Test 1 Flashcards

1
Q

Displacement Hypothesis and Wegener Theory

A

Continents were together and glaciation occurred over a smaller area (most likely) Wegener also assembled paleoclimatic data showing the distribution of coal deposits(evidence of moist temperate zones), and salt, gypsum and desert sandstones(evidence of dry sandstones(evidence of dry climate) for several geological eras These reflected climatic belts like today’s, e.g. an equatorial tropical rain belt, two adjacent dry belts, two temperate belts and two polar ice caps

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2
Q

Weakness in Wegener Theory

A

Wegener failed to address a convincing mechanism for continental drift
he proposed that the continents slide over ocean floor

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3
Q

Paleoclimatology

A

Paleoclimatology is the study of climates for which direct measurements were not taken.

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4
Q

Paleomagnetism

A

determination of direction and strength of magnetic field in old rocks
Old pole positions can then be determined (magnetic dip or inclination)

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5
Q

Seafloor spreading and evidence to support it

A

Harry Hess(1962) proposed that besides continents, sea floor might also be moving

  1. Marine Magnetic Anomalies
  2. Fracture Zones and transform faults
  3. Measuring plate motion directly w/ GPS
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6
Q

Stages of Data Retrieval

A
  1. Data Acquisition
  2. Data Reduction
  3. Data Processing
  4. Data Interpretation
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7
Q

Data Acquisition

A

Taking Measurements

Target: Anomalies

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8
Q

Data Reduction

A

Converting Readings into a more useful form

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9
Q

Noise

A

Unwanted variations in the quantities being measured

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10
Q

Signal

A

The wanted quantities you want measured

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11
Q

S/N Ratio

A

Repeat readings and take their average, also called stacking
You want high S/N ratio

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12
Q

Inverse Modeling

A

to deduce the causative body directly from the results

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13
Q

Forward Modeling

A

To “guess” a model, calculate the values it would produce, compare them with the observations, and then modify the model until it matches the results sufficiently well.
“Trial and error”

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14
Q

Inversion Problem

A

Trying to deduce the form of the body from the anomaly

Not possible if more than one body could produce the results

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15
Q

Resolution

A

stations may not be close enough to reveal all the details of the signal
i.e. Trying to define in a picture details smaller than the size of the pixels

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16
Q

Data Interpretation

A

The physical model has to be translated into geological terms

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17
Q

Data Processing

A

Fourier analysis
Harmonic analysis
Digital Filtering

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18
Q

Fourier analysis

A

Sort features by their widths, from which we can then select the one we want

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19
Q

Harmonic Analysis

A

Only certain wavelengths are used, such that 1, 2, 3,… half-wavelengths exactly fit the length of the profile; these are called harmonics
As more harmonics are added the approximation improves

20
Q

Harmonic analysis: residual anomaly

A

How well this recombined harmonics match the observed profile can be measured by showing their differences as a residual anomaly

21
Q

Harmonic Analysis: Considerations

A
  1. usually contains a range of wavelengths, so separation of wanted/unwanted signals is only partial
  2. Since the length of the profile are rather arbitrary, so are the harmonics
  3. rejecting shorter wavelengths is often regarded as removing anomalies of bodies near the surface to leave deeper ones. (But whereas a narrow anomaly cannot be due to a deep body, the converse is not true)
22
Q

Digital Filtering: Low pass

A

they let pass through all wavelengths longer than some value, but reduce those shorter

23
Q

Digital Filtering: High pass

A

lets through only wavelengths shorter than some value

24
Q

Digital Filtering: Band pass

A

lets through only a range of intermediate wavelengths

25
Q

Aliasing

A

wavelengths that do not exist can appear to be that do not exist can appear to be present because of large intervals

26
Q

Nyquist wavelength

A

The critical wavelength(twice the sampling interval)

27
Q

Waves (Seismology)

A

Vibrations of Rocks

28
Q

4 Parts of Seismology

A
  1. Global seismology and seismic waves
  2. Refraction
  3. Reflection
  4. Earthquakes and seismotectonics
29
Q

Wave Fronts

A

compression travels spherically outwards (spherical surfaces)

30
Q

Rays

A

conforms a small portion of the wave front always perpendicular to it v=km/s

31
Q

Seismometers

A

More sensitive
Less Robust
used to measure weak signals (like distant earthquakes)

32
Q

Geophone

A

Used in small scale surveys

where highest sensitivity is not needed

33
Q

Earth symmetry analysis as based on epicentral angles

A
  1. Times to travel all paths with the same epicentral angle are nearly the same (for both small and large angles), so the Earth is indeed spherically symmetrical
  2. (gets faster with depth) Earth is not seismically uniform
34
Q

Refraction

A

When wave fronts cross obliquely into a rock with a higher seismic velocity they speed up, which causes them to change direction

35
Q

Snell’s Law

A

Determines degree of change of direction for refraction

Sin(i1)/v1 = sin(i2)/v2

36
Q

P-ray parameter

A

sin i1 / v1= sin i2 / v2= sin i3 / v3 … = constant = p= ray parameter. Used to deduce ray paths through Earth.

37
Q

Iasp91 Model

A

The model that displays P and S wave velocities throughout the depths of Earth

38
Q

P-ray shadow zone

A

98-144 degrees, caused by core refraction

39
Q

S-ray shadow zone

A

98-180 degrees, S-waves cannot travel through core

40
Q

Attenuation

A

Amplitude of seismic waves changes for two main reasons:
1. the wave front usually spreads out as it travels away from the source.

  1. If wave energy is absorbed, such as if rock is not fully elastic or S-waves entering rocks with some liquid
41
Q

Elastic rebound theory

A

explains how rocks store energy until it is suddenly released in an earthquake: b) strain accumulates (elastically); c) elastic limit is exceeded, the fault slips releasing the pressure; d) surface rupture and surface offsets releasing the pressure; d)surface rupture, and surface offsets

42
Q

Earthquake location

A

Traces recorded at seismograms from seismometer stations used to deduce location or origin time
If we use only time of first arrivals If we use only time of first arrivals(P-waves) at different stations we can deduce location.

43
Q

Fault-plane solutions

A

It is also possible to deduce the orientation of the fault plane and the direction of displacement in that plane and the direction of displacement in that plane

Beach ball example, like lab. Compress= +, Dilation= -
Strike strip = basic quadrant
normal fault = +,-,+
Thrust fault = -,+,-

44
Q

Rupture and displacement Principles

A

The ruptured area of a fault due to a large earthquake has a length along strike that is usually much greater than its depth
Earthquakes have rupture lengths up to hundreds of km, widths up to tens of km, and displacements up to tens of m

45
Q

Measures of earthquake size

A

Intensity, Mercalli Scale

Magnitude, Richter Scale, uses Log scale

46
Q

Seismic moment (M0)

A

Value = to the product of shear force, displacement, and rupture area.
and/or
equals the product of the shear forces (F) and the perpendicular distance between them (b)