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This is geology B with Oliver's 
trampled. 

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We all know about the massive 
earthquake that occurred in 

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March 2011 off the east coast of
Japan. 

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It had a registered magnitude 
greater than 9.0 making it the 

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most powerful earthquake ever 
recorded in Japan and the fourth

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most powerful earthquake in the 
world. 

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Since modern record keeping 
began in 1900, it triggered its 

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tsunami with waves of up to 40 
meters that swept ashore. 

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Killing nearly 20,000 people and
causing the Fukushima. 

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And Nuclear disaster, the 
earthquake occurred. 

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Where the Pacific Plate is 
subducting under the plate that 

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Lies Beneath the Japanese island
of Honshu. 

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During the earthquake, the 
Eastern edge of the overriding 

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plate. 
Jumped over 50 meters to the 

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east over a length of about 500 
kilometers. 

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It was this unexpectedly large 
slip, that displaced enough 

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water to set the giant tsunami 
in motion. 

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Why was the slip so large? 
Was it something to do with the 

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nature of the fault Zone on the 
boundary between the two plates 

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as it nears, the Japan trench 
Patrick Fulton led a team that 

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probe, the tohoku. 
Okay, earthquake fault, which is

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the Fault along which the main 
rupture occurred, his team, 

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overcame enormous engineering 
challenges to install what he 

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calls a temperature, 
Observatory? 

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Right through the fault Zone, 
the observations revealed the 

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temperature. 
I peek across the fault which in

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turn enabled him to estimate the
coefficient of dynamic friction 

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at the plate boundary and it 
turned out to be extremely low. 

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Patrick Fulton is an assistant 
professor in the department of 

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Earth and atmospheric sciences 
at Cornell University. 

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Patrick Fulton, welcome to 
geology B. 

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Thank you. 
And thank you for having me. 

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Can we start with a bit of 
tectonic context for the 

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subduction zone off? 
The east coast of Japan? 

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Does Japan's sit on its own 
plate, or is it on the Eastern 

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edge of a Eurasian plate? 
Japan is actually in a 

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Confluence of a number of 
different plates. 

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The northern part of Japan where
this earthquake happened 

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actually sits on the North 
American Plate. 

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And some people will see that 
the plate goes all the way 

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around, from the United States 
up through Canada, around from 

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Alaska. 
And reaches down into the 

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northern part of Japan. 
Some people call that little 

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part of it. 
In Japan. 

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The acoustic plate kind of a 
micro plate and then when it 

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hits Mount Fuji, south of Tokyo,
that's where it intersects with 

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the Eurasian plate and how fast 
of the plates, converging in the

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region, where the earthquake 
occurred somewhere around eight 

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centimeters per year. 
I think that must be one of the 

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faster convergence speeds of 
plates around the planet. 

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That's right, it's fast. 
And some of it's because the 

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rocks are old and cold roughly, 
130 million years and that old 

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cold rocks are fairly tense. 
And it's trying to sink down 

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into these the unisphere. 
So slab pull is especially 

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effective for that reason. 
So what exactly happens when an 

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earthquake occurs along a 
subduction zone, so when the 

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down going oceanic plates are 
pulled down from their own 

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weight. 
Into the steam is for they get 

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stuck to the overlying plate and
they build up elastic energy and

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every once in a while, they 
relieve that elastic energy, and

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that's what we observe is. 
And how deep down does the 

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earthquake normally start? 
Does that stress? 

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Get released. 
So in subduction zones, about 30

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kilometers depth is where we see
a lot of earthquake starts. 

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That's fine. 
The middle of the seismic Janek 

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Zone on was the tohoku 
earthquake at that depth. 

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It was it was about 30 
kilometers deep. 

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As I said in the introduction 
there was a 50 meter slip 

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recorded at the surface and that
was unexpectedly large. 

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What would one normally expect 
for such an earthquake and and 

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what can we infer from this 
enormously large slip? 

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Yeah this was a very interesting
and confusing earthquake. 

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Generally we thought that most 
of the slip would happen where 

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they start. 
So at 30 kilometers depth you 

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mapped out on a map where the 
Contours of sip were you would 

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see maybe at the beginning of 
the earthquake you had somewhere

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around 5 or 10 meters or sip and
then it would Decay out as the 

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rupture try to expand it would 
essentially hit the brakes. 

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The surrounding rocks and died 
out. 

