WEBVTT
e1a6d0f5-c720-4206-b6ae-9c1973856016/38-0
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Ok, happy to introduce Martijn
van den Ende.
e1a6d0f5-c720-4206-b6ae-9c1973856016/47-0
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From the Université Côte d'Azur
in southern France. Where he's a
e1a6d0f5-c720-4206-b6ae-9c1973856016/47-1
00:00:13.636 --> 00:00:13.943
post-doc
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there as well.
e1a6d0f5-c720-4206-b6ae-9c1973856016/90-0
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In rock mechanics that tracks
university master's and
e1a6d0f5-c720-4206-b6ae-9c1973856016/90-1
00:00:21.117 --> 00:00:24.837
bachelors in Urban Sciences,
please work on a number of
e1a6d0f5-c720-4206-b6ae-9c1973856016/90-2
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topics from Earth made cycle
modeling, possible seismology,
e1a6d0f5-c720-4206-b6ae-9c1973856016/90-3
00:00:28.823 --> 00:00:32.943
raycasting, and deep learning,
which is Helen with this work.
e1a6d0f5-c720-4206-b6ae-9c1973856016/101-0
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One thing I really appreciate
about work is limited to his
e1a6d0f5-c720-4206-b6ae-9c1973856016/101-1
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Open Access research.
e1a6d0f5-c720-4206-b6ae-9c1973856016/114-0
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Umm, so there are number of
things in this area, but umm
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also mention two.
e1a6d0f5-c720-4206-b6ae-9c1973856016/142-0
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The first things most people do
is the boundary line in Open
e1a6d0f5-c720-4206-b6ae-9c1973856016/142-1
00:00:46.598 --> 00:00:50.365
Access journals seismicode,
which has been a global effort
e1a6d0f5-c720-4206-b6ae-9c1973856016/142-2
00:00:50.365 --> 00:00:53.303
to have Open Access publishing
in seismology.
e1a6d0f5-c720-4206-b6ae-9c1973856016/160-0
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One cool thing about that is
there's the meeting article that
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kind of interests the journals
in five of the abstracts in
e1a6d0f5-c720-4206-b6ae-9c1973856016/160-2
00:01:00.387 --> 00:01:01.383
languages purely.
e1a6d0f5-c720-4206-b6ae-9c1973856016/179-0
00:01:03.143 --> 00:01:06.284
Second thing, how to begin this
work to run this paper on
e1a6d0f5-c720-4206-b6ae-9c1973856016/179-1
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graphical networks is really
interested in how did it.
e1a6d0f5-c720-4206-b6ae-9c1973856016/195-0
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So we'll just get a page and
we'll be able to post it the
e1a6d0f5-c720-4206-b6ae-9c1973856016/195-1
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full model and training code. So
it's easy to see what you're
e1a6d0f5-c720-4206-b6ae-9c1973856016/195-2
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done.
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So I think that's it.
e1a6d0f5-c720-4206-b6ae-9c1973856016/207-0
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Posting code kind of full access
to.
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Service attacked in multiple
seismology and just community
e1a6d0f5-c720-4206-b6ae-9c1973856016/237-1
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efforts is going to receive the
2024 KA work in about two to
e1a6d0f5-c720-4206-b6ae-9c1973856016/237-2
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outstanding early career
seismologist.
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Us to monitor a number of
phenom.
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En traffic, aftershock sequences
and phenomena, these are folks
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today on potential DAS perfect
early in the morning, until this
e1a6d0f5-c720-4206-b6ae-9c1973856016/265-2
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talk is EW.
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What about the dynamic range so
that we get?
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Alright. Well thank you, Tim and
thank you also for the
e1a6d0f5-c720-4206-b6ae-9c1973856016/288-1
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invitation to to present here.
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I would like to begin by
introducing you to the Abyss
e1a6d0f5-c720-4206-b6ae-9c1973856016/308-1
00:02:13.445 --> 00:02:17.423
team, which hopefully now you
can see over here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/345-0
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So the Abyss project is a
project funded by the ERC, which
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is the European Research
Council, and the objective, the
e1a6d0f5-c720-4206-b6ae-9c1973856016/345-2
00:02:26.527 --> 00:02:30.623
main objective of this project
is to monitor mega trust faults.
e1a6d0f5-c720-4206-b6ae-9c1973856016/348-0
00:02:31.383 --> 00:02:32.703
With fiber optic cables.
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And so within this team, led by
Diane River, we have Marie, who
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is in charge of data management
and transfer.
e1a6d0f5-c720-4206-b6ae-9c1973856016/381-0
00:02:43.103 --> 00:02:49.223
We have a postdoc, Alastair and
Yuqing and PhD student Clara.
e1a6d0f5-c720-4206-b6ae-9c1973856016/400-0
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And the three sort of main work
packages of this project are,
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first of all to detect weak
cycling.
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00:03:01.363 --> 00:03:05.051
Make seismic signals and
complement online sizing
e1a6d0f5-c720-4206-b6ae-9c1973856016/419-1
00:03:05.051 --> 00:03:08.003
networks with offshore
instrumentation.
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00:03:08.163 --> 00:03:10.003
So that is DAS cables.
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The second objective is to
monitor the crust for precursory
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00:03:14.897 --> 00:03:16.603
seismic velocity changes.
e1a6d0f5-c720-4206-b6ae-9c1973856016/455-0
00:03:16.883 --> 00:03:21.041
So essentially the preparation
phase of large earthquakes and
e1a6d0f5-c720-4206-b6ae-9c1973856016/455-1
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the first one that I'm going to
talk about today is to develop
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00:03:25.266 --> 00:03:25.803
the 1st.
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Prototype of offshore Das
Earthwake early warning in
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00:03:30.427 --> 00:03:30.863
Chile.
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So to give you a bit of context
of the project, we are situated
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in Chile, so this is the map we
are focusing on this rectangle
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over here in the centre of Chile
where we have access to three
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offshore dask cables. These sort
of red little wires that.
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You see here.
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These are sensitive 3 up to DAS
interrogate units. As you can
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see over here.
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For a total of about 450
kilometers.
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And the location of the the
project is not by accident
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because here we have some major
seismic gaps.
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So there is a real possibility
that within the duration of the
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project there are some large
earthquakes occurring in this
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00:04:23.933 --> 00:04:24.383
region.
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00:04:25.983 --> 00:04:29.654
On top of these three
permanently installed
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00:04:29.654 --> 00:04:30.823
interrogators.
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We will also soon have one
travelling interrogator that
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00:04:35.527 --> 00:04:39.551
moves S to north or back to do
temporary deployments to
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00:04:39.551 --> 00:04:43.863
characterise local seismicity
and and cross off properties.
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00:04:45.423 --> 00:04:49.276
And off the data that are being
generated in this project are
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transferred to France daily with
a sort of a daily
e1a6d0f5-c720-4206-b6ae-9c1973856016/638-2
00:04:52.446 --> 00:04:54.063
synchronization procedure.
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00:04:57.213 --> 00:05:02.211
We acquire the data at a special
sampling rates of about 15
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00:05:02.211 --> 00:05:06.293
metres and a temporal sampling
rate of 62 Hertz.
e1a6d0f5-c720-4206-b6ae-9c1973856016/697-0
00:05:06.293 --> 00:05:10.797
So if you then work out the
maths, that amounts to about 300
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00:05:10.797 --> 00:05:15.302
gigabytes of data per day, or
about half a petabytes of data
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00:05:15.302 --> 00:05:20.028
over the periods of five years.
And so for this, we have plenty
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00:05:20.028 --> 00:05:24.163
of storage and processing
capacities at zero by zero to
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00:05:24.163 --> 00:05:24.533
deal.
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00:05:24.533 --> 00:05:25.013
With the data.
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00:05:26.103 --> 00:05:30.416
But on top of the daily
transfers that's transferred the
e1a6d0f5-c720-4206-b6ae-9c1973856016/730-1
00:05:30.416 --> 00:05:35.336
roll data to France, we also are
experimenting with sort of live
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00:05:35.336 --> 00:05:36.623
transfer of data.
e1a6d0f5-c720-4206-b6ae-9c1973856016/757-0
00:05:37.423 --> 00:05:41.028
So for this we have set up a
live stream on YouTube, which
e1a6d0f5-c720-4206-b6ae-9c1973856016/757-1
00:05:41.028 --> 00:05:44.939
unfortunately doesn't work right
now, but hopefully in the near
e1a6d0f5-c720-4206-b6ae-9c1973856016/757-2
00:05:44.939 --> 00:05:48.849
future it will work again. But
in our office we have actually a
e1a6d0f5-c720-4206-b6ae-9c1973856016/757-3
00:05:48.849 --> 00:05:51.783
screen that shows the data
coming in real time.
e1a6d0f5-c720-4206-b6ae-9c1973856016/765-0
00:05:52.583 --> 00:05:55.543
So here we have an earthquake
and Marie probably presenting.
e1a6d0f5-c720-4206-b6ae-9c1973856016/773-0
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The the data coming in in real
time.
e1a6d0f5-c720-4206-b6ae-9c1973856016/797-0
00:05:59.963 --> 00:06:04.561
Now, the reason why we're doing
this experimentation with the
e1a6d0f5-c720-4206-b6ae-9c1973856016/797-1
00:06:04.561 --> 00:06:08.714
live data transfer is of course
to work on the topic of
e1a6d0f5-c720-4206-b6ae-9c1973856016/797-2
00:06:08.714 --> 00:06:10.643
earthquake really warning.
e1a6d0f5-c720-4206-b6ae-9c1973856016/810-0
00:06:12.183 --> 00:06:15.501
And there are lots of advantages
of using DAS for earthquake
e1a6d0f5-c720-4206-b6ae-9c1973856016/810-1
00:06:15.501 --> 00:06:16.263
early warning.
e1a6d0f5-c720-4206-b6ae-9c1973856016/841-0
00:06:17.943 --> 00:06:22.185
First of all, we can use DAS to
complements sometimes very
e1a6d0f5-c720-4206-b6ae-9c1973856016/841-1
00:06:22.185 --> 00:06:26.860
sparse coverage of seismometers.
So particularly in the northern
e1a6d0f5-c720-4206-b6ae-9c1973856016/841-2
00:06:26.860 --> 00:06:31.103
parts of the region where we're
working, we have very few.
e1a6d0f5-c720-4206-b6ae-9c1973856016/865-0
00:06:31.663 --> 00:06:36.491
Land stations and so the special
coverage is very sparse and in
e1a6d0f5-c720-4206-b6ae-9c1973856016/865-1
00:06:36.491 --> 00:06:40.263
addition to that we get offshore
instrumentation.
e1a6d0f5-c720-4206-b6ae-9c1973856016/893-0
00:06:40.263 --> 00:06:44.162
So we are closer to the trench
and closer to the seasick
e1a6d0f5-c720-4206-b6ae-9c1973856016/893-1
00:06:44.162 --> 00:06:48.130
source. We can use existing
infrastructures because we're
e1a6d0f5-c720-4206-b6ae-9c1973856016/893-2
00:06:48.130 --> 00:06:52.508
using dark fibre here, so we do
not have any deployment and and
e1a6d0f5-c720-4206-b6ae-9c1973856016/893-3
00:06:52.508 --> 00:06:54.903
maintenance costs related to
that.
e1a6d0f5-c720-4206-b6ae-9c1973856016/907-0
00:06:56.463 --> 00:07:00.924
And lastly, the acquisition and
processing of the data takes
e1a6d0f5-c720-4206-b6ae-9c1973856016/907-1
00:07:00.924 --> 00:07:01.583
place in.
e1a6d0f5-c720-4206-b6ae-9c1973856016/917-0
00:07:02.103 --> 00:07:03.743
And earthquake proof
environment.
e1a6d0f5-c720-4206-b6ae-9c1973856016/934-0
00:07:04.063 --> 00:07:08.166
The interrogators are placed in
server rooms that serve as
e1a6d0f5-c720-4206-b6ae-9c1973856016/934-1
00:07:08.166 --> 00:07:11.783
central hubs for communication
in case of disaster.
e1a6d0f5-c720-4206-b6ae-9c1973856016/949-0
00:07:12.303 --> 00:07:16.554
So they are really designed to
withstand even the strongest of
e1a6d0f5-c720-4206-b6ae-9c1973856016/949-1
00:07:16.554 --> 00:07:20.063
earthquakes and be operational
during those events.
