ) D s = z A ( , x z 600|0, , ) D s 0.04 CdH accurate data Asymptotic prediction Wave prediction 0.035 0.03 0.025 Amplitude 0.02 0.015 0.01 0.005 20 0 0 2 4 6 8 10 12 14 16 18 20 Frequency/Hz

  21. Outline Theory Wave equation prediction and its corresponding asymptotic form for one way waves; Numerical test Summary 21

  22. Summary The difference in the spectrum at the low end has a dramatic impact on subsequent imaging step, and makes the asymptotic migration method NOT an approximate source and receiver coincident experiment at time equals zero. 22

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