1. Chapter 1- General Properties of Waves Reflection Seismology Geol 4068 Elements of 3D Seismology, 2nd Edition by Christopher Liner August 25, 2005

2. Outline-I General Properties of Waves Mechanical definition of a wave Physical Assumptions Wave descriptions Body waves Surface waves Particle motion

3. General Properties of Waves Wave descriptions Graphical Mathematical Outline-II

4. General Properties of Waves General theorems and principles Reciprocity Theorem Fermat’s Principle Snell’s Law, Conservation of ray parameter, critical angle Huygen’s Principle Outline-III

5. Outline-I General Properties of Waves Mechanical definition of a wave Physical Assumptions Wave descriptions Body waves Surface waves Particle motion

6. t1 t2 t3 Homogeneous, isotropic medium … cylindrical wavefronts-- rays are at right angles to the wavefronts Mechanical definition of a wave Physical Assumptions

7. t1 t2 t3 Anisotropic-- rays are not at right angles to the wavefronts! Mechanical definition of a wave Physical Assumptions

8. General Properties of Waves Mechanical definition of a wave Physical Assumptions Wave descriptions Body waves Surface waves Particle motion

9. Body Waves Direction of propagation of the body wave Direction of particle displaement Direction of propagation of the body wave Direction of particle displaement X Y Z Direction of propagation of the body wave Direction of particle displaement

10. Body Waves - do not require a boundary to travel Direction of propagation of the body wave Direction of particle displaement X Y Z Sv Direction of propagation of the body wave Direction of particle displaement Direction of propagation of the body wave Direction of particle displaement Sh P

11. General Properties of Waves Mechanical definition of a wave Physical Assumptions Wave descriptions Body waves Surface waves Particle motion

12. Surface Waves XX Z Amplitude of Rayleigh wave decays with depth Adapted fromAki and Richards, 2002, p. 156

13. General Properties of Waves Mechanical definition of a wave Physical Assumptions Wave descriptions Body waves Surface waves Particle motion

14. --Image 1 Particle Motion

15. --Image 2 Particle Motion

16. --Image 3 Particle Motion

17. --Image 4 Particle Motion

18. --Image 5 Particle Motion

19. General Properties of Waves Wave descriptions Graphical Mathematical Outline-II

20. Graphical * particle velocity V.s/m distance time Fixed time particle velocity V.s/m * Fixed position

21. Graphical particle velocity V.s/m time particle velocity V.s/m Fixed time distance * * Fixed position

22. Mathematical Temporal frequency = 1/period; units of (1/s) Spatial wavenumber = 1/wavelength; units of (1/m) Temporal and Spatial mixed velocity (m/s) = frequency * wavelength

23. Mathematical Signal power can be measured in a relative scale known as decibels: Decibels: db = ratio of powers (energies): 10 log (P1/P2) e.g. P1 =100, P2 = 10 then, P1/P2 = 10 10.log10= 10 dB = 10 e.g., P1 = 4, P2 = 1 then, P1/P2 = 4 ( log4 = 0.6) dB = 10 log4 = 6 octave = f, 2f, 4f, 8f

24. Mathematical Geometric Spreading seismic Amplitude = Energy ^ 0.5 energy on a spherically expanding wavefront is proportional to 4.pi.r^2 amplitude is proportional to 2*pi^0.5*r where r is the distance traveled by a ray along its path

25. Mathematical Geometrical Spreading e.g., using cubes 2x Energy density= energy/Area Area2 Area 1 Energy density in Area2/Energy density in Area 1 = Area1/Area2 2x

26. Mathematical Geometrical Spreading 2x 2^0.5*x r2 r1=2^0.5*x TOP VIEW=SIDE VIEW “longer side”

27. Mathematical Geometric Spreading with a CUBE By similarity of triangles: r2/r1 = length of longer side/2x length of longer side = r2/r1*2x short side =2x Area1 = 4 * x^2 Area 2 = (r2/r1)^2 *4*x^2 Area1/Area2 = (r2/r1)^2

28. Mathematical Geometrical Spreading Distance r1 = X.2^0.5 r2 Area1/Area2 = (r2/r1)^2 Area2 Area 1 r1 Distance r2 = (X+0.5*r2- 0.5*r1)*2^0.5 Longer side = x + r2-r1

29. Mathematical Geometrical Spreading r2 Energy ratios = (r2/r1) ^2 Area2 Area 1 r1 Amplitude ratios = r2/r1

30. General Properties of Waves General theorems and principles Reciprocity Theorem Fermat’s Principle Snell’s Law, Conservation of ray parameter, critical angle Huygen’s Principle

31. Reciprocity Theorem (e.g.,Aki and Richards, 2002, p. 24) Corollary: Displacements measured by interchanging source and receivers are indistinguishable