e1a6d0f5-c720-4206-b6ae-9c1973856016/975-0
00:07:21.623 --> 00:07:26.043
So after setting up the
interrogators last year, we were
e1a6d0f5-c720-4206-b6ae-9c1973856016/975-1
00:07:26.043 --> 00:07:30.540
sort of hoping between quotes
for a magnitude 6 or larger
e1a6d0f5-c720-4206-b6ae-9c1973856016/975-2
00:07:30.540 --> 00:07:34.263
earthquake to occur within a
five years period.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1004-0
00:07:35.803 --> 00:07:39.799
And so two months later, our
prayers were heard and a
e1a6d0f5-c720-4206-b6ae-9c1973856016/1004-1
00:07:39.799 --> 00:07:43.869
magnitude 6.6 earthquake
occurred right at the edge of
e1a6d0f5-c720-4206-b6ae-9c1973856016/1004-2
00:07:43.869 --> 00:07:47.643
one of the three cables that we
are instrumenting.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1008-0
00:07:48.483 --> 00:07:51.043
So here we have the three
cables.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1015-0
00:07:51.043 --> 00:07:53.963
That's that we are that are
located offshore.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1029-0
00:07:54.683 --> 00:07:57.472
Earthquake was here in the
north, and so we have this
e1a6d0f5-c720-4206-b6ae-9c1973856016/1029-1
00:07:57.472 --> 00:08:00.003
beautiful propagation of the
seismic waves from.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1039-0
00:08:00.863 --> 00:08:04.724
North to South here on the
slides, we have N on the left
e1a6d0f5-c720-4206-b6ae-9c1973856016/1039-1
00:08:04.724 --> 00:08:05.063
side.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1044-0
00:08:05.593 --> 00:08:09.313
And South on the right and time
is is moving up.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1075-0
00:08:10.863 --> 00:08:15.103
And so this look very promising
and this this look like
e1a6d0f5-c720-4206-b6ae-9c1973856016/1075-1
00:08:15.103 --> 00:08:19.571
fantastic data to try early
warning algorithms etcetera on
e1a6d0f5-c720-4206-b6ae-9c1973856016/1075-2
00:08:19.571 --> 00:08:24.039
and some of the data looked
really nice, but unfortunately
e1a6d0f5-c720-4206-b6ae-9c1973856016/1075-3
00:08:24.039 --> 00:08:26.463
most of the data look like this.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1082-0
00:08:28.143 --> 00:08:29.943
So clearly here something is
wrong.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1088-0
00:08:30.143 --> 00:08:32.863
The amplitudes are clips and.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1090-0
00:08:34.423 --> 00:08:34.463
This.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1102-0
00:08:35.273 --> 00:08:38.473
Prompted us to ask a couple of
questions on OK.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1114-0
00:08:38.473 --> 00:08:42.473
How feasible is it to use DAS
for earthquake warning?
e1a6d0f5-c720-4206-b6ae-9c1973856016/1142-0
00:08:44.063 --> 00:08:47.613
And so some of the main
questions that we had was well,
e1a6d0f5-c720-4206-b6ae-9c1973856016/1142-1
00:08:47.613 --> 00:08:51.608
why are these DAS measurements,
clips or saturated as we as we
e1a6d0f5-c720-4206-b6ae-9c1973856016/1142-2
00:08:51.608 --> 00:08:52.623
tend to call it?
e1a6d0f5-c720-4206-b6ae-9c1973856016/1152-0
00:08:53.423 --> 00:08:57.646
And what is the big round
displacement or velocity or
e1a6d0f5-c720-4206-b6ae-9c1973856016/1152-1
00:08:57.646 --> 00:08:58.663
acceleration?
e1a6d0f5-c720-4206-b6ae-9c1973856016/1168-0
00:09:00.383 --> 00:09:03.728
That that triggers this
saturation or other words, what
e1a6d0f5-c720-4206-b6ae-9c1973856016/1168-1
00:09:03.728 --> 00:09:04.863
is the maximum bgd.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1195-0
00:09:05.783 --> 00:09:11.254
HGV PGA that we can measure with
us and be more precisely what is
e1a6d0f5-c720-4206-b6ae-9c1973856016/1195-1
00:09:11.254 --> 00:09:15.813
the maximum magnitude of an
event that we can reliably
e1a6d0f5-c720-4206-b6ae-9c1973856016/1195-2
00:09:15.813 --> 00:09:17.223
measure with DAS?
e1a6d0f5-c720-4206-b6ae-9c1973856016/1230-0
00:09:19.183 --> 00:09:22.930
So to answer the first question,
that's actually relatively
e1a6d0f5-c720-4206-b6ae-9c1973856016/1230-1
00:09:22.930 --> 00:09:26.739
straightforward. If you look at
the measurement principle of
e1a6d0f5-c720-4206-b6ae-9c1973856016/1230-2
00:09:26.739 --> 00:09:30.611
DAS, what does measures is the
phase of of light or the phase
e1a6d0f5-c720-4206-b6ae-9c1973856016/1230-3
00:09:30.611 --> 00:09:34.358
difference between consecutive
processes of lights that are
e1a6d0f5-c720-4206-b6ae-9c1973856016/1230-4
00:09:34.358 --> 00:09:34.983
sent down.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1259-0
00:09:35.753 --> 00:09:39.572
An optical fiber and the
relation between the face that
e1a6d0f5-c720-4206-b6ae-9c1973856016/1259-1
00:09:39.572 --> 00:09:43.528
you measure and the sort of
length of the trajectory that
e1a6d0f5-c720-4206-b6ae-9c1973856016/1259-2
00:09:43.528 --> 00:09:46.393
the light follows is a simple
linear one.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1279-0
00:09:46.393 --> 00:09:51.377
So here on the left we have the
phase diodes by Phi. The
e1a6d0f5-c720-4206-b6ae-9c1973856016/1279-1
00:09:51.377 --> 00:09:55.313
distance of the light travels
here is D and.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1299-0
00:09:56.943 --> 00:10:01.103
The the proportionality constant
here in the middle contains the
e1a6d0f5-c720-4206-b6ae-9c1973856016/1299-1
00:10:01.103 --> 00:10:05.007
refractive index photo as the
coefficient and the wavelength
e1a6d0f5-c720-4206-b6ae-9c1973856016/1299-2
00:10:05.007 --> 00:10:05.583
of light.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1318-0
00:10:07.033 --> 00:10:11.666
And because there's a linear
relationship, we can split this
e1a6d0f5-c720-4206-b6ae-9c1973856016/1318-1
00:10:11.666 --> 00:10:14.553
in a reference phase measurement
and.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1329-0
00:10:16.263 --> 00:10:19.303
A deviation or a change in the
length of the trajectory.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1336-0
00:10:21.103 --> 00:10:23.303
Now normally we don't want to
deal with this reference.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1373-0
00:10:25.263 --> 00:10:29.283
Phase so we can get rid of that
by time differentiation and
e1a6d0f5-c720-4206-b6ae-9c1973856016/1373-1
00:10:29.283 --> 00:10:32.901
likewise we want our
measurements to be local, so not
e1a6d0f5-c720-4206-b6ae-9c1973856016/1373-2
00:10:32.901 --> 00:10:36.921
affected by everything that
happens before in the cable and
e1a6d0f5-c720-4206-b6ae-9c1973856016/1373-3
00:10:36.921 --> 00:10:38.463
we can achieve that by.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1415-0
00:10:39.223 --> 00:10:43.229
Differentiating this
relationship in space, and so
e1a6d0f5-c720-4206-b6ae-9c1973856016/1415-1
00:10:43.229 --> 00:10:48.021
typically what does instrument
records, is this quantity the
e1a6d0f5-c720-4206-b6ae-9c1973856016/1415-2
00:10:48.021 --> 00:10:52.656
gradient of the phase rate,
which is still proportional to
e1a6d0f5-c720-4206-b6ae-9c1973856016/1415-3
00:10:52.656 --> 00:10:57.447
the change in the length of the
cable, and so in a way it is
e1a6d0f5-c720-4206-b6ae-9c1973856016/1415-4
00:10:57.447 --> 00:11:00.983
proportional more or less to the
to the STR.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1417-0
00:11:00.983 --> 00:11:01.103
Rate.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1456-0
00:11:04.363 --> 00:11:08.885
Any facial measurement is
periodic around ±π, so as a
e1a6d0f5-c720-4206-b6ae-9c1973856016/1456-1
00:11:08.885 --> 00:11:13.911
result this quantity that we are
recording is bounded by by
e1a6d0f5-c720-4206-b6ae-9c1973856016/1456-2
00:11:13.911 --> 00:11:19.271
divided by Delta T, Delta X and
here Delta T is the the rate at
e1a6d0f5-c720-4206-b6ae-9c1973856016/1456-3
00:11:19.271 --> 00:11:22.203
which you are requiring your
data.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1465-0
00:11:22.203 --> 00:11:26.523
So the sampling rate and delta X
is the spatial sampling.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1476-0
00:11:28.583 --> 00:11:32.863
And so if we now use this, this
sort of upper bound.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1486-0
00:11:33.763 --> 00:11:36.083
Plug it back into the equation
as you had on a previous slide.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1499-0
00:11:36.083 --> 00:11:39.658
Then this gives us that we get
the maximum strain rate that we
e1a6d0f5-c720-4206-b6ae-9c1973856016/1499-1
00:11:39.658 --> 00:11:40.283
can record.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1516-0
00:11:41.823 --> 00:11:45.629
Is is given by this relationship
which contains this something
e1a6d0f5-c720-4206-b6ae-9c1973856016/1516-1
00:11:45.629 --> 00:11:47.503
rate and and special something.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1533-0
00:11:49.873 --> 00:11:53.223
And if we plug in some
reasonable numbers for the
e1a6d0f5-c720-4206-b6ae-9c1973856016/1533-1
00:11:53.223 --> 00:11:57.444
wavelength of light and these
two parameters together of order
e1a6d0f5-c720-4206-b6ae-9c1973856016/1533-2
00:11:57.444 --> 00:11:57.713
one.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1535-0
00:11:59.263 --> 00:11:59.303
A.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1550-0
00:11:59.303 --> 00:12:02.279
Times sampling rate of about
kilohertz and a special sampling
e1a6d0f5-c720-4206-b6ae-9c1973856016/1550-1
00:12:02.279 --> 00:12:02.903
of 10 meters.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1558-0
00:12:03.303 --> 00:12:06.771
This gives us a upper bound on
the strain rate that we can
e1a6d0f5-c720-4206-b6ae-9c1973856016/1558-1
00:12:06.771 --> 00:12:07.183
record.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1572-0
00:12:08.783 --> 00:12:12.723
Of around 40 micro strain per
second. So micrometer per meter
e1a6d0f5-c720-4206-b6ae-9c1973856016/1572-1
00:12:12.723 --> 00:12:13.423
per second.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1583-0
00:12:15.143 --> 00:12:18.171
And if we then compare that with
our actual measurements, we see
e1a6d0f5-c720-4206-b6ae-9c1973856016/1583-1
00:12:18.171 --> 00:12:19.383
that it works really well.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1591-0
00:12:20.523 --> 00:12:23.523
So here the values here on the
vertical axis.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1612-0
00:12:25.303 --> 00:12:27.933
Denote the strain rate but with
lower values because the
e1a6d0f5-c720-4206-b6ae-9c1973856016/1612-1
00:12:27.933 --> 00:12:30.656
acquisition settings were a bit
different than what I just
e1a6d0f5-c720-4206-b6ae-9c1973856016/1612-2
00:12:30.656 --> 00:12:31.903
plugged into as an example.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1634-0
00:12:32.583 --> 00:12:36.387
But here what we have is actual
data from the swell, so the the
e1a6d0f5-c720-4206-b6ae-9c1973856016/1634-1
00:12:36.387 --> 00:12:38.943
ocean waves that are passing by
the cable.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1666-0
00:12:39.223 --> 00:12:43.130
This is nice long period signal
and we can see it as soon as it
e1a6d0f5-c720-4206-b6ae-9c1973856016/1666-1
00:12:43.130 --> 00:12:47.037
hits this dynamic range and then
upper limit it's kind of flips
e1a6d0f5-c720-4206-b6ae-9c1973856016/1666-2
00:12:47.037 --> 00:12:50.823
to the other side and continues
and then goes back and so on.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1668-0
00:12:50.823 --> 00:12:51.943
So this is the typical.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1681-0
00:12:53.843 --> 00:12:57.865
Type of saturation that we're
getting with with gas data on
e1a6d0f5-c720-4206-b6ae-9c1973856016/1681-1
00:12:57.865 --> 00:12:58.603
the bottom.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1724-0
00:12:58.603 --> 00:13:01.596
Here we have a vibrating
segment, so a segment of of
e1a6d0f5-c720-4206-b6ae-9c1973856016/1724-1
00:13:01.596 --> 00:13:05.154
cable that is hanging freely in
the water column and vibrates.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1724-2
00:13:05.154 --> 00:13:08.373
And these vibrations have
increasing amplitude and so as
e1a6d0f5-c720-4206-b6ae-9c1973856016/1724-3
00:13:08.373 --> 00:13:11.649
soon as these amplitudes hits
the dynamic range, we start
e1a6d0f5-c720-4206-b6ae-9c1973856016/1724-4
00:13:11.649 --> 00:13:13.683
getting very complicated
behaviour.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1739-0
00:13:16.473 --> 00:13:21.574
Now, what is this number of 40
microstrane per second really
e1a6d0f5-c720-4206-b6ae-9c1973856016/1739-1
00:13:21.574 --> 00:13:21.993
mean?