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That was not the case in this 
earthquake. 

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And this earthquake, most of the
slip actually happened at the 

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very shallowest parts. 
So where it was roughly 30 

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meters, a huge amount of slip 
down where it started at the 

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shallowest part. 
At the sea floor, it jumped as 

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much as 50, 60 meters. 
That reminds me of the podcast I

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did with Roger bilham in which 
he talked about the earthquake 

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in 2015, in goloka in the Paul. 
And in that case, the rupture 

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did not propagate to the 
surface, the brakes, if you like

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were effective, thus, the stress
was built up further along the 

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fault, and everyone's expecting 
another big Quake sometime soon.

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They're so why do we think this 
one was so different? 

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This is really kind of the big 
question and kind of motivated, 

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some of our work on land. 
Like in the Corker earthquake, 

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the rocks are strong and they 
are brittle and they break, but 

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sometimes they don't go all the 
way to the surface. 

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It's because they intersect 
areas where it's a bunch of soft

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sediments where the rupture kind
of will dissipate into different

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areas or may deform more 
plastically. 

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Some of the rocks and sediments 
above it here. 

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We think in subduction zones, 
the rocks are often softer, 

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especially when they get to the 
shadow parts that we almost 

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never have really seen a surface
break like this or at least of 

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this magnitude. 
And so that led to a lot of 

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questions about why the shallow 
part Slip so much was it because

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the shallow part was really 
strong and built up. 

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A lot of elastic energy or was 
it really weak? 

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And the rupture came through. 
And it just essentially 

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hydroplaned didn't have any 
brakes on the show. 

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Part that actually takes us to 
your work which was indeed to 

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probe the fault Zone to see if 
you could gather data that would

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help us figure out what the 
friction walls along the 

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surface. 
So how did you go about this one

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way that we can figure out how 
much She resistance or how much 

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brakes were on the float when it
slipped is by measuring, how 

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much heat is generated during 
the earthquake. 

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So, just like when you rub your 
hands together, it generates 

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heat. 
And it's a function of how much 

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you move them pass each other to
displacement, but also how much 

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force and friction is between 
your hands as you're sharing it.

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So if we could measure how much 
heat was generated on the fault,

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we could figure out this big 
question and to do that meant 

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that we would have to drill down
at depth where the earthquake 

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happened and measured any 
temperature anomaly measure the 

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excess heat across the fault 
after an earthquake, which is 

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really challenging because that 
heat could generate really hot 

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temperatures. 
May be up to 1000 degrees on the

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fault in a very thin Zone. 
Maybe it's CM thick during the 

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earthquake, but then it diffuses
into the surroundings. 

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And so, we figured that we would
have to be there within about a 

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year or two. 
Afterwards to be able to do 

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that. 
And this earthquake with a lot 

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of slip will give it a very big 
signature, and because so much 

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of that soup was that shallow 
depth? 

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It meant that perhaps, we could 
actually drill into it and put 

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sensors down there, to actually 
measure the temperature anomaly 

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across the fall. 
How's anyone successfully 

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measured temperature normally 
across the fault during all 

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right. 
After an earthquake, not quite 

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there has been a few attempts 
particularly After the chi chi 

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earthquake in Taiwan large 
earthquake. 

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But there it took many years 
before they could drill across 

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the fault and I could only get 
one profile of temperature 

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before the hole collapsed. 
So if you see something across 

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the fault, you don't know 
whether that little temperature 

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blip is really due to frictional
heat does it diffuse over time 

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as you would expect, or is it 
due to water flowing through a 

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fracture? 
Or is it maybe just due to 

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differences in rock type as you 
go? 

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So we learned a lot from that 
experience. 

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We learned that you really need 
to monitor the temperature over 

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time. 
And you really need to get a 

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good understanding of the Rocks 
themselves. 

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Take core samples, and rock 
samples. 

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There's also been a long-term 
study of trying to look for 

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frictional, heat, not from a 
single earthquake, but over 

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millions of years of shearing, 
along the San Andreas fault. 

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And there you would expect a 
large increase over many 

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kilometers of heat, coming out 
around the The fault Zone and 

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there it was not observed, 
despite a lot of attempts, 

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including some of my own during 
my PhD, which has led us to 

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think that maybe rocks, aren't 
as strong as we think they are 

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at least how they behave in the 
lab. 

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Maybe there is something 
different during an earthquake 

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or something different about 
mature plate. 

