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

Date post: 25-Dec-2015
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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?


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