Geol 492/692 - Surface-Wave Dispersion Analysis and Modeling Lab

John Louie, February 15, 2005
Copyright © 2000-2005 John N. Louie, all rights reserved.

Due: Feb. 16, 2005

Purpose

Surface-wave velocity spectra can determine shallow earth structure and contribute to the estimation of earthquake ground-shaking hazards. This exercise functions as a tutorial to detail how to analyze surface-wave data recorded on common seismic refraction equipment. The surface waves can arise from controlled sources, or from microtremor noise. See the Refraction Microtremor web page at www.seismo.unr.edu/remi for a listing of case histories, publications, and the field data-collection tutorials. This exercise does not describe much about how to derive a velocity structure from a dispersion curve, or how to interpret S-wave velocity structure for any particular purpose.

All SeisOpt®ReMiTM software is highly confidential, and has great commercial value. While students are allowed to use this package here at UNR for work in this course, any other use not specifically authorized in writing by me or by Optim LLC constitutes theft. Unauthorized copying of this software from our computers would subject you to academic disciplinary procedures, and perhaps civil and criminal penalties as well. That said, I encourage you to seek our permission to use SeisOpt®ReMiTM in your course, project, or thesis work here.

This writeup begins with a general description and links to explanations of procedures. I've annotated the links so you will know what parts of the procedures you need to do. The next part of the writeup lists your assignment, and contains the links to the data sets you will use.

Accessing SeisOpt®ReMiTM

You are welcome to log in to a Sun workstation or one of the PCs in LME 320. Use the login ``guest'' on the Suns; I will give you the password in class. On a Seismology workstation you will not have to download the disper or JRG programs; just start the programs with the commands ``Viewmat'' or ``Disper'' typed into a Terminal or Command Window (these commands are case-sensitive). These commercial software packages are not available for installation on your home computer or laptop.

Explanations of Procedures

There are several steps involved in getting some new data set from a seismograph to a computer where you can do the surface-wave analysis. These steps were broken down according to the kind of computer needed, for students who want to analyze their own data sets. Some of these steps have been done already, and you will not have to repeat them.

The main surface-wave analysis must be done on a UNR Seismology computer, with the commercial ReMi plug-in for the JRG package installed. On Seismo Suns (and our Macs if you have access to one) the Vspect package operates identically to the Viewmat package you got running for the previous lab exercise. On Seismo PCs with the full commercial license, the operation is somewhat different, so consult the accompanying manual. The last step of modeling the S-velocity structure is accomplished with another program called Disper, only slightly different between our academic and commercial versions.

  1. Convert the data from the seismograph. You will not have to do this for the lab exercise, since I have you download data examples from the assignment section.

  2. Obtain the Java software. You will not have to do this for this lab exercise, since you must use proprietary software installed on Seismology computers. The page does offer some helpful links.

  3. Run the velocity-spectrum analysis. This you will do for the lab exercise. Here you will be opening both SEG-Y and raw float data sets. The link here goes in after the instructions for opening the data file, but you will want to scroll up to those instructions when I give you a raw float data set. You will be instructed in the assignment to also apply geometry information.

  4. Model structure from the results. You will do this too. Where this page talks about labeling and tracing axes to make picks, you should realize that you can now use Viewmat's Pick Window to get picks exactly.

Assignment

  1. Analysis of surface waves on refraction records: First we will identify and analyze surface waves recorded in Dixie Valley during the same survey we analyzed for refraction picks last week. We collected it as a seismic reflection survey; you can see the many different purposes a good data set can be used for.
    1. Download two separate records in binary SEG-Y format: DIXI0106.sgy and DIXI0114.sgy. Record 114 is from a playa in the center of Dixie Valley while record 106 is from a shallow granite pediment (the Piedmont) at the edge of the basin.
      • You may have trouble getting a web browser to copy these binary files correctly. If you are doing this lab by logging into a Seismo Sun as ``guest'', I have already put these files into the ``surf'' sub-folder of guest's home directory. In Viewmat's Open Binary File dialogue you can look for them in ``/home/guest/surf''.
    2. Open each record separately in Viewmat. These SEG-Y files do have the 3600-byte reel header block present (so leave the box checked), but they still have IEEE/Java float and not IBM float trace sample data. Note that the first 24 channels are out of order. Apply the source-receiver geometry to each record, similar to how you applied geometries in the previous lab. For record 106, the single line of observer's report to use is ``0106 193 2 219 196 220 243''. For record 114, the observer's report is ``0114 53 2 76 53 77 100''. These observer's reports are not the same as what we used last week. They account for the trace ordering by defining two receiver patches, one reversed. For the station coordinates use the very same ``dixie-med-vp.txt'' file you used last week. Applying geometry ensures correct analysis but will not fix the reversed appearance of the plotted records. Note these records have 4 seconds total time.
    3. In Viewmat use the Pick Window to identify the following phases on record 114: P-wave refraction, direct S wave, Rayleigh wave. Report their approximate velocities. For information on surface waves see Telford et al. p. 153-154, 182. Do you see an air wave? What measurement would confirm its existence? Is there an air wave on record 106?
    4. Identify some spatial aliasing effects on record 114. Turn in a plot with the artifacts circled, or describe them.
    5. Now run the velocity-spectrum analysis on each record separately, for two different velocity-spectral plots. When you run the vspect method, note that you should confirm the correct source-receiver offset range for the record. Use the default Fmax and Vmin values, but increase Np to 48 for improved velocity resolution.
    6. Try several values for the clip levels of the velocity-spectral plots. Identify the Rayleigh-wave phase-velocity dispersion trend in each. Try to make a least a dozen picks along the center of the trend in each. If you see more than one trend, pick the lower-velocity trend, since the fundamental-mode Rayleigh waves we want to interpret have lower phase velocities than the higher-mode overtones. What is the lowest frequency at which you can get a good phase-velocity estimate for each record? Turn in the two picked, grayscale velocity-spectrum plots (or email color plots).
    7. Discuss briefly how well your Rayleigh-wave phase-velocity picks agree with the velocities of the waves you could observe directly in the record 114.
    8. Compare the phase velocities from the two records. How do they differ? Can you justify the difference from the information above about their recording locations?

