| Seismometer
current
data,
uploaded
hourly (time is UTC-7h) |
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Observations:
1. 3/21/10 Sensitivity appears to be improved with the
longer
pendulum - 39 inches versus 9 inches in V1.0. But the sensitivity
has
come with a cost. It appears that any slow change in temperature
sets
up a thermal gradient within the enclosure, with
accompanying oscillation at a frequency of about 2 cycles per
minute.
Peak amplitude is about 5% of full-scale. This is the effective
noise
floor until I can find a way to reduce this artifact. Foam
insulation
between the top opening and its cover helps. The artifact is not
electronic in nature - the same circuit in the V1.0 enclosure
never
exhibited the behavior.
2. 04/06/10 M7.7 Sumatra quake recorded, distance 9400 mi.,
shows significantly improved sensitivity over the previous V1.0
mechanical design.
3. 01/06/11 Removed the 802.11g access node and
hardwired the seismometer USB bridge to ethernet, lowering the
incidence of data packet loss.
4. 02/24/11 A year's worth of data has given a better indication of the sensitivity. A M6.2 quake in Spain was at the limit of sensitivity at 5220 miles distance, while a M6.9 quake in New Guinea registered a peak response of 10% of full scale over a 6920 mile path. A M7.7 quake over a 9400 mile path made a response of 50% of full scale. Because each decrease of 0.2 in magnitude is a halving of energy, that quake would have been detectable at M7.0. Finally, the Feb 21, 2011 M6.3 quake in Christchurch, New Zealand was, after inspection, undetectable in the data - a path length of 6300 mi.
Given this, it seems that the instrument is
able
to detect a M7.0 quake from
just about anywhere. The present limit to sensitivity is
entirely mechanical - mostly the response of the pendulum frame to
thermal input. Increasing sensitivity further will require
improvement
in the mechanical design.
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The completed seismometer board. To the right you can
see the
IR emitter, magnet assembly and differential
photodetector. From right
to left, in order: 1) Photodiode transimpedance amplifier/filter (dc-coupled, abbreviated "TZA" in the dataplots) 2) Instrumentation amplifier and HPF 3) Sallen-Key LPF 4) SE-to-balanced output buffer to DAQ board. The response characteristic is bandpass, with passband of 0.008 to 3 Hz. |
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Seismometer in its enclosure. The board is mounted on
top of
a 10 inch circular aluminum base plate, about 1/2 inch
thick. Mount
point screws are tapped and threaded, providing a means
for adjusting
tilt. The pendulum wire, 5-mil dia tungsten, is suspended from the top of a rigid square aluminum pipe one meter long. Height adjustment is provided by a threaded set screw with a knob attached. |
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Seismometer enclosure.
The
DAQ board, USB-IP converter and WiFi access node are on
top of the
cabinet to the right. The enclosure proper is a 10 inch spiral-wound cardboard cast form for concrete, 4 feet tall. Cost: about $12 at Lowe's hardware. It is thermally isolated on both ends with foam rubber. The top opening is covered by a sheet of foam with plywood on top. |
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Detail of the torsion
balance, showing how the copper weights are suspended
between the
rare earth magnets. With a meter-long pendulum, the motion
is slower
and the magnets provide insufficient damping alone. The
small nut at
the bottom of the tungsten wire in the photo, is now
suspended in a
vial of mineral oil for extra damping. A long pendulum is sensitive, but the mechanical design has some flaws: - It has multiple modes of response: lateral motion of the weight as well as twisting motion. In a long pendulum the lateral motion dominates, so it's really not a tosrion balance. - Sensitivity is affected by the angle and height of the flag at the point where the input integrator is centered. This makes calibration impractical. - The pennies and the end nut on the pendulum make for two separate resonances, which can be seen in FFT plots when damping is removed. Fewer natural resonances are better. - A meter-long pendulum combined with electronics which can detect microns of motion, is hard to stabilize mechanically. There are several joints between aluminum and steel, which have different thermal coefficients of expansion. One or more of these, I suspect, creates a low-level thermal relaxation oscillation at 0.02 - 0.04 Hz which can be seen in the raw data. It tends to appear whenever there's a thermal gradient dT/dt in the garage. It's suppressed by numerical filtering, but better to suppress it at the source. |
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This is the first large
quake
detected by the V2 seismometer. The M7.7 quake in Sumatra
on 4/6/10,
distance
9400 mi. made a response peak of 60% of full-scale. The
distance record
for V1.0 was the M8.0 quake in American Samoa in Sept
2009, a much
weaker
response at 5000 mi. distance. The surface wave frequency is about 0.07 Hz - a very low frequency typical for the large quakes. Prior to this quake, well over 50 aftershocks have been recorded to date from the M7.2 Baja California quake of 04/04/10, some as low as M2.0. |
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USGS seismic wave travel
times for
the M7.7 quake, 4/6/10. |
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This M6.2 quake in
southern
Spain on 4/11/2010 is at the limit of sensitivity for
detection. The
pressure and
shear wave components labeled P and S can only be seen in
this zoom
plot, superimposed against the instrument's own
twice-per-minute
mechanical thermal oscillation - a flaw which I still must
correct. This is a milestone for me. This device was born because my wife Pam was in Italy when the M6.7 quake struck in L'Aquila in April 2009. My goal was to be able to detect that quake from that distance, and it appears now to have been achieved. Now on to curing the thermal/mechanical oscillation - (which wont be easy if the required thermal isolation for the enclosure is too high). |
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USGS seismic
wave
travel
times for
the M6.2 Andalusia quake, 4/12/10 (UTC). The times for P
and S agree
with the recorded arrivals to within seconds. Nomenclature for the phases of seismic waves is given here. The P waves are pressure (longitudinal) waves which travel in a linear path beneath the Earth's crust. The S waves are shear transverse waves which propagate at a slower speed than the P wave. LQ and LR are surface waves which propagate along the curvature of the Earth's crust - a longer path. |
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The
M6.9 at
Papua New Guinea July 18, 2010, was one of three closely
spaced quakes,
and had the best definition from the garage detector.
