1 / 38

The earth, ca. 1800

The earth, ca. 1800. Nevil Maskelyne and the Schiehallion experiment (1774). Schiehallion (‘Sidh Chailleann’) Scotland. Nevil Maskelyne doing his impression of Ben Franklin. d. . F. M s. m . g. F = m . g . tan(  ) = G . m . M s /d 2.

lam
Download Presentation

The earth, ca. 1800

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. The earth, ca. 1800

  2. Nevil Maskelyne and the Schiehallion experiment (1774) Schiehallion (‘Sidh Chailleann’) Scotland Nevil Maskelyne doing his impression of Ben Franklin d  F Ms m.g F = m.g.tan() = G.m.Ms/d2 ME = (RE2/d2).(Ms/tan()) ~ 6.1024 kg RE = 6.37.106 m; VE = 1.1.1021 m3 m.g = G.m.ME/RE2  ~ 5.5 g/cm2 (initially found ~ 4.5)

  3. Densities of common substances (all in g/cc) Ice 0.917 Water 1.000 Seawater 1.025 Graphite 2.200 Granite ~2.70 Titanium 4.507 Iron 7.870 Copper 8.960 Mercury 13.58 Gas: proportional to P/RT Two options: sub-equal mix of metal and rock or… an ideal gas, w/ high density at high P (B. Franklin)

  4. Mass distribution in earth’s interior Period of precession Moment of inertia Period of spin Torque (sun and moon trying to pull earth’s tidal bulge into plane of ecliptic) ri I = i mi.ri2 mi Higher Earth has I much less than expected for homogeneous sphere Lower

  5. Kraemer, 1902 View combining known density, moment of inertia, oblateness, rigidity of surface rocks, and topography Note bad for a bunch of turn-of-the-century quacks!

  6. Earthquakes! The sources of seismic waves

  7. Earthquake nomenclature Epicenter Ground Hypocenter (‘focus’) Fault plane Other side of the earth Anticenter

  8. Basic types of faults Ground Hanging wall Foot wall Fault plane Dip-slip (cut-away view) Normal: Hanging wall down Thrust (‘reverse’): Hanging wall up Strike-slip (bird’s eye view) Right lateral Left lateral Fault trace

  9. 0 Seconds Rupture expands circularly on fault plane, sending out seismic waves in all directions. Focus Fault cracks at surface 5 Seconds Rupture continues to expand as a crack along the fault plane. Rocks at the surface begin to rebound from their deformed state. Fault crack extends 10 Seconds The rupture front progresses down the fault plane, reducing the stress. 20 Seconds Rupture has progressed along the entire length of the fault. The earthquake stops.

  10. The fault plane of the Landers earthquake (eastern California shear zone; 1992) Displacement on fault plane

  11. The broader context of faulting Fault plane; episodic rupture Brittle Ca. 10-30 km deep Ductile Broad zone; continuous plastic shear

  12. Focus “sample” outer ca. 200 km, but most energy in upper 10 km Surface waves Mantle Body waves Seismograph Core S P

  13. A mechanical seismograph

  14. Anatomy of a seismic signal Minutes 0 10 20 30 40 50 Surface waves P S ‘Primary’ (first to arrive) ‘Secondary’ (second to arrive)

  15. P waves — analogous to sound Wave direction

  16. S waves—analogous to light Wave direction

  17. Surface waves Rayleigh wave (analogous to ocean surface) Wave direction Love wave (analogous to a snake or shaken rope) Wave direction

  18. Real data is more complicated…

  19. Normal modes (‘natural’ or ‘harmonic’ oscillations) Spheroidal (radial motion) Toroidal (torsional, shearing motion) On earth, periods are ca. tens of minutes

  20. Speeds of seismic waves • Surface and normal modes have complex velocity dependencies; take 11d to learn about these! • Body waves are simpler (and more important for studying earth’s interior) elastic modulus’ (stiffness) Velocity is proportional to density (momentum) F/m2 — kg/s2m stress strain Elastic modulus = Unitless; e.g., ∂Volume/Volume Two elastic moduli: • Bulk modulus (): isotropic compression; springiness of bonds • Shear modulus (): resistance to change in shape

  21. Speeds of seismic waves General relation: V = (modulus/)0.5 VP = ([+4/3]/)0.5 VS = (/)0.5 • For finite  and , VP must be faster than VS •  = 0 in fluids, so VP drops sharply and VS goes to 0 when waves hit a solid/fluid boundary

  22. Locating the hypocenter using networks of multiple seismographs Seismograph Seismograph Epicenter Focus Seismograph

  23. Seismogram C Seismogram B S wave Seismogram A 25 20 11-minute interval at 8600 km Time elapsed after start of earthquake (min) 8-minute interval at 5600 km 15 P wave 10 5 3-minute interval at 1500 km 0 2000 4000 6000 8000 10,000 Distance traveled from earthquake epicenter (km)

  24. measure the amplitude of the largest seismic wave… P S Amplitude =23 mm P-wave S-wave interval = 24 seconds …and the time interval between the P- and S-waves (I.e., the distance from the epicenter. Interval between S and P waves (s) Distance (km) Connect the points to determine the Richter magnitude. Richter magnitude Amplitude (mm)

  25. Moment magnitude Moment = Slip x Area x Elastic modulus N.meters Meters Kg/s2.m Meters2 Log10 of moment

  26. The Mercalli Intensity scale (earthquake intensities for people who don’t like numbers and are easily scared) Board

  27. Mg2SiO4 in upper mantle Mg2SiO4 in lower mantle

  28. The core’s density is less than that of pure Fe. Requires a low-mass Alloying agent. S? O? H? ???

More Related