e1a6d0f5-c720-4206-b6ae-9c1973856016/1769-0
00:13:22.193 --> 00:13:26.164
And because usually work with
particle motions like P DRAM
e1a6d0f5-c720-4206-b6ae-9c1973856016/1769-1
00:13:26.164 --> 00:13:29.933
displacement or P ground
acceleration, so we can make a
e1a6d0f5-c720-4206-b6ae-9c1973856016/1769-2
00:13:29.933 --> 00:13:33.433
conversion using a simple
monochromatic oscillator.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1788-0
00:13:34.153 --> 00:13:39.608
So if we have sort of a cosine
like wave form with a frequency
e1a6d0f5-c720-4206-b6ae-9c1973856016/1788-1
00:13:39.608 --> 00:13:42.033
F and a propagation speed C.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1795-0
00:13:42.903 --> 00:13:45.863
And the maximum peak ground
displacement a.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1818-0
00:13:46.973 --> 00:13:51.593
Then if we differentiate this
expression once in time, once in
e1a6d0f5-c720-4206-b6ae-9c1973856016/1818-1
00:13:51.593 --> 00:13:55.919
space, then we getting the
strain rate that corresponds to
e1a6d0f5-c720-4206-b6ae-9c1973856016/1818-2
00:13:55.919 --> 00:13:57.093
that oscillator.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1826-0
00:13:57.853 --> 00:14:01.797
And so if we then plug this into
the criterion for the dynamic
e1a6d0f5-c720-4206-b6ae-9c1973856016/1826-1
00:14:01.797 --> 00:14:02.173
range.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1864-0
00:14:03.743 --> 00:14:07.513
Then we get an expression like
this and I'm just split it out
e1a6d0f5-c720-4206-b6ae-9c1973856016/1864-1
00:14:07.513 --> 00:14:11.283
into three components, one that
is related to the wave field,
e1a6d0f5-c720-4206-b6ae-9c1973856016/1864-2
00:14:11.283 --> 00:14:14.932
one that is intrinsic to the
fibre and one it is related to
e1a6d0f5-c720-4206-b6ae-9c1973856016/1864-3
00:14:14.932 --> 00:14:17.183
the acquisition or your
instruments.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1907-0
00:14:18.253 --> 00:14:22.871
And so if we again plug in some
realistic numbers for this, we
e1a6d0f5-c720-4206-b6ae-9c1973856016/1907-1
00:14:22.871 --> 00:14:26.317
get a maximum P prime
displacement of about 25
e1a6d0f5-c720-4206-b6ae-9c1973856016/1907-2
00:14:26.317 --> 00:14:30.862
micrometres, meaning that any P
gram displacement larger than
e1a6d0f5-c720-4206-b6ae-9c1973856016/1907-3
00:14:30.862 --> 00:14:34.821
that would saturate our
measurements. And so those of
e1a6d0f5-c720-4206-b6ae-9c1973856016/1907-4
00:14:34.821 --> 00:14:38.926
you working with earthquake
warning will recognize that
e1a6d0f5-c720-4206-b6ae-9c1973856016/1907-5
00:14:38.926 --> 00:14:39.293
this.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1920-0
00:14:39.293 --> 00:14:42.467
Is a very small number and this
would correspond with a very
e1a6d0f5-c720-4206-b6ae-9c1973856016/1920-1
00:14:42.467 --> 00:14:43.613
small magnitude event.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1922-0
00:14:44.543 --> 00:14:45.303
That is close by.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1934-0
00:14:48.593 --> 00:14:51.513
Now, earthquakes are of course
not monochromatic.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1941-0
00:14:51.513 --> 00:14:56.608
They are broadband and the
threshold for saturation depends
e1a6d0f5-c720-4206-b6ae-9c1973856016/1941-1
00:14:56.608 --> 00:14:57.713
on frequency.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1956-0
00:14:59.263 --> 00:15:02.100
Particularly because of this
conversion between the strain
e1a6d0f5-c720-4206-b6ae-9c1973856016/1956-1
00:15:02.100 --> 00:15:03.303
rates to particle motion.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1988-0
00:15:04.983 --> 00:15:08.282
So maybe you know this
relationship is not entirely
e1a6d0f5-c720-4206-b6ae-9c1973856016/1988-1
00:15:08.282 --> 00:15:12.279
accurate for earthquakes, and so
one of the objectives that we
e1a6d0f5-c720-4206-b6ae-9c1973856016/1988-2
00:15:12.279 --> 00:15:16.023
had was to come up with a
saturation threshold in terms of
e1a6d0f5-c720-4206-b6ae-9c1973856016/1988-3
00:15:16.023 --> 00:15:17.863
earthquake source parameters.
e1a6d0f5-c720-4206-b6ae-9c1973856016/1999-0
00:15:19.483 --> 00:15:22.523
And I will spare you the
details, but this is the result.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2009-0
00:15:23.083 --> 00:15:27.331
So this looks very long and
complicated, but I'll just break
e1a6d0f5-c720-4206-b6ae-9c1973856016/2009-1
00:15:27.331 --> 00:15:29.003
it down into small bits.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2029-0
00:15:31.143 --> 00:15:34.983
So on the left here we have the
magnitude of an earthquake that
e1a6d0f5-c720-4206-b6ae-9c1973856016/2029-1
00:15:34.983 --> 00:15:37.143
would cause saturation of our
data.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2042-0
00:15:38.693 --> 00:15:41.905
And the components that we have
here in this in this
e1a6d0f5-c720-4206-b6ae-9c1973856016/2042-1
00:15:41.905 --> 00:15:42.693
relationship.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2057-0
00:15:44.303 --> 00:15:46.943
The notes parameters relating to
the acquisition.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2076-0
00:15:47.063 --> 00:15:51.643
So the things like the time
something rate and the special
e1a6d0f5-c720-4206-b6ae-9c1973856016/2076-1
00:15:51.643 --> 00:15:56.223
sampling going here, seismic
source parameters go in here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2082-0
00:15:56.223 --> 00:15:58.623
So we have a stress drop and
radiation pattern.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2103-0
00:16:00.263 --> 00:16:03.995
We have some parameters related
to the propagation in the
e1a6d0f5-c720-4206-b6ae-9c1973856016/2103-1
00:16:03.995 --> 00:16:08.049
medium, so we have this quality
factor for attenuation and the
e1a6d0f5-c720-4206-b6ae-9c1973856016/2103-2
00:16:08.049 --> 00:16:09.143
shear wave speed.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2112-0
00:16:09.953 --> 00:16:12.818
And finally, we have here
component related to the Hyper
e1a6d0f5-c720-4206-b6ae-9c1973856016/2112-1
00:16:12.818 --> 00:16:13.673
central distance.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2159-0
00:16:15.223 --> 00:16:19.698
So in most cases all the 1st 3
components are simply fixed or
e1a6d0f5-c720-4206-b6ae-9c1973856016/2159-1
00:16:19.698 --> 00:16:23.524
well approximated by a
representative number, and so
e1a6d0f5-c720-4206-b6ae-9c1973856016/2159-2
00:16:23.524 --> 00:16:27.567
this this equation simply is a
relationship between the
e1a6d0f5-c720-4206-b6ae-9c1973856016/2159-3
00:16:27.567 --> 00:16:31.826
magnitude that would cause
saturation in our dash data and
e1a6d0f5-c720-4206-b6ae-9c1973856016/2159-4
00:16:31.826 --> 00:16:33.703
the hypercentral distance.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2167-0
00:16:35.383 --> 00:16:37.943
And this relationship I plotted
over here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2216-0
00:16:38.743 --> 00:16:43.337
So in this very busy figure we
have on the horizontal axis the
e1a6d0f5-c720-4206-b6ae-9c1973856016/2216-1
00:16:43.337 --> 00:16:47.421
hypercentral distance in
kilometers and on the vertical
e1a6d0f5-c720-4206-b6ae-9c1973856016/2216-2
00:16:47.421 --> 00:16:51.579
axis the magnitudes of the
events and this long equation
e1a6d0f5-c720-4206-b6ae-9c1973856016/2216-3
00:16:51.579 --> 00:16:56.173
that I had on a previous slide
is given by this solid or this.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2216-4
00:16:56.173 --> 00:16:58.143
This dashed line over here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2226-0
00:16:59.103 --> 00:17:03.543
So any earthquake, it has a
magnitude that falls above.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2240-0
00:17:04.343 --> 00:17:08.268
This this line would call
saturation and any earthquake
e1a6d0f5-c720-4206-b6ae-9c1973856016/2240-1
00:17:08.268 --> 00:17:11.143
this either far away or has a
magnitude.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2251-0
00:17:12.303 --> 00:17:16.648
Plots within this this space
below the Black line would not
e1a6d0f5-c720-4206-b6ae-9c1973856016/2251-1
00:17:16.648 --> 00:17:17.663
saturate data.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2279-0
00:17:19.223 --> 00:17:22.504
Then the colours that you see
here are actual measurements,
e1a6d0f5-c720-4206-b6ae-9c1973856016/2279-1
00:17:22.504 --> 00:17:25.513
because we have lots of
earthquakes that were recorded
e1a6d0f5-c720-4206-b6ae-9c1973856016/2279-2
00:17:25.513 --> 00:17:28.303
at various hyper central
distances and magnitudes.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2311-0
00:17:28.503 --> 00:17:33.161
So for each of these events, I
took the catalogue magnitude and
e1a6d0f5-c720-4206-b6ae-9c1973856016/2311-1
00:17:33.161 --> 00:17:37.965
and location and then determined
whether a given task measurement
e1a6d0f5-c720-4206-b6ae-9c1973856016/2311-2
00:17:37.965 --> 00:17:41.023
was saturated or not for this
earthquake.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2317-0
00:17:41.863 --> 00:17:42.703
Was not saturated.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2327-0
00:17:42.703 --> 00:17:47.172
I plotted it in green if it was
saturated, I plotted it in
e1a6d0f5-c720-4206-b6ae-9c1973856016/2327-1
00:17:47.172 --> 00:17:47.703
orange.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2353-0
00:17:49.263 --> 00:17:53.177
And so you can see that this
criterion that was on the
e1a6d0f5-c720-4206-b6ae-9c1973856016/2353-1
00:17:53.177 --> 00:17:57.377
previous slide more or less
device the data into saturated
e1a6d0f5-c720-4206-b6ae-9c1973856016/2353-2
00:17:57.377 --> 00:17:58.943
and and non saturated.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2382-0
00:18:00.783 --> 00:18:04.553
Recordings and this is perhaps a
bit better to see if we just
e1a6d0f5-c720-4206-b6ae-9c1973856016/2382-1
00:18:04.553 --> 00:18:08.263
rescale the horizontal axis or
transform it to a logarithmic
e1a6d0f5-c720-4206-b6ae-9c1973856016/2382-2
00:18:08.263 --> 00:18:11.912
scaling, and then we can see
nicely that both are large and
e1a6d0f5-c720-4206-b6ae-9c1973856016/2382-3
00:18:11.912 --> 00:18:12.703
small events.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2389-0
00:18:14.193 --> 00:18:16.513
All the events that plot above
these lines.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2402-0
00:18:18.063 --> 00:18:20.894
They are saturated and below the
lines they're mostly not
e1a6d0f5-c720-4206-b6ae-9c1973856016/2402-1
00:18:20.894 --> 00:18:21.383
saturated.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2443-0
00:18:23.143 --> 00:18:26.852
And now if you look a bit more
closely at the range of
e1a6d0f5-c720-4206-b6ae-9c1973856016/2443-1
00:18:26.852 --> 00:18:31.101
distances that are relevant for
earthquake related warning. So
e1a6d0f5-c720-4206-b6ae-9c1973856016/2443-2
00:18:31.101 --> 00:18:35.215
let's say that we take a high
percentile distance of, say 50
e1a6d0f5-c720-4206-b6ae-9c1973856016/2443-3
00:18:35.215 --> 00:18:39.464
kilometers, then you will see
that saturation is predicted and
e1a6d0f5-c720-4206-b6ae-9c1973856016/2443-4
00:18:39.464 --> 00:18:41.623
also observed to occur for magn.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2445-0
00:18:41.623 --> 00:18:42.743
As small as three.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2484-0
00:18:44.623 --> 00:18:49.096
And so, of course it is really
bad news that even for very
e1a6d0f5-c720-4206-b6ae-9c1973856016/2484-1
00:18:49.096 --> 00:18:53.872
small magnitude earthquakes, we
already have saturation of our
e1a6d0f5-c720-4206-b6ae-9c1973856016/2484-2
00:18:53.872 --> 00:18:58.800
DAS data and what we would like
to do is to record correctly the
e1a6d0f5-c720-4206-b6ae-9c1973856016/2484-3
00:18:58.800 --> 00:19:03.576
wave forms of earthquakes up to
magnitude 6 or even larger. So
e1a6d0f5-c720-4206-b6ae-9c1973856016/2484-4
00:19:03.576 --> 00:19:04.183
we have.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2499-0
00:19:04.183 --> 00:19:07.816
This gap of orders of magnitude
in the the dynamic range that we
e1a6d0f5-c720-4206-b6ae-9c1973856016/2499-1
00:19:07.816 --> 00:19:08.823
are still missing.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2507-0
00:19:11.693 --> 00:19:15.093
O could we potentially fix this
in a way?