32. Reciprocity Theorem * time

33. Reciprocity Theorem * = time

34. Reciprocity Theorem: Assumption of isotropy *

35. General Properties of Waves General theorems and principles Reciprocity Theorem Fermat’s Principle Snell’s Law, Conservation of ray parameter, critical angle Huygen’s Principle

36. Fermat’s Principle The path a wave travels will always be that which takes the least amount of time to go from the source to a particular receiver

37. General Properties of Waves General theorems and principles Reciprocity Theorem Fermat’s Principle Snell’s Law, Conservation of ray parameter, critical angle Huygen’s Principle

38. Snell’s Law: Consequence of Fermat’s Principle “Ratio of the sines of the angles of incidence and reflection or refraction are proportional to the ratios of the velocities of the waves in their respective media”

39. Snell’s Law V1 V2 V1<V2 V2 Angle of incidence Angle of refraction

40. Snell’s Law V1 V2 V1=V2 Angle of incidence Angle of refraction

41. Snell’s Law V1 V2 V1>V2 Angle of incidence Angle of refraction

42. Snell’s Law V1 V2 V1<V2 V2 Angle of incidence Angle of refraction Angle of reflection transmitted ray

43. Snell’s Law V1 V2 V1<V2 V2 Angle of incidence = critical angle Angle of refraction = 90 degrees

44. Snell’s Law Critical angle = angle whose sine is the ratio of the slow over the fast velocity across the interfaces

45. Snell’s Law Conservation of the horizontal ray parameter p = sin (incident angle)/V1 p (ray parameter) is constant along a ray path (Aki and Richards, 2002, p.88)

46. Snell’s Law Assumption Mechanical continuity across the interface i.e., no sliding, i.e., complete coupling of both media across the interface

47. Snell’s Law V1 V2 V1<V2 V2 Angle of incidence Angle of refraction

48. Snell’s Law V1 V2 V1<V2 V2 Angle of incidence Angle of refraction delta t

49. Snell’s Law Delta t = distance traveled along the interface in the horizontal direction/ V1 = distance traveled along the interface, in the horizontal direction/V2 = sin (angle of incidence) / V1 = p

50. General Properties of Waves General theorems and principles Reciprocity Theorem Fermat’s Principle Snell’s Law, Conservation of ray parameter, critical angle Huygen’s Principle

51. “…every point of a wavefront may be considered to be act as a secondary wave in the direction of wave propagation. The sum of these wavelets generates the new wavefront...”

52. Huygen’s Principle Diffractions

53. Huygen’s Principle Diffractions

54. Huygen’s Principle Diffractions

55. Huygen’s Principle Diffractions

56. Huygen’s Principle Diffractions

57. Huygen’s Principle Diffractions

58. Huygen’s Principle Diffractions

59. Huygen’s Principle Diffractions

60. Huygen’s Principle Diffractions

61. Huygen’s Principle Diffractions

62. Huygen’s Principle Diffractions

63. Huygen’s Principle Diffractions

64. Huygen’s Principle Diffractions

65. Huygen’s Principle Diffractions

66. Huygen’s Principle Diffractions

67. Movies Thomas Bohlen, at the University of Kiel, in Germany has many interesting finite difference movies on wave propagation through the earth. Here is the web link to his web site: http://www.geophysik.uni- kiel.de/~tbohlen/movies/http://www.g eophysik.uni-kiel.de/~tbohlen/movies/

68. Q. 1 What is the P-wave velocity of the following earth materials measured near the surface of the earth: basalt, granite, peridotite, gabbro, iron Homework 1-due September 8, 2005 at 9.30 a.m.

69. Q. 2 Following a surface explosion, as a “ray” of sound enters the blue synform what will the angle of refraction at point A for the following interface geometry? Apply Snell’s Law with the values provided. Explain your work clearly and succinctly. Hint: simplify the geometry of the geology

70. Homework 1-due September 8, 2005 at 9.30 a.m. Q. 2

71. Homework 1-due September 8, 2005 at 9.30 a.m. Q. 3 If the lowest frequency your body size can register is about 8 times your greatest dimension, does this value change whether you are in water or in air? What are these values? Assume sound travels at 1500 m/s in water and 330 m/s in air. Assume you are 2 m high.

72. Homework 1-due September 8, 2005 at 9.30 a.m. Q. 4 What is the critical angle between water and basalt? This is a typical scenario in oceanic spreading ridges. Assume a Pwave velocity of 1500 m/s

74. Surface Waves X When body waves traveling through rock reach the interface below a fluid or below the atmosphere they combine to form complex particle motions in the rock, such as Rayleigh waves (air/rock) or Stonely waves (water /rock). These motions are retrograde elliptical shallow to prograde elliptical deep