  2. Comparison with last week's records:
    1. Load the data set used for the previous lab into Viewmat and apply geometry, just as you did before, using the observer's report lines from that lab.
    2. Run the velocity-spectrum analysis on all four records together, for one composite velocity-spectral plot. Note that the Methods menu has an On Each Plane sub-menu that contains the vspectSum command, since there are multiple records in this file.
    3. Compare the result to the velocity-spectral result from record 106 you got above. Versions of record 106 were used in both these analyses, yet they look very different. Explain what happened. Hint: frequency resolution is proportional to the duration of time recorded. It is not dependent on the time sampling interval.

  3. Analysis of microtremor noise. Here we look at a passive seismic record, taken without any active source. A 24-channel refraction layout was made along Mill St. in Reno, extending west from the corner with Rock Blvd. It was afternoon, and there was plenty of traffic.
    1. Download the rno-noise.flt 1.1 Mbyte data file, setting raw binary FTP mode if needed.
    2. Import the data into Viewmat. This file has the Raw Float format (just a stream of IEEE/Java floating-point binary trace amplitude values, no headers or labels) and is not SEG-Y. In the Open Binary File... dialog, set the Binary File Type to Raw Float. As the instructions describe, you need to know the number of bytes to skip from the beginning of the file (0), the number of samples per trace (elements per vector = 3000), the number of traces per record (vectors per plane = 24), and the number of records in the data file (number of planes = 4).
    3. Plot the record. The further instructions show how to apply an existing plot parameter file. Download the plrno-noise.par file (it is plain text). Now use the Edit menu on the data plot that came up, and select Apply Parameter File....
    4. Now you should be able to Animate and interpret the passive records. How many seconds long is each record? What is the aperture of the 24-channel spread? Since the receivers were in a straight line and evenly spaced, the plot parameter file actually defines the geometry well enough for this analysis.
    5. Examine the records to decide where their energy comes from. You'll notice a thick, fuzzy group of high-energy waves running almost the length of each record; some have more than one group. Estimate the apparent velocity of such a group - it will be very low. Make a few picks in Viewmat along the center of the group, and you will be able to compute the velocity easily. This is not a seismic wave-propagation velocity. Convert the velocity to miles/hour and you will be able to say what is propagating.
    6. Radiating from each group of fuzzy energy in these records are noticeable seismic waves that have reasonable velocities - 100 to several hundred meters/sec. Turn in a plot of one record (email is OK) where you have made a couple of picks of one such wave, and computed its velocity.
      (If you cannot plot the record in Viewmat, look at this PDF plot.)
    7. Now run the velocity-spectrum analysis on all four records together, for one composite velocity-spectral plot. When you run the vspect method, note that you should confirm the correct dt=0.016 s and dx=15.24 m. Use the default Fmax and Vmin values, but increase Np to 48 for improved velocity resolution.
    8. Adjust the clip level of the velocity-spectral plot, identify the surface-wave dispersion trend, and try to make a least a dozen picks along the trend. Pick the lowest velocity reasonable, since a passive array records energy from all directions, and any energy not propagating in the array direction will have an artificially high apparent velocity. What is the lowest frequency you can get a good phase-velocity estimate for? Turn in a picked, grayscale plot (or email a color plot).
      (If you cannot plot the vspect result in Viewmat, look at this PDF plot.)
    9. Discuss briefly how well your Rayleigh-wave phase-velocity picks agree with the velocities of the waves you could observe directly in the noise record.
    10. Estimate the wavelength of a Rayleigh wave that samples 0-30 m depth S-wave velocities best (Hint: it is more than 30 m). Justify your estimate briefly with one of: surface-wave or skin-depth theory (e.g. Aki and Richards p. 259-267); references from the engineering literature (the Stokoe papers are useful); or simple principles of wave propagation (e.g. Telford et al. p. 149, 153-154). Identify from your velocity-spectral picks a frequency and phase-velocity combination that matches that wavelength, and report your estimate for the 0-30 m depth average S-wave velocity at Rock and Mill.
    11. Examine the soil-type classifications for earthquake ground-shaking hazard mapping found at:
      • Seekins, Linda C. , Boatwright, Jack, and Fumal, Tom, 1999, Soil type and shaking hazard in the San Francisco Bay Area: U.S. Geological Survey web site at http://quake.wr.usgs.gov/hazprep/soil_type/ (the classification table is a popup link on the left side of the page).
      Using your 0-30 m velocity estimate, report the ground-shaking hazard classification for Rock and Mill (don't call any newspapers; we already know). Now you have boiled 1.1 megabytes of data down to one letter.

  4. Modeling S-velocity structure.
    1. Follow these instructions to do the modeling yourself with the Disper module on a Seismology workstation.
    2. Report the maximum depth your dispersion data constrain velocities to.
    3. Report any attempts to evaluate velocity-depth trade-offs.
    4. Briefly compare the two velocity structures from records 106 and 114, and justify these differences in terms of the local geology I described above.