e1a6d0f5-c720-4206-b6ae-9c1973856016/2527-0
00:19:16.663 --> 00:19:20.212
Well, first of all, you have to
realise that when saturation
e1a6d0f5-c720-4206-b6ae-9c1973856016/2527-1
00:19:20.212 --> 00:19:23.703
starts, most of the original
information is still retained.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2570-0
00:19:24.463 --> 00:19:28.779
So here again we have the
example of the the swell, even
e1a6d0f5-c720-4206-b6ae-9c1973856016/2570-1
00:19:28.779 --> 00:19:33.474
though it starts to saturate the
recordings, we can recognise
e1a6d0f5-c720-4206-b6ae-9c1973856016/2570-2
00:19:33.474 --> 00:19:37.866
most of the swell in in in the
recordings here and if you
e1a6d0f5-c720-4206-b6ae-9c1973856016/2570-3
00:19:37.866 --> 00:19:42.183
calculate the spectrum you will
more or less obtain the.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2575-0
00:19:42.863 --> 00:19:44.903
Spectrum for this type of
signal.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2595-0
00:19:46.873 --> 00:19:51.102
And so, in a way, we could maybe
try some spectral analysis and
e1a6d0f5-c720-4206-b6ae-9c1973856016/2595-1
00:19:51.102 --> 00:19:55.067
see if we can still extract
useful information relevant for
e1a6d0f5-c720-4206-b6ae-9c1973856016/2595-2
00:19:55.067 --> 00:19:55.993
early warning.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2605-0
00:19:58.413 --> 00:20:01.373
So here is a synthetic example
of that.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2629-0
00:20:01.573 --> 00:20:05.363
So this is a simple spectrum on
the horizontal axis I have a
e1a6d0f5-c720-4206-b6ae-9c1973856016/2629-1
00:20:05.363 --> 00:20:07.973
frequency on the vertical axis I
have oh.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2656-0
00:20:08.063 --> 00:20:12.264
This is not spectral density,
but the spectral amplitude, and
e1a6d0f5-c720-4206-b6ae-9c1973856016/2656-1
00:20:12.264 --> 00:20:16.602
this is for. So what I do here
is I take a a waveform generated
e1a6d0f5-c720-4206-b6ae-9c1973856016/2656-2
00:20:16.602 --> 00:20:18.703
from a standard prune spectrum.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2703-0
00:20:18.703 --> 00:20:23.342
So the spectrum is given in
black in the background and then
e1a6d0f5-c720-4206-b6ae-9c1973856016/2703-1
00:20:23.342 --> 00:20:28.058
I scale up the amplitude beyond
the dynamic range and sort of
e1a6d0f5-c720-4206-b6ae-9c1973856016/2703-2
00:20:28.058 --> 00:20:33.078
rescale or wrap the signal as if
we are recording it with DAS and
e1a6d0f5-c720-4206-b6ae-9c1973856016/2703-3
00:20:33.078 --> 00:20:37.642
so the spectrum resulting from
that is the orange line over
e1a6d0f5-c720-4206-b6ae-9c1973856016/2703-4
00:20:37.642 --> 00:20:38.023
here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2705-0
00:20:38.303 --> 00:20:38.463
4.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2745-0
00:20:39.263 --> 00:20:43.773
And so you can see that while
most of the original spectrum is
e1a6d0f5-c720-4206-b6ae-9c1973856016/2745-1
00:20:43.773 --> 00:20:47.998
is is retained, there are some
sidelobes that are that are
e1a6d0f5-c720-4206-b6ae-9c1973856016/2745-2
00:20:47.998 --> 00:20:52.366
forming and the lower and the
higher frequencies. But if you
e1a6d0f5-c720-4206-b6ae-9c1973856016/2745-3
00:20:52.366 --> 00:20:56.948
were to record a spectrum like
this, you would still be able to
e1a6d0f5-c720-4206-b6ae-9c1973856016/2745-4
00:20:56.948 --> 00:20:58.023
recover things.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2754-0
00:20:58.023 --> 00:20:59.903
Like the corner frequency for
instance.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2770-0
00:21:01.573 --> 00:21:05.609
And if we then gradually
increase this amplitude and then
e1a6d0f5-c720-4206-b6ae-9c1973856016/2770-1
00:21:05.609 --> 00:21:08.533
do the exercise again, you will
see that.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2787-0
00:21:09.063 --> 00:21:13.403
Actually, more of this energy
around the peak starts to leak
e1a6d0f5-c720-4206-b6ae-9c1973856016/2787-1
00:21:13.403 --> 00:21:15.183
away into the side lobes.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2799-0
00:21:15.183 --> 00:21:18.118
So the side lobes become more
prominent and the peak, the peak
e1a6d0f5-c720-4206-b6ae-9c1973856016/2799-1
00:21:18.118 --> 00:21:19.143
becomes a bit smaller.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2845-0
00:21:20.693 --> 00:21:24.864
And so keep doing this for
higher and higher amplitudes and
e1a6d0f5-c720-4206-b6ae-9c1973856016/2845-1
00:21:24.864 --> 00:21:28.688
then you will see that
eventually the spectrum that we
e1a6d0f5-c720-4206-b6ae-9c1973856016/2845-2
00:21:28.688 --> 00:21:33.138
record becomes pretty much flat,
which would be indicative of a
e1a6d0f5-c720-4206-b6ae-9c1973856016/2845-3
00:21:33.138 --> 00:21:37.449
uniform distribution. And so if
you were to record a spectrum
e1a6d0f5-c720-4206-b6ae-9c1973856016/2845-4
00:21:37.449 --> 00:21:39.813
like this, you would not be
able.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2848-0
00:21:39.813 --> 00:21:40.853
To recover.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2853-0
00:21:42.123 --> 00:21:43.443
Things like the corner
frequency.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2869-0
00:21:46.373 --> 00:21:50.643
Another way to look at this is
to look at how close our data
e1a6d0f5-c720-4206-b6ae-9c1973856016/2869-1
00:21:50.643 --> 00:21:53.093
represents a uniform
distribution.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2889-0
00:21:54.053 --> 00:21:58.135
So if you just focus on the
bottom left panel over here,
e1a6d0f5-c720-4206-b6ae-9c1973856016/2889-1
00:21:58.135 --> 00:22:01.573
here are plotted a cumulative
density function.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2896-0
00:22:01.613 --> 00:22:04.173
So essentially sort of the
integral of a histogram.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2908-0
00:22:05.733 --> 00:22:09.493
Of the the data skills between
this case minus and plus one.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2917-0
00:22:11.173 --> 00:22:14.369
In this representation, a
uniform distribution would
e1a6d0f5-c720-4206-b6ae-9c1973856016/2917-1
00:22:14.369 --> 00:22:14.973
simply be.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2926-0
00:22:15.553 --> 00:22:20.113
A straight line, so it is dotted
line over here would be what?
e1a6d0f5-c720-4206-b6ae-9c1973856016/2947-0
00:22:20.113 --> 00:22:24.957
The uniform distribution would
give you and initially our data
e1a6d0f5-c720-4206-b6ae-9c1973856016/2947-1
00:22:24.957 --> 00:22:29.033
is more or less sort of Gaussian
in in distribution.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2974-0
00:22:29.033 --> 00:22:33.754
So it's kind of gives you this
nice *** shape over here, but as
e1a6d0f5-c720-4206-b6ae-9c1973856016/2974-1
00:22:33.754 --> 00:22:38.180
the amplitude increases, we
gradually get closer and closer
e1a6d0f5-c720-4206-b6ae-9c1973856016/2974-2
00:22:38.180 --> 00:22:40.393
to this to this diagonal line.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2985-0
00:22:41.173 --> 00:22:45.239
Indicating that our data become
more and more close to a uniform
e1a6d0f5-c720-4206-b6ae-9c1973856016/2985-1
00:22:45.239 --> 00:22:46.053
distribution.
e1a6d0f5-c720-4206-b6ae-9c1973856016/2991-0
00:22:46.943 --> 00:22:49.023
Losing all useful information.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3005-0
00:22:51.633 --> 00:22:55.299
We can actually measure the
distance between our current
e1a6d0f5-c720-4206-b6ae-9c1973856016/3005-1
00:22:55.299 --> 00:22:57.873
data distribution and that of an
ideal.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3009-0
00:22:59.413 --> 00:23:00.533
Uniform distribution.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3019-0
00:23:02.213 --> 00:23:04.533
The metric for this is given
over here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3032-0
00:23:05.093 --> 00:23:08.434
I guess it will not make much
sense to you right now, but I
e1a6d0f5-c720-4206-b6ae-9c1973856016/3032-1
00:23:08.434 --> 00:23:10.773
can assure you that it makes
sense to me.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3046-0
00:23:12.693 --> 00:23:17.318
And so when we have wave forms
with different degrees of
e1a6d0f5-c720-4206-b6ae-9c1973856016/3046-1
00:23:17.318 --> 00:23:21.133
saturation, we can use this
metric to measure.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3056-0
00:23:21.713 --> 00:23:26.153
How saturated it is O if the
data are retty.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3059-0
00:23:26.153 --> 00:23:27.393
Much not saturated.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3083-0
00:23:27.673 --> 00:23:32.458
We have a relatively low metric
of value of the metric and as
e1a6d0f5-c720-4206-b6ae-9c1973856016/3083-1
00:23:32.458 --> 00:23:36.549
the data become more and more
saturated, this metric
e1a6d0f5-c720-4206-b6ae-9c1973856016/3083-2
00:23:36.549 --> 00:23:37.553
approaches 1.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3109-0
00:23:39.093 --> 00:23:43.650
And so basically what I just
said is also depicted here is
e1a6d0f5-c720-4206-b6ae-9c1973856016/3109-1
00:23:43.650 --> 00:23:48.053
figure where we have the
amplitude by which the waveform
e1a6d0f5-c720-4206-b6ae-9c1973856016/3109-2
00:23:48.053 --> 00:23:50.293
exceeds the dynamic range so.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3133-0
00:23:51.543 --> 00:23:55.694
One here indicates dynamic range
and then we get here a factor of
e1a6d0f5-c720-4206-b6ae-9c1973856016/3133-1
00:23:55.694 --> 00:23:59.405
10 a factor hundred a factor of
1000 exceeding the dynamic
e1a6d0f5-c720-4206-b6ae-9c1973856016/3133-2
00:23:59.405 --> 00:23:59.783
range.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3165-0
00:24:00.463 --> 00:24:04.781
And so if we do that, we can
measure how the saturation
e1a6d0f5-c720-4206-b6ae-9c1973856016/3165-1
00:24:04.781 --> 00:24:09.562
metric changes with increasing
amplitude, and we can see that
e1a6d0f5-c720-4206-b6ae-9c1973856016/3165-2
00:24:09.562 --> 00:24:14.497
up to about a factor 10 or maybe
a factor of 20. We could still
e1a6d0f5-c720-4206-b6ae-9c1973856016/3165-3
00:24:14.497 --> 00:24:15.423
distinguish.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3177-0
00:24:16.573 --> 00:24:20.802
Based on the saturation metric,
what the original amplitude has
e1a6d0f5-c720-4206-b6ae-9c1973856016/3177-1
00:24:20.802 --> 00:24:21.133
been.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3188-0
00:24:22.233 --> 00:24:25.181
So what we do is we just take a
particular waveform that is
e1a6d0f5-c720-4206-b6ae-9c1973856016/3188-1
00:24:25.181 --> 00:24:25.673
saturated.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3216-0
00:24:25.913 --> 00:24:29.465
We compute the saturation
metric, which could fall
e1a6d0f5-c720-4206-b6ae-9c1973856016/3216-1
00:24:29.465 --> 00:24:33.854
somewhere over here, and then
the corresponding amplitude that
e1a6d0f5-c720-4206-b6ae-9c1973856016/3216-2
00:24:33.854 --> 00:24:38.313
causes this kind of saturation
would here be, say, a factor 15.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3233-0
00:24:39.853 --> 00:24:44.312
So even though the amplitudes
are saturating, they cannot
e1a6d0f5-c720-4206-b6ae-9c1973856016/3233-1
00:24:44.312 --> 00:24:46.773
increase beyond a certain value.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3250-0
00:24:47.133 --> 00:24:51.125
We could still estimate the
original signal amplitudes that
e1a6d0f5-c720-4206-b6ae-9c1973856016/3250-1
00:24:51.125 --> 00:24:54.053
have caused a certain degree of
saturation.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3269-0
00:24:54.973 --> 00:25:00.096
Up to a factor 20 or so, after
which this metric itself
e1a6d0f5-c720-4206-b6ae-9c1973856016/3269-1
00:25:00.096 --> 00:25:03.573
saturates ironically and and
plateau.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3287-0
00:25:03.573 --> 00:25:08.823
So we cannot distinguish whether
the signal is 20 or 100 or 1000