There are 4 identifiable phases: P is the initial pressure
wave
arrival, PKiKP is the same wave bouncing from the Earth's
inner core
boundary, S is the shear wave, and LQ is the surface wave.
The surface
waves are always lower in frequency, and typically the
strongest
signals from a distant quake. Distance 6920 miles. |
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This large M7.6
earthquake in
the
Philippines on July 23, 2010 was atypical in that its
epicenter was
600km below the
earth's surface. Little damage was reported. Note also
that the
normally strong surface waves LQ and LR are not prominent. |
| Mindanao
Mag
7.6
Quake
Audio
recording
at
250x
speed |
This is an audio file of
the
Mindanao M7.6 quake with a
superimposed image of the 22 second waveform made by
playing the quake
datafile at a sample rate of 3072 Hz, (about 250 times the
actual
sample rate). It sounds a bit like rolling thunder. |
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Ecuador M6.9 quake, Aug
12,
2010, 0454 PDT, distance 3360 miles. This quake occurred
in a sparsely
populated area east of the Andes, facing the Amazon
tropical forest. P = initial body wave. S = transverse shear wave. sPKiKP = the same shear wave reflected off of the earth's inner core. LQ and LR are the surface waves. An audio recording of this event, compressing 48 minutes into 12 seconds, is here. |
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This is the M 9.0 quake
90
mi NE of Sendai, Japan, 03/11/11. The pressure wave
arrived just after
22:58:30 MST here 03/10/11. I happened to be at the
computer at the
time. When it started arriving, the pressure wave was strong enough that I thought it was in one of the more local hot spots in the Gulf of California. By the time the shear waves started arriving, a check with the USGS KML overlay for Google Earth showed a M7.9 off the Honshu coast near Sendai. The instrument had picked up a M7.2 from that spot two nights earlier. I made two postings of the plots as they were building, on Facebook. An hour after onset, the USGS amended their initial M7.9 estimate to M8.8, then to M8.9. That full point in magnitude is a 32-times increase in energy. On 03/14/11, USGS refined its measurement to M9.0. Tempe arrival times and a more detailed plot of this quake are shown below. |
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USGS
seismic wave travel times to Tempe, AZ. The initial
arrival time was
accurate to within a few seconds. One notable detail in this printout: predicted peak amplitude for the surface waves was over 1/2 centimeter. That's ground movement in Tempe from a quake 5900 miles distant. I have good reason to believe that we did indeed see that motion here. GPS measurements showed that the land mass of Honshu Island (the main island of Japan) shifted by 8 feet after the quake. |
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A closer look at the
Honshu
M9.0 quake of 03/11/11. The P group is the pressure wave.
S is the slower traveling shear wave and LQ is the guided
surface wave
that dominates the response in powerful, distant quakes.
Because the
surface wave is constrained between layers of the Earth's
crust, it
weakens more gradually with distance. Besides the large magnitude of this record there is one other interesting detail, highlighted by the green arrow. The blue-colored trace of the preamplifier response shows activity at the onset of surface wave arrival. The preamp is at 200-400 times lower gain than the output. I normally see a response in the blue trace only when I park my car on the same concrete slab as the seismometer - the car changes the tilt of the slab. This makes a 1/2 centimeter peak ground motion plausible. Since it occured over a 20 second period, it normally would not have been felt. |
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Since it's rare to witness a piece of (geological) history as it's happening, I've posted two screen captures of Facebook threads I sent out as the seismic energy was arriving from the M 9.0 Honshu quake. The pressure wave arrived at 10:58:35 PM MST in Tempe on 03/10/11. The timestamps on the threads are one hour early because Facebook erroneously applied Daylight Savings Time retroactively, to a date before DST was in effect, to Arizona which doesn't observe DST. |
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I posted the second thread after it became apparent this was a very large event and I had a more descriptive plot of the signal arriving. Having direct access to a seismometer meant I could poll USGS as soon as I suspected amendments to their measurements, which is common as quakes are occurring. I could post news before news organizations had it. I have friends who have friends/family in the Pacific, so I wanted to get tsunami info out on the thread for this large offshore quake. The US suffered one fatality on the Calif. coastline, and significant damage to small boats in a few harbors. To put historical context on the human cost of this quake, the single best article I've read comes from a historian who lived in that area of Japan. |
Notes:
1. Another example of a torsion balance seismometer may be found
here .
2. A torsion pendulum is a special case of a compound
pendulum. The two main handles on the resonant frequency are
the
moment of inertia of the weight, and the torsion constant of the
wire
(inversely proportional to the wire cross-sectional area).
3. A schematic diagram for this design is here.
The
seismometer
is
completely
powered
off
of
the
5V
USB
bus
from
the
Labjack
U12 12-bit data acquisition
board. Supply current consumption is under 100 mA. Note: U3A
should be
an OP284 and not an MC33202, since low offset is needed in the
feedback
path. U1 and U3 have been changed to OP284, which has greatly
reduced
1/f noise in the seismic frequency range down to 0.01 Hz. The IR
photodiodes are Vishay BPV23NF, which are inexpensive, sensitive,
and
have a helpful daylight blocking filter integrated in the package.