note: at this point, the wave hits an “edge” from it’s perspective. this is where the...

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Page 1: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from
Page 2: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from
Page 3: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from

Note: at this point, the wave hits an “edge” from it’s perspective.

This is where the “diffracted” term comes from

Page 4: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from
Page 5: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from
Page 6: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from

Instrument response?

Page 7: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from
Page 8: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from
Page 9: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from
Page 10: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from

Seismic wave velocities• Wave equation:

– Part 1: • Force = stress x area

– Part 2: • Force = mass x

acceleration

• Also need:– Hooke’s law:

• F = -k x

• Deep breath (lower stress)…..

Page 11: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from

Deriving wave equation1. Go over some tools

2. Relate stress and displacement

3. Simplify as much as possible

4. Substitute into F=ma equation

5. Apply some vector identities

6. Show that there are only two solutions, which have the

velocities of the P- and S- waves

Page 12: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from

Stress & Strain

• Stress– Force/unit area

• Strain (1-dimension)– Here = L/L– Finite strain

• Whole history• >few %• Shape/relationships

change

– Infinitesimal strain• Less than few %• Allows some simplifications

(L’-L)/L = L/L = xx=dux/dx

Page 13: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from
Page 14: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from

Vector fields

• Divergence of a vector field:– No rotation– Just volume change– Which body wave?

Page 15: Note: at this point, the wave hits an “edge” from it’s perspective. This is where the “diffracted” term comes from

Vector fields

• Curl:– No volume change– Just rotation– Which body wave?