e1a6d0f5-c720-4206-b6ae-9c1973856016/3287-1
00:25:08.823 --> 00:25:11.813
times higher than the dynamic
range.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3312-0
00:25:14.973 --> 00:25:19.109
So I kind of want to stop here
talking about the dynamic range
e1a6d0f5-c720-4206-b6ae-9c1973856016/3312-1
00:25:19.109 --> 00:25:23.377
because there is more and let me
just check how much time I have
e1a6d0f5-c720-4206-b6ae-9c1973856016/3312-2
00:25:23.377 --> 00:25:25.413
left. OK. So I still have time.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3341-0
00:25:26.973 --> 00:25:30.920
So as an intermediate
conclusion, I just want to know
e1a6d0f5-c720-4206-b6ae-9c1973856016/3341-1
00:25:30.920 --> 00:25:35.672
give you as a take home message
that currently the dynamic range
e1a6d0f5-c720-4206-b6ae-9c1973856016/3341-2
00:25:35.672 --> 00:25:39.693
of DAS is not sufficient for
earthquake early warning.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3353-0
00:25:41.333 --> 00:25:45.344
And possibly we can extend this
dynamic range by a factor 10 or
e1a6d0f5-c720-4206-b6ae-9c1973856016/3353-1
00:25:45.344 --> 00:25:45.533
20.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3382-0
00:25:46.673 --> 00:25:51.441
By analyzing the data in a
different way, but it will not
e1a6d0f5-c720-4206-b6ae-9c1973856016/3382-1
00:25:51.441 --> 00:25:56.046
get us up to the level of
recording a magnitude 6 event
e1a6d0f5-c720-4206-b6ae-9c1973856016/3382-2
00:25:56.046 --> 00:25:59.993
faithfully with typical
acquisition parameters.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3436-0
00:26:01.373 --> 00:26:05.984
But we could use DAS together
with the online strong motion
e1a6d0f5-c720-4206-b6ae-9c1973856016/3436-1
00:26:05.984 --> 00:26:10.826
sensors to at least expedite a
warning. For instance, we could
e1a6d0f5-c720-4206-b6ae-9c1973856016/3436-2
00:26:10.826 --> 00:26:15.361
consider locating the seismic
event with DAS, which is not
e1a6d0f5-c720-4206-b6ae-9c1973856016/3436-3
00:26:15.361 --> 00:26:19.819
affected by by saturation
because the first arrival is is
e1a6d0f5-c720-4206-b6ae-9c1973856016/3436-4
00:26:19.819 --> 00:26:22.433
week, and then as soon as the
SE.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3447-0
00:26:22.533 --> 00:26:26.018
Waves hits the first strong
motion sensor. We can estimate
e1a6d0f5-c720-4206-b6ae-9c1973856016/3447-1
00:26:26.018 --> 00:26:27.613
the magnitude of the event.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3455-0
00:26:28.393 --> 00:26:31.433
With the single sensor from
based on the spectrum.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3470-0
00:26:32.343 --> 00:26:36.755
And then we can already send out
an alert, even though only the
e1a6d0f5-c720-4206-b6ae-9c1973856016/3470-1
00:26:36.755 --> 00:26:39.583
first online station has been
triggered.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3495-0
00:26:41.083 --> 00:26:44.633
And clearly there is a need for
more technological advances,
e1a6d0f5-c720-4206-b6ae-9c1973856016/3495-1
00:26:44.633 --> 00:26:48.009
particularly in photonics, to
see if we can increase this
e1a6d0f5-c720-4206-b6ae-9c1973856016/3495-2
00:26:48.009 --> 00:26:50.163
dynamic range in one way or
another.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3505-0
00:26:51.993 --> 00:26:54.153
All right, now the second thing
I want to talk about.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3538-0
00:26:55.873 --> 00:27:00.045
Is local back projection, so for
not necessarily earthquake
e1a6d0f5-c720-4206-b6ae-9c1973856016/3538-1
00:27:00.045 --> 00:27:03.662
related warning, but
particularly for tsunami early
e1a6d0f5-c720-4206-b6ae-9c1973856016/3538-2
00:27:03.662 --> 00:27:07.626
warning, we need to characterize
the rupture in terms of
e1a6d0f5-c720-4206-b6ae-9c1973856016/3538-3
00:27:07.626 --> 00:27:11.313
magnitude and whether it has a
surface break or not.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3544-0
00:27:11.853 --> 00:27:13.413
And the rupture area and things
like that.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3562-0
00:27:14.913 --> 00:27:19.023
And for these kind of things, we
don't want to wait for Taylor
e1a6d0f5-c720-4206-b6ae-9c1973856016/3562-1
00:27:19.023 --> 00:27:21.633
seismic W phases to estimate
magnitude.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3586-0
00:27:23.473 --> 00:27:28.324
So instead things we can do is
do for instance a rapid finite
e1a6d0f5-c720-4206-b6ae-9c1973856016/3586-1
00:27:28.324 --> 00:27:33.097
fault inversion using the local
xorometer network to get the
e1a6d0f5-c720-4206-b6ae-9c1973856016/3586-2
00:27:33.097 --> 00:27:34.193
finer details.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3597-0
00:27:36.073 --> 00:27:41.129
Or as fine as possible of the
rupture. But a second solution
e1a6d0f5-c720-4206-b6ae-9c1973856016/3597-1
00:27:41.129 --> 00:27:41.793
to this.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3607-0
00:27:42.383 --> 00:27:46.303
To this challenge is using local
arrays to do back projection.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3640-0
00:27:47.343 --> 00:27:51.338
So here it is nicely sort of
drawn schematically where we
e1a6d0f5-c720-4206-b6ae-9c1973856016/3640-1
00:27:51.338 --> 00:27:55.196
have an earthquake that is
recorded by multiple seismic
e1a6d0f5-c720-4206-b6ae-9c1973856016/3640-2
00:27:55.196 --> 00:27:59.123
arrays that are then used to
back project the signal and
e1a6d0f5-c720-4206-b6ae-9c1973856016/3640-3
00:27:59.123 --> 00:28:02.223
essentially track the rupture as
it evolves.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3673-0
00:28:04.743 --> 00:28:08.931
And I guess that's that's many
of you are familiar with data
e1a6d0f5-c720-4206-b6ae-9c1973856016/3673-1
00:28:08.931 --> 00:28:12.845
seismic back projection where
you take Continental scale
e1a6d0f5-c720-4206-b6ae-9c1973856016/3673-2
00:28:12.845 --> 00:28:16.759
arrays to zoom in and look at
relatively large magnitude
e1a6d0f5-c720-4206-b6ae-9c1973856016/3673-3
00:28:16.759 --> 00:28:17.583
earthquakes.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3687-0
00:28:18.143 --> 00:28:22.244
And this has been very
successful in in characterising
e1a6d0f5-c720-4206-b6ae-9c1973856016/3687-1
00:28:22.244 --> 00:28:24.183
these very large ruptures.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3696-0
00:28:24.503 --> 00:28:28.525
So here's an example from Peru
where we could very nicely track
e1a6d0f5-c720-4206-b6ae-9c1973856016/3696-1
00:28:28.525 --> 00:28:29.343
this rupture.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3711-0
00:28:30.153 --> 00:28:33.851
Propagating in a particular
direction, then also identify a
e1a6d0f5-c720-4206-b6ae-9c1973856016/3711-1
00:28:33.851 --> 00:28:35.393
back propagating rupture.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3714-0
00:28:35.903 --> 00:28:36.703
At the same time.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3756-0
00:28:39.473 --> 00:28:43.704
We can also do this at the local
scale. What's very nice about
e1a6d0f5-c720-4206-b6ae-9c1973856016/3756-1
00:28:43.704 --> 00:28:47.332
that is that local back
projection should have a much
e1a6d0f5-c720-4206-b6ae-9c1973856016/3756-2
00:28:47.332 --> 00:28:51.362
higher resolution because you're
much closer to the seasick
e1a6d0f5-c720-4206-b6ae-9c1973856016/3756-3
00:28:51.362 --> 00:28:54.855
source. But these local
waveforms tend to be rather
e1a6d0f5-c720-4206-b6ae-9c1973856016/3756-4
00:28:54.855 --> 00:28:58.617
messy. Having lots of local
scattering and simultaneous
e1a6d0f5-c720-4206-b6ae-9c1973856016/3756-5
00:28:58.617 --> 00:28:58.953
Arri.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3761-0
00:28:59.153 --> 00:28:59.993
Or phases.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3773-0
00:29:00.633 --> 00:29:03.967
And so it is not very likely
that waveform coherence that we
e1a6d0f5-c720-4206-b6ae-9c1973856016/3773-1
00:29:03.967 --> 00:29:05.553
need for the back projection.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3780-0
00:29:06.353 --> 00:29:08.793
Persists across the scale of an
entire array.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3806-0
00:29:09.923 --> 00:29:14.009
So instead we would have to
break up the array into locally
e1a6d0f5-c720-4206-b6ae-9c1973856016/3806-1
00:29:14.009 --> 00:29:17.960
coherent sub arrays and then
combine the results of these
e1a6d0f5-c720-4206-b6ae-9c1973856016/3806-2
00:29:17.960 --> 00:29:21.843
smaller arrays to really focus
on the earthquake source.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3819-0
00:29:23.393 --> 00:29:26.313
And this has been the the PhD
work of Iiqing.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3831-0
00:29:26.713 --> 00:29:31.593
Who is now a applying these kind
of methods on on DAS data?
e1a6d0f5-c720-4206-b6ae-9c1973856016/3875-0
00:29:34.193 --> 00:29:38.545
And so one of the things that
she looked at was, well, how
e1a6d0f5-c720-4206-b6ae-9c1973856016/3875-1
00:29:38.545 --> 00:29:43.045
feasible is it to actually use
an offshore gas cable that is
e1a6d0f5-c720-4206-b6ae-9c1973856016/3875-2
00:29:43.045 --> 00:29:47.841
not deployed for the purpose of
back projection and how how much
e1a6d0f5-c720-4206-b6ae-9c1973856016/3875-3
00:29:47.841 --> 00:29:52.193
of A details can we extract from
the back, back projection
e1a6d0f5-c720-4206-b6ae-9c1973856016/3875-4
00:29:52.193 --> 00:29:53.153
procedure so.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3902-0
00:29:53.153 --> 00:29:57.191
For this you took one of the the
cables that we have in the in
e1a6d0f5-c720-4206-b6ae-9c1973856016/3902-1
00:29:57.191 --> 00:30:00.909
the region and here is an
example for one earthquake here
e1a6d0f5-c720-4206-b6ae-9c1973856016/3902-2
00:30:00.909 --> 00:30:03.153
to the West of this of this
cable.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3916-0
00:30:03.903 --> 00:30:07.094
So you can see this this
beautiful move out of this.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3916-1
00:30:07.094 --> 00:30:09.623
This, I think it was a magnitude
4 event.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3923-0
00:30:11.473 --> 00:30:13.993
So the data were not not
saturated.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3966-0
00:30:15.793 --> 00:30:20.542
And in order to make this back
projection work, she had to do a
e1a6d0f5-c720-4206-b6ae-9c1973856016/3966-1
00:30:20.542 --> 00:30:24.847
lot of different kinds of
processing. And yeah, basically
e1a6d0f5-c720-4206-b6ae-9c1973856016/3966-2
00:30:24.847 --> 00:30:29.225
apply particular procedure to
convert the raw data that we
e1a6d0f5-c720-4206-b6ae-9c1973856016/3966-3
00:30:29.225 --> 00:30:33.233
record to something that is
sufficiently coherent and
e1a6d0f5-c720-4206-b6ae-9c1973856016/3966-4
00:30:33.233 --> 00:30:33.753
useful.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3969-0
00:30:35.213 --> 00:30:36.413
So some of the steps including.
e1a6d0f5-c720-4206-b6ae-9c1973856016/3996-0
00:30:37.953 --> 00:30:42.170
Converting the strain rates to
particle velocity and then
e1a6d0f5-c720-4206-b6ae-9c1973856016/3996-1
00:30:42.170 --> 00:30:46.750
making corrections for the local
settlement layer to make sure
e1a6d0f5-c720-4206-b6ae-9c1973856016/3996-2
00:30:46.750 --> 00:30:50.895
that any uncertainties in the
velocity model are kind of
e1a6d0f5-c720-4206-b6ae-9c1973856016/3996-3
00:30:50.895 --> 00:30:51.913
cancelled out.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4033-0
00:30:54.203 --> 00:30:58.863
OK. And so by dividing the
entire cable into these local
e1a6d0f5-c720-4206-b6ae-9c1973856016/4033-1
00:30:58.863 --> 00:31:03.688
sub arrays and then focusing
each of these sub arrays onto
e1a6d0f5-c720-4206-b6ae-9c1973856016/4033-2
00:31:03.688 --> 00:31:09.085
the seismic source, she was able
to very nicely focus or identify
e1a6d0f5-c720-4206-b6ae-9c1973856016/4033-3
00:31:09.085 --> 00:31:12.683
the the origin location of this
earthquake.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4046-0
00:31:13.203 --> 00:31:16.724
So here again we have the cable.
Each of these triangles
e1a6d0f5-c720-4206-b6ae-9c1973856016/4046-1
00:31:16.724 --> 00:31:18.083
indicates 1 sub array.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4064-0
00:31:19.233 --> 00:31:22.721
And by by focusing each of them
in the right direction, they
e1a6d0f5-c720-4206-b6ae-9c1973856016/4064-1
00:31:22.721 --> 00:31:25.353
kind of intersect here in the
middle, so the.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4073-0
00:31:25.943 --> 00:31:29.470
Brighter colors indicate the
strength of the intersection, if
e1a6d0f5-c720-4206-b6ae-9c1973856016/4073-1
00:31:29.470 --> 00:31:29.983
you will.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4095-0
00:31:31.553 --> 00:31:36.242
And given that this is just a
small local earthquake, there is
e1a6d0f5-c720-4206-b6ae-9c1973856016/4095-1
00:31:36.242 --> 00:31:40.113
no propagation effect that are
to be recorded here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4128-0
00:31:41.833 --> 00:31:45.957
But now what we can do is we can
take a whole bunch of these
e1a6d0f5-c720-4206-b6ae-9c1973856016/4128-1
00:31:45.957 --> 00:31:50.284
small earthquakes and treat them
as empirical Green's functions
e1a6d0f5-c720-4206-b6ae-9c1973856016/4128-2
00:31:50.284 --> 00:31:54.747
to construct a much larger or to
simulate a much larger magnitude
e1a6d0f5-c720-4206-b6ae-9c1973856016/4128-3
00:31:54.747 --> 00:31:55.153
event.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4153-0
00:31:56.243 --> 00:32:00.713
So focusing here on this, this
top panel here on the right, our
e1a6d0f5-c720-4206-b6ae-9c1973856016/4153-1
00:32:00.713 --> 00:32:04.973
cable is now over here where we
have these triangles. And So
e1a6d0f5-c720-4206-b6ae-9c1973856016/4153-2
00:32:04.973 --> 00:32:05.323
what?
e1a6d0f5-c720-4206-b6ae-9c1973856016/4169-0
00:32:05.523 --> 00:32:10.046
I chain did was taking small
earthquakes that are occurring
e1a6d0f5-c720-4206-b6ae-9c1973856016/4169-1
00:32:10.046 --> 00:32:13.363
in this region and then
basically creating.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4195-0
00:32:15.153 --> 00:32:19.388
A line of these, this green
function and sort of stacking
e1a6d0f5-c720-4206-b6ae-9c1973856016/4195-1
00:32:19.388 --> 00:32:23.988
them into a wave form that is
recorded by the by the cable and
e1a6d0f5-c720-4206-b6ae-9c1973856016/4195-2
00:32:23.988 --> 00:32:27.713
then by back projecting those
synthetic waveforms.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4215-0
00:32:28.353 --> 00:32:32.690
We were able to very accurately
locate the the position and
e1a6d0f5-c720-4206-b6ae-9c1973856016/4215-1
00:32:32.690 --> 00:32:36.233
timing at which each of these
sources is active.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4245-0
00:32:36.833 --> 00:32:40.918
So the stars here indicate the
progression of the simulated
e1a6d0f5-c720-4206-b6ae-9c1973856016/4245-1
00:32:40.918 --> 00:32:45.139
magnitude 7 earthquake and the
circles here indicate what you
e1a6d0f5-c720-4206-b6ae-9c1973856016/4245-2
00:32:45.139 --> 00:32:48.884
would get from back, projecting
the wave forms of this
e1a6d0f5-c720-4206-b6ae-9c1973856016/4245-3
00:32:48.884 --> 00:32:49.633
earthquake.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4266-0
00:32:51.193 --> 00:32:55.289
And what is very nice about this
procedure is that a lot of the
e1a6d0f5-c720-4206-b6ae-9c1973856016/4266-1
00:32:55.289 --> 00:32:59.129
work needs to be done can be
done in advance. And so once a
e1a6d0f5-c720-4206-b6ae-9c1973856016/4266-2
00:32:59.129 --> 00:33:01.433
proper pipeline is set up, you
can.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4273-0
00:33:02.273 --> 00:33:05.033
Operate this pipeline in almost
in real time.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4312-0
00:33:06.673 --> 00:33:11.585
So with the DAS data coming in
and with selective windowing
e1a6d0f5-c720-4206-b6ae-9c1973856016/4312-1
00:33:11.585 --> 00:33:16.334
would be able to track the
rupture almost in in real time
e1a6d0f5-c720-4206-b6ae-9c1973856016/4312-2
00:33:16.334 --> 00:33:21.492
and especially for tsunami early
warning, this would be a very
e1a6d0f5-c720-4206-b6ae-9c1973856016/4312-3
00:33:21.492 --> 00:33:24.113
useful and valuable tool to use.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4332-0
00:33:27.983 --> 00:33:32.808
And so with that, I just want to
give you a little outlook on
e1a6d0f5-c720-4206-b6ae-9c1973856016/4332-1
00:33:32.808 --> 00:33:35.143
where we want to go from here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4353-0
00:33:35.903 --> 00:33:40.499
So clearly there is a need for a
larger range in order to do
e1a6d0f5-c720-4206-b6ae-9c1973856016/4353-1
00:33:40.499 --> 00:33:44.343
conventional earthquake related
warning with this.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4365-0
00:33:45.063 --> 00:33:49.069
Either that or we need other
clever methods to work around
e1a6d0f5-c720-4206-b6ae-9c1973856016/4365-1
00:33:49.069 --> 00:33:50.903
this limited dynamic range.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4369-0
00:33:51.543 --> 00:33:53.943
For instance, we could think of
ways to.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4376-0
00:33:54.713 --> 00:33:56.313
Unwrap the data and try to
reconstruct.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4394-0
00:33:57.453 --> 00:34:02.089
The original waveform that's
that's turned into a more
e1a6d0f5-c720-4206-b6ae-9c1973856016/4394-1
00:34:02.089 --> 00:34:05.293
saturated waveform when we
record it.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4429-0
00:34:05.853 --> 00:34:09.859
And so we have actually several
projects in the pipeline where
e1a6d0f5-c720-4206-b6ae-9c1973856016/4429-1
00:34:09.859 --> 00:34:13.165
we're trying to use deep
learning methods to try to
e1a6d0f5-c720-4206-b6ae-9c1973856016/4429-2
00:34:13.165 --> 00:34:16.408
recover the original waveform
and then do use more
e1a6d0f5-c720-4206-b6ae-9c1973856016/4429-3
00:34:16.408 --> 00:34:20.097
conventional early warning
methods on these reconstructed
e1a6d0f5-c720-4206-b6ae-9c1973856016/4429-4
00:34:20.097 --> 00:34:20.733
waveforms.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4440-0
00:34:22.193 --> 00:34:25.926
And the 2nd Ave. that we're
gonna develop further is trying
e1a6d0f5-c720-4206-b6ae-9c1973856016/4440-1
00:34:25.926 --> 00:34:26.113
to.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4450-0
00:34:26.663 --> 00:34:30.885
And develop this this real time
local back projection pipeline
e1a6d0f5-c720-4206-b6ae-9c1973856016/4450-1
00:34:30.885 --> 00:34:31.623
and seeing.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4467-0
00:34:33.193 --> 00:34:36.866
How it will work in practice
when we have large earthquakes
e1a6d0f5-c720-4206-b6ae-9c1973856016/4467-1
00:34:36.866 --> 00:34:39.193
that are propagating along the
cable?
e1a6d0f5-c720-4206-b6ae-9c1973856016/4478-0
00:34:40.993 --> 00:34:43.393
And with that, I'd like to thank
you for your attention.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4483-0
00:34:52.003 --> 00:34:52.723
Thank you so much.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4491-0
00:34:52.723 --> 00:34:56.826
That was a great talk. We'll
start with any questions in the
e1a6d0f5-c720-4206-b6ae-9c1973856016/4491-1
00:34:56.826 --> 00:34:57.163
room.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4493-0
00:34:57.163 --> 00:34:58.563
We're gonna wrap it.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4499-0
00:35:00.173 --> 00:35:01.333
Anne Marie has a question.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4503-0
00:35:01.333 --> 00:35:03.133
And remember, the mic is behind
you, right?
e1a6d0f5-c720-4206-b6ae-9c1973856016/4508-0
00:35:04.673 --> 00:35:05.433
This is Ann revolte.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4509-0
00:35:05.433 --> 00:35:06.033
Thanks so much.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4516-0
00:35:06.033 --> 00:35:07.353
That was a really clear talk.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4518-0
00:35:07.633 --> 00:35:08.433
I'm just curious.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4522-0
00:35:10.233 --> 00:35:10.833
Your conclusion?
e1a6d0f5-c720-4206-b6ae-9c1973856016/4564-0
00:35:10.833 --> 00:35:14.470
How how much of your conclusions
about the dynamic range are
e1a6d0f5-c720-4206-b6ae-9c1973856016/4564-1
00:35:14.470 --> 00:35:17.930
dependent on this particular
setup? And I don't know much
e1a6d0f5-c720-4206-b6ae-9c1973856016/4564-2
00:35:17.930 --> 00:35:21.508
about DOS at all, but there's
certainly parameters that you
e1a6d0f5-c720-4206-b6ae-9c1973856016/4564-3
00:35:21.508 --> 00:35:24.907
put in that are specific to
something about the cable, I
e1a6d0f5-c720-4206-b6ae-9c1973856016/4564-4
00:35:24.907 --> 00:35:27.353
guess and or the the attenuation
in the.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4568-0
00:35:27.513 --> 00:35:28.753
Region offshore Chile.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4583-0
00:35:30.273 --> 00:35:34.342
Yeah. Well, let me just go back
to the very first criterion that
e1a6d0f5-c720-4206-b6ae-9c1973856016/4583-1
00:35:34.342 --> 00:35:36.033
I had on on the slide here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4591-0
00:35:37.593 --> 00:35:40.713
So this this criterion that you
have over here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4615-0
00:35:42.393 --> 00:35:45.550
Kind of is is sort of shared by
the majority of DAS
e1a6d0f5-c720-4206-b6ae-9c1973856016/4615-1
00:35:45.550 --> 00:35:49.316
interrogators, at least as far
as I can tell, because I'm not
e1a6d0f5-c720-4206-b6ae-9c1973856016/4615-2
00:35:49.316 --> 00:35:50.713
really a photonics guy.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4634-0
00:35:50.713 --> 00:35:53.593
So I don't know the exact
details of how these
e1a6d0f5-c720-4206-b6ae-9c1973856016/4634-1
00:35:53.593 --> 00:35:57.392
interrogators work, but from
what I've gathered by discussing
e1a6d0f5-c720-4206-b6ae-9c1973856016/4634-2
00:35:57.392 --> 00:35:59.353
with with various manufacturers.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4649-0
00:36:00.763 --> 00:36:03.757
This is would be the
relationship that would apply to
e1a6d0f5-c720-4206-b6ae-9c1973856016/4649-1
00:36:03.757 --> 00:36:05.643
a lot of interrogators out
there.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4672-0
00:36:07.233 --> 00:36:10.426
Because this is simply the sort
of measurement principle of
e1a6d0f5-c720-4206-b6ae-9c1973856016/4672-1
00:36:10.426 --> 00:36:13.833
tasks, and that is really just a
matter of how you estimate the
e1a6d0f5-c720-4206-b6ae-9c1973856016/4672-2
00:36:13.833 --> 00:36:14.153
phase.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4686-0
00:36:15.093 --> 00:36:18.758
But using most standard ways of
estimating phase, this is what
e1a6d0f5-c720-4206-b6ae-9c1973856016/4686-1
00:36:18.758 --> 00:36:19.573
you would get.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4711-0
00:36:19.573 --> 00:36:23.881
And So what goes in there is the
wavelength of light, which is,
e1a6d0f5-c720-4206-b6ae-9c1973856016/4711-1
00:36:23.881 --> 00:36:27.853
well, kind of fixed by the the
core diameter of the fiber.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4719-0
00:36:28.293 --> 00:36:30.978
And then you have the refractive
index and the photodetect
e1a6d0f5-c720-4206-b6ae-9c1973856016/4719-1
00:36:30.978 --> 00:36:32.253
coefficient that are simply.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4736-0
00:36:33.793 --> 00:36:37.668
Material properties of the fibre
and then these two guys here are
e1a6d0f5-c720-4206-b6ae-9c1973856016/4736-1
00:36:37.668 --> 00:36:39.313
your acquisition parameters.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4749-0
00:36:39.953 --> 00:36:43.698
So if you could go to a very
high time, something like very
e1a6d0f5-c720-4206-b6ae-9c1973856016/4749-1
00:36:43.698 --> 00:36:46.633
high spatial something rate, you
could really.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4781-0
00:36:47.333 --> 00:36:52.129
Bump up this dynamic range by a
lot, but unfortunately this time
e1a6d0f5-c720-4206-b6ae-9c1973856016/4781-1
00:36:52.129 --> 00:36:56.556
sampling rate is kind of has
like an upper bound by the the
e1a6d0f5-c720-4206-b6ae-9c1973856016/4781-2
00:36:56.556 --> 00:37:01.131
range of your cable like. The
longer you are sensing in terms
e1a6d0f5-c720-4206-b6ae-9c1973856016/4781-3
00:37:01.131 --> 00:37:05.633
of range, the longer you have to
wait for the light to come.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4798-0
00:37:05.633 --> 00:37:09.548
Back and so there is an upper
limit to how well I would say a
e1a6d0f5-c720-4206-b6ae-9c1973856016/4798-1
00:37:09.548 --> 00:37:12.453
lower limit of how small this
delta T can be.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4812-0
00:37:13.233 --> 00:37:17.538
And likewise there is a limit on
how small your gauge length or
e1a6d0f5-c720-4206-b6ae-9c1973856016/4812-1
00:37:17.538 --> 00:37:19.153
spatial sampling can be.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4825-0
00:37:19.933 --> 00:37:24.813
And so really there is a bounds
to how how large the strain
e1a6d0f5-c720-4206-b6ae-9c1973856016/4825-1
00:37:24.813 --> 00:37:27.173
rates you can you can record.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4836-0
00:37:31.193 --> 00:37:34.830
Awesome. Thanks. We're having a
little bit of static, I think
e1a6d0f5-c720-4206-b6ae-9c1973856016/4836-1
00:37:34.830 --> 00:37:36.473
from potentially your audio.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4842-0
00:37:37.803 --> 00:37:38.723
Ah, OK.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4855-0
00:37:38.033 --> 00:37:40.950
I'm not sure if there's anything
you can check your plug in or
e1a6d0f5-c720-4206-b6ae-9c1973856016/4855-1
00:37:40.950 --> 00:37:42.433
connection, but we can hear you.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4857-0
00:37:42.303 --> 00:37:42.423
Umm.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4861-0
00:37:42.433 --> 00:37:44.033
But there's just a little bit of
background static.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4870-0
00:37:45.463 --> 00:37:47.743
OK, it might be Internet
connection.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4877-0
00:37:48.623 --> 00:37:51.103
I'm not hearing anything myself
over here so.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4879-0
00:37:51.133 --> 00:37:51.573
OK, OK.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4891-0
00:37:52.093 --> 00:37:54.693
Well, we'll keep going forward,
but if it gets worse, I'll, I'll
e1a6d0f5-c720-4206-b6ae-9c1973856016/4891-1
00:37:54.693 --> 00:37:55.213
let you know.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4890-0
00:37:55.643 --> 00:37:55.923
OK.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4895-0
00:37:56.833 --> 00:37:58.553
So questions in the room.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4903-0
00:38:01.463 --> 00:38:04.223
If not, then we'll go to Ben
Brooks again, question.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4907-0
00:38:05.503 --> 00:38:06.383
Can you hear me OK?
e1a6d0f5-c720-4206-b6ae-9c1973856016/4908-0
00:38:06.883 --> 00:38:07.363
Yes.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4920-0
00:38:08.233 --> 00:38:12.953
Yeah, maybe the static is the
the desk saturation possible.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4926-0
00:38:15.633 --> 00:38:16.593
Thanks for thanks.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4941-0
00:38:16.633 --> 00:38:19.975
Really interesting. And as Emory
said, really clearly presented
e1a6d0f5-c720-4206-b6ae-9c1973856016/4941-1
00:38:19.975 --> 00:38:22.273
talk and sorry if this is a
silly question.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4963-0
00:38:22.433 --> 00:38:26.208
The slide that you showed where
you were detecting the open
e1a6d0f5-c720-4206-b6ae-9c1973856016/4963-1
00:38:26.208 --> 00:38:30.046
ocean swells moved a little fast
for me to see what what the
e1a6d0f5-c720-4206-b6ae-9c1973856016/4963-2
00:38:30.046 --> 00:38:33.443
periods were, but is there any
possibility of tsunami
e1a6d0f5-c720-4206-b6ae-9c1973856016/4963-3
00:38:33.443 --> 00:38:34.073
detection?
e1a6d0f5-c720-4206-b6ae-9c1973856016/4981-0
00:38:35.743 --> 00:38:39.166
Yeah, that's very interesting
question. And I think there are
e1a6d0f5-c720-4206-b6ae-9c1973856016/4981-1
00:38:39.166 --> 00:38:41.983
several groups in the world
working on that topic.
e1a6d0f5-c720-4206-b6ae-9c1973856016/4999-0
00:38:42.783 --> 00:38:47.698
We actually have a PhD student
at Yale who looked at these sort
e1a6d0f5-c720-4206-b6ae-9c1973856016/4999-1
00:38:47.698 --> 00:38:50.463
of theoretical feasibility of
that.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5034-0
00:38:52.033 --> 00:38:56.238
And then kind of towards the end
of his PhD, other people
e1a6d0f5-c720-4206-b6ae-9c1973856016/5034-1
00:38:56.238 --> 00:39:00.588
actually published the first
sort of sightings of a tsunami
e1a6d0f5-c720-4206-b6ae-9c1973856016/5034-2
00:39:00.588 --> 00:39:04.793
with DAZ, although it's, it was
very faint in my opinion.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5047-0
00:39:05.803 --> 00:39:09.762
But certainly if you, especially
if you have a shallow cable or
e1a6d0f5-c720-4206-b6ae-9c1973856016/5047-1
00:39:09.762 --> 00:39:11.123
like in shallow water.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5061-0
00:39:12.673 --> 00:39:16.393
It is quite likely that that you
can record a tsunami.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5096-0
00:39:17.713 --> 00:39:21.678
I've also been asked whether
that can actually saturate the
e1a6d0f5-c720-4206-b6ae-9c1973856016/5096-1
00:39:21.678 --> 00:39:25.180
desk recordings which maybe
would have been a second
e1a6d0f5-c720-4206-b6ae-9c1973856016/5096-2
00:39:25.180 --> 00:39:29.079
question you wanted to ask, but
that is not very likely to
e1a6d0f5-c720-4206-b6ae-9c1973856016/5096-3
00:39:29.079 --> 00:39:32.846
happen. So tsunami seem to be
sitting in a sort of happy
e1a6d0f5-c720-4206-b6ae-9c1973856016/5096-4
00:39:32.846 --> 00:39:35.953
medium between being detectable
and still not.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5101-0
00:39:36.073 --> 00:39:37.233
Saturating the data.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5106-0
00:39:39.523 --> 00:39:40.203
Yeah, I wonder.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5116-0
00:39:41.003 --> 00:39:43.590
I mean, maybe you could design
some kind of match filter,
e1a6d0f5-c720-4206-b6ae-9c1973856016/5116-1
00:39:43.590 --> 00:39:44.483
something like that.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5123-0
00:39:44.483 --> 00:39:47.723
That might help you with the the
seismic aspect of it.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5133-0
00:39:51.193 --> 00:39:53.153
I mean in terms of detection or?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5162-0
00:39:53.483 --> 00:39:58.283
Yeah. Yeah. I mean, if you could
potentially use use coincident
e1a6d0f5-c720-4206-b6ae-9c1973856016/5138-0
00:39:54.793 --> 00:39:54.953
Kind of.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5162-1
00:39:58.283 --> 00:40:02.783
tsunami data or model to feed
back into your detection, but
e1a6d0f5-c720-4206-b6ae-9c1973856016/5162-2
00:40:02.783 --> 00:40:06.683
that might not be useful in the
time period of eew.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5167-0
00:40:08.193 --> 00:40:08.633
But maybe.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5187-0
00:40:08.203 --> 00:40:12.123
Yeah, normally you don't want to
wait for tsunami to pass by to
e1a6d0f5-c720-4206-b6ae-9c1973856016/5187-1
00:40:12.123 --> 00:40:14.083
send out an an earthquake alert.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5182-0
00:40:12.203 --> 00:40:12.403
Right.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5201-0
00:40:14.083 --> 00:40:18.331
So I mean it does have to
propagate to be detectable over
e1a6d0f5-c720-4206-b6ae-9c1973856016/5192-0
00:40:15.593 --> 00:40:16.033
Exactly.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5201-1
00:40:18.331 --> 00:40:20.163
by the, by the cable, so.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5229-0
00:40:20.663 --> 00:40:25.125
Just maybe more in terms of just
source, you know and and so so
e1a6d0f5-c720-4206-b6ae-9c1973856016/5215-0
00:40:25.023 --> 00:40:25.903
Yes. Yeah.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5229-1
00:40:25.125 --> 00:40:29.587
near near real time situational
awareness instead of instead of
e1a6d0f5-c720-4206-b6ae-9c1973856016/5229-2
00:40:29.587 --> 00:40:30.703
EW specifically.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5231-0
00:40:31.483 --> 00:40:32.083
Yeah, yeah.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5233-0
00:40:33.793 --> 00:40:34.073
Yes.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5235-0
00:40:34.803 --> 00:40:35.363
No, thank you.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5238-0
00:40:37.103 --> 00:40:38.583
I think Theresa, good question.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5244-0
00:40:41.283 --> 00:40:42.443
Yes, hi. My name.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5251-0
00:40:42.443 --> 00:40:44.163
Thank you so much for your talk.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5259-0
00:40:44.163 --> 00:40:48.483
I'm actually calling in from the
DAS SSA Photonics conference.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5268-0
00:40:50.033 --> 00:40:52.033
And so this is very appropriate
on brand.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5273-0
00:40:52.713 --> 00:40:53.873
I have a few questions.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5291-0
00:40:53.873 --> 00:40:59.434
One, I think I saw in your map
that the cable may be actually
e1a6d0f5-c720-4206-b6ae-9c1973856016/5291-1
00:40:59.434 --> 00:41:02.753
crossing a fault line. Is that
true?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5309-0
00:41:03.353 --> 00:41:08.327
And if so, or maybe even in any
case, are you worried in the
e1a6d0f5-c720-4206-b6ae-9c1973856016/5309-1
00:41:08.327 --> 00:41:11.753
event of a large earthquake of
the cable?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5311-0
00:41:12.853 --> 00:41:13.813
Breaking.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5333-0
00:41:16.143 --> 00:41:20.197
Well, it's quite likely that
there are several smaller faults
e1a6d0f5-c720-4206-b6ae-9c1973856016/5333-1
00:41:20.197 --> 00:41:23.663
on the sea floor that are either
mapped or unmapped.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5354-0
00:41:25.233 --> 00:41:29.712
But these are commercial telecom
cables, so these have been sort
e1a6d0f5-c720-4206-b6ae-9c1973856016/5354-1
00:41:29.712 --> 00:41:32.193
of tried and tested over the
years.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5357-0
00:41:32.753 --> 00:41:34.753
So at least over the last few
years.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5382-0
00:41:36.393 --> 00:41:39.849
Where there were significant
earthquakes but none of them
e1a6d0f5-c720-4206-b6ae-9c1973856016/5382-1
00:41:39.849 --> 00:41:43.485
managed to actually break the
cable, you would have to be, I
e1a6d0f5-c720-4206-b6ae-9c1973856016/5382-2
00:41:43.485 --> 00:41:45.393
think, pretty unlucky to really.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5394-0
00:41:46.133 --> 00:41:49.173
Snap a cable, but I've heard
reports of it happening.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5412-0
00:41:49.173 --> 00:41:52.995
Then there's always a question
whether it is the ground sort of
e1a6d0f5-c720-4206-b6ae-9c1973856016/5412-1
00:41:52.995 --> 00:41:56.699
displacement itself, or like a
subsequent submarine landslide
e1a6d0f5-c720-4206-b6ae-9c1973856016/5412-2
00:41:56.699 --> 00:41:58.133
that that broke it, but.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5436-0
00:41:59.753 --> 00:42:03.478
Yeah. So that might be a
possibility. Perhaps in the case
e1a6d0f5-c720-4206-b6ae-9c1973856016/5436-1
00:42:03.478 --> 00:42:07.524
of a large earthquakes that any
submarine landslides will kind
e1a6d0f5-c720-4206-b6ae-9c1973856016/5436-2
00:42:07.524 --> 00:42:08.873
of destroy the cable.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5458-0
00:42:10.553 --> 00:42:13.845
But hopefully at that point we
would have already sort of
e1a6d0f5-c720-4206-b6ae-9c1973856016/5458-1
00:42:13.845 --> 00:42:17.478
acquired the data and the data
should be safe and sound at this
e1a6d0f5-c720-4206-b6ae-9c1973856016/5458-2
00:42:17.478 --> 00:42:18.273
landing point.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5461-0
00:42:19.383 --> 00:42:20.023
On land.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5466-0
00:42:20.743 --> 00:42:22.223
So we could still do something
with it.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5470-0
00:42:24.363 --> 00:42:26.163
And then another question is.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5474-0
00:42:28.273 --> 00:42:30.473
For locations.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5486-0
00:42:32.073 --> 00:42:35.793
How certain are you of the
locations of the cables?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5490-0
00:42:35.793 --> 00:42:38.033
Do they drift about?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5499-0
00:42:38.193 --> 00:42:42.233
I mean, I I'm sure they're
buried to some degree, but then.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5505-0
00:42:43.953 --> 00:42:45.033
Do they migrate at all?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5519-0
00:42:45.393 --> 00:42:50.373
Are like do the telecom
companies even know themselves
e1a6d0f5-c720-4206-b6ae-9c1973856016/5519-1
00:42:50.373 --> 00:42:53.633
the exact location of these
cables?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5524-0
00:42:55.283 --> 00:42:57.483
How certain are you of their
locations?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5548-0
00:42:59.053 --> 00:43:02.121
Yeah. So the telecom companies
are not necessarily certain
e1a6d0f5-c720-4206-b6ae-9c1973856016/5548-1
00:43:02.121 --> 00:43:05.501
about the location of the cable,
but they were certain about the
e1a6d0f5-c720-4206-b6ae-9c1973856016/5548-2
00:43:05.501 --> 00:43:07.893
location of the boat that
deployed the cable.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5560-0
00:43:08.333 --> 00:43:12.146
So what we were given was
basically the trajectory of the
e1a6d0f5-c720-4206-b6ae-9c1973856016/5560-1
00:43:12.146 --> 00:43:14.053
boat that deployed the cable.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5575-0
00:43:15.593 --> 00:43:19.070
With with various parameters
like whether the cable was
e1a6d0f5-c720-4206-b6ae-9c1973856016/5575-1
00:43:19.070 --> 00:43:20.313
trenched or not and.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5579-0
00:43:21.953 --> 00:43:22.913
Yeah. So in these cases.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5589-0
00:43:24.633 --> 00:43:28.433
We have sort of a reasonable
grip on where the cable is.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5612-0
00:43:29.753 --> 00:43:33.347
On the orientation, because
depending on the amount of slack
e1a6d0f5-c720-4206-b6ae-9c1973856016/5612-1
00:43:33.347 --> 00:43:36.353
on the cable it could kind of
wiggle a little bit.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5657-0
00:43:36.353 --> 00:43:40.630
And so it could be oriented a
bit more East or West. And we
e1a6d0f5-c720-4206-b6ae-9c1973856016/5657-1
00:43:40.630 --> 00:43:45.193
have seen not for these cables,
but for other cables in shallow
e1a6d0f5-c720-4206-b6ae-9c1973856016/5657-2
00:43:45.193 --> 00:43:49.470
water we have seen some ROV
footage showing that the cables
e1a6d0f5-c720-4206-b6ae-9c1973856016/5657-3
00:43:49.470 --> 00:43:54.033
is well, you know it makes loops
it, it sort of wiggles around.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5659-0
00:43:54.153 --> 00:43:54.753
It's even.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5670-0
00:43:55.553 --> 00:43:59.722
Managed to get sort of suspend
in the air by a chair on the sea
e1a6d0f5-c720-4206-b6ae-9c1973856016/5670-1
00:43:59.722 --> 00:44:00.113
floor.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5698-0
00:44:01.403 --> 00:44:04.783
So all sorts of weird things
happen on the sea floor with the
e1a6d0f5-c720-4206-b6ae-9c1973856016/5698-1
00:44:04.783 --> 00:44:07.891
cable, but at least the location
is sort of more or less
e1a6d0f5-c720-4206-b6ae-9c1973856016/5698-2
00:44:07.891 --> 00:44:11.163
constrained by the trajectory of
the ship that deployed it.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5711-0
00:44:12.713 --> 00:44:15.953
But yeah, it will not be super
precise.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5731-0
00:44:15.953 --> 00:44:19.222
So depending on what you want to
do, you might have to do a
e1a6d0f5-c720-4206-b6ae-9c1973856016/5731-1
00:44:19.222 --> 00:44:22.328
survey to actually locate the
cable, which could be very
e1a6d0f5-c720-4206-b6ae-9c1973856016/5731-2
00:44:22.328 --> 00:44:22.873
expensive.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5749-0
00:44:25.783 --> 00:44:31.257
And then one last question,
looking at the equation you were
e1a6d0f5-c720-4206-b6ae-9c1973856016/5749-1
00:44:31.257 --> 00:44:36.103
giving in terms of magnitude and
the the propagation.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5751-0
00:44:37.673 --> 00:44:38.233
Term.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5756-0
00:44:43.263 --> 00:44:45.343
Yeah. The that middle term
there.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5762-0
00:44:46.913 --> 00:44:48.593
Does that have? Like any?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5779-0
00:44:48.593 --> 00:44:52.782
Yeah, the propagation medium
does that take into account the
e1a6d0f5-c720-4206-b6ae-9c1973856016/5779-1
00:44:52.782 --> 00:44:55.873
conduit conditions or the burial
conditions.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5788-0
00:44:55.873 --> 00:45:00.553
Because I know that can really
affect the amplitude.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5795-0
00:45:02.393 --> 00:45:05.273
Of recording of the DAS cable.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5802-0
00:45:07.433 --> 00:45:08.113
So does that.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5807-0
00:45:08.113 --> 00:45:12.393
Is that taken into account in
this equation anywhere?
e1a6d0f5-c720-4206-b6ae-9c1973856016/5814-0
00:45:13.593 --> 00:45:15.673
Yeah, that's that's a that's a
really good point.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5831-0
00:45:15.673 --> 00:45:21.518
And you can actually see it in
the wave forms a little bit. If
e1a6d0f5-c720-4206-b6ae-9c1973856016/5831-1
00:45:21.518 --> 00:45:24.673
I go back to the waterfall
plots.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5868-0
00:45:24.993 --> 00:45:28.936
Yeah. So you can see here that
there seems to be some sort of
e1a6d0f5-c720-4206-b6ae-9c1973856016/5868-1
00:45:28.936 --> 00:45:32.815
gaps in the recordings these
sort of vertical whitish lines,
e1a6d0f5-c720-4206-b6ae-9c1973856016/5868-2
00:45:32.815 --> 00:45:36.822
those are sections of the cable
that are not very well coupled
e1a6d0f5-c720-4206-b6ae-9c1973856016/5868-3
00:45:36.822 --> 00:45:37.713
to the ground.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5875-0
00:45:37.913 --> 00:45:40.873
And so they record amplitudes at
much lower values.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5879-0
00:45:41.673 --> 00:45:42.873
Than well coupled sections.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5883-0
00:45:43.663 --> 00:45:44.863
And this is another.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5887-0
00:45:46.553 --> 00:45:47.433
Avenue to to explore.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5913-0
00:45:49.233 --> 00:45:53.486
Because if these if the coupling
coefficient is basically just
e1a6d0f5-c720-4206-b6ae-9c1973856016/5913-1
00:45:53.486 --> 00:45:57.605
sort of a scalar multiplier that
it doesn't affect frequency
e1a6d0f5-c720-4206-b6ae-9c1973856016/5913-2
00:45:57.605 --> 00:45:58.753
content too much.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5932-0
00:46:00.473 --> 00:46:04.539
And if it is sort of just linear
and constant in time, then we
e1a6d0f5-c720-4206-b6ae-9c1973856016/5932-1
00:46:04.539 --> 00:46:06.153
can actually use this as.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5950-0
00:46:07.753 --> 00:46:11.316
Sections that have sort of an
apparently higher dynamic range
e1a6d0f5-c720-4206-b6ae-9c1973856016/5950-1
00:46:11.316 --> 00:46:14.938
because they simply did records
the the wave fields with lower
e1a6d0f5-c720-4206-b6ae-9c1973856016/5950-2
00:46:14.938 --> 00:46:15.513
amplitude.
e1a6d0f5-c720-4206-b6ae-9c1973856016/5953-0
00:46:17.403 --> 00:46:17.883
From what?
e1a6d0f5-c720-4206-b6ae-9c1973856016/6003-0
00:46:17.963 --> 00:46:22.371
From some initial exploration,
we found that the variation in
e1a6d0f5-c720-4206-b6ae-9c1973856016/6003-1
00:46:22.371 --> 00:46:26.425
this coupling factors of the
order of a factor 10, which
e1a6d0f5-c720-4206-b6ae-9c1973856016/6003-2
00:46:26.425 --> 00:46:30.763
sounds like a lot, but because
of the logarithmic scaling of
e1a6d0f5-c720-4206-b6ae-9c1973856016/6003-3
00:46:30.763 --> 00:46:35.100
magnitudes, it doesn't help that
much. In the end, you would
e1a6d0f5-c720-4206-b6ae-9c1973856016/6003-4
00:46:35.100 --> 00:46:37.803
really need sections that have a
cou.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6017-0
00:46:38.043 --> 00:46:43.105
Of this, less than essentially
maybe like a factor of 1000 or
e1a6d0f5-c720-4206-b6ae-9c1973856016/6017-1
00:46:43.105 --> 00:46:45.963
so, in order to faithfully
record.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6020-0
00:46:46.723 --> 00:46:47.043
The wave forms.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6031-0
00:46:47.533 --> 00:46:50.613
But we actually do have a few of
those channels on land.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6059-0
00:46:50.613 --> 00:46:55.460
So if you look here close to the
edge of each of the panels, this
e1a6d0f5-c720-4206-b6ae-9c1973856016/6059-1
00:46:55.460 --> 00:47:00.160
is a section that is on land and
those sections were not at all
e1a6d0f5-c720-4206-b6ae-9c1973856016/6059-2
00:47:00.160 --> 00:47:04.053
saturated. And that gave us this
waveform over here.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6089-0
00:47:05.603 --> 00:47:09.192
So it is possible, but you have
to be lucky that certain
e1a6d0f5-c720-4206-b6ae-9c1973856016/6089-1
00:47:09.192 --> 00:47:13.348
sections are sufficiently poorly
coupled to be able to record the
e1a6d0f5-c720-4206-b6ae-9c1973856016/6089-2
00:47:13.348 --> 00:47:15.363
waveform without any distortion.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6095-0
00:47:15.363 --> 00:47:18.963
And then there's the question,
do you really record the wave?
e1a6d0f5-c720-4206-b6ae-9c1973856016/6107-0
00:47:19.533 --> 00:47:23.773
Form properly? Or is there like
other factors involved?
e1a6d0f5-c720-4206-b6ae-9c1973856016/6100-0
00:47:19.933 --> 00:47:21.213
So OK.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6112-0
00:47:26.623 --> 00:47:27.423
Thank you so much.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6114-0
00:47:27.423 --> 00:47:28.743
I've really enjoyed your talk.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6116-0
00:47:29.533 --> 00:47:30.053
No, thank you.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6123-0
00:47:32.353 --> 00:47:35.313
OK. Questions. Any more
questions in the room?
e1a6d0f5-c720-4206-b6ae-9c1973856016/6133-0
00:47:36.883 --> 00:47:39.763
Everybody. And I'm not seeing
any more questions online.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6134-0
00:47:39.763 --> 00:47:40.963
Last chance, anybody?
e1a6d0f5-c720-4206-b6ae-9c1973856016/6142-0
00:47:43.213 --> 00:47:45.835
OK, then let's go ahead and take
Martian one more time for his
e1a6d0f5-c720-4206-b6ae-9c1973856016/6142-1
00:47:45.835 --> 00:47:46.293
great talk.
e1a6d0f5-c720-4206-b6ae-9c1973856016/6147-0
00:47:50.503 --> 00:47:51.823
And you was a pleasure to be
there.