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Boundary fault zones. 
That makes it all the more 

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interesting that you actually 
were successful in determining a

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temperature anomaly. 
So, as I mentioned earlier, you 

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went about this bye. 
Installing what you call a 

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temperature Observatory, tell us
about what that is and how you 

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did that. 
Exactly. 

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So one of the big challenges 
with this project is that 

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perhaps we could drill Across 
The Fault in a place where it 

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had a lot of slip and perhaps 
measure the temperature across 

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it. 
But to do that, we were just at 

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the limits of where 
technologically, we could 

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actually drill. 
We're working in a water depth 

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of 7 km and then the fault Zone.
The Beneath that was another 

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eight hundred and twenty meters 
below the sea floor. 

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So, no one had ever drilled that
deep within the ocean before let

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alone trying to put instruments 
under there. 

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So to do that, we first had to 
characterize the hole, we 

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drilled and found out exactly 
where the fault was first. 

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We took core samples out. 
We did you physical lugging but 

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now we drilled underneath the 
sea floor and we put a 

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protective casing at the very 
shallow part just so that we 

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Reenter the whole, then we built
the observatories. 

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So we built a 855 M, long steel 
pipe inside of it. 

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We built our temperature 
Observatory, which was 

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essentially a static climbing 
rope, or a rope. 

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That does not stretch much where
we had woven in temperature 

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sensors, each of them with their
own Data Logger and each of them

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encased in titanium. 
So all the electronics would not

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implode, do the huge pressures 
at those steps? 

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And then the temperature sensors
themselves, Elves have an 

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accuracy of a thousandth of a 
degree celsius. 

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We want to be able to see just 
the smallest little details in 

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the smallest little increases of
what the temperature is. 

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So we then lower that down to 
the sea floor, and then 

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re-entered the hole and install 
that bit of casing, all the way 

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down. 
And then left it there, and went

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away for several months and then
came back to collect the data, 

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those temperature sensors, 55 of
them, at different depths were 

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measuring the You're at those 
steps over time and once the 

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whole rig equilibrated, we could
see if we saw a temperature 

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anomaly Crossville just before 
we get to your results. 

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I'm completely boggled by the 
idea that you could return to a 

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hole that I don't know what is 
it about a meter across or 

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something at the depth of 7 
kilometers of water from a ship 

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that's like floating on the 
waves above. 

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How on Earth is that possible? 
Well it's just barely possible. 

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So essentially we have 850 M 
long Observatory of steel pipe 

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connected to another seven 
kilometers of drill pipe that 

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bring it down to the sea floor 
and we're trying to re-enter 

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that into the hole. 
There's no motor on the bottom 

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of this. 
All we have is the ship, which 

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can use Dynamic positioning to 
stay in one position on the 

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surface of the water. 
But down below, we have a TV 

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camera that can see only a few 
metres ahead of it at the 

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bottom. 
Of the whole assembly. 

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And so with the light on it we 
could see where we are. 

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We tell the captain. 
Well we think it might be over 

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to the north and he/she will 
move the ship over there. 

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And then the whole thing, all 
that steel pipe below us it's 

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like a wet. 
Spaghetti noodle. 

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It's just hanging there in it. 
Slowly starts to wiggle over in 

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that direction in response. 
And we did that for many hours 

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until we see the observatory or 
the whole rather on the seafloor

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and little bit of Tubing that 
sits above the sea floor. 

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And once we're above it, someone
says now. 

230
00:13:08,700 --> 00:13:12,500
Now now and then the Drillers 
drop everything into it. 

231
00:13:13,000 --> 00:13:14,300
And luckily, it was a 
hole-in-one. 

232
00:13:14,300 --> 00:13:17,500
We got straight in and then 
continue to lower it down. 

233
00:13:17,800 --> 00:13:19,900
That's up to incredible. 
I want to off. 

234
00:13:19,900 --> 00:13:23,200
So how you selected the precise 
location for the whole because 

235
00:13:23,200 --> 00:13:27,800
it seems like you are 850 meters
of Observatory that you could 

236
00:13:27,800 --> 00:13:32,300
feed in below the level of the 
sea floor, the earthquake itself

237
00:13:32,300 --> 00:13:35,700
was at 30 kilometers depth. 
So, obviously, The fault zone of

238
00:13:35,700 --> 00:13:38,200
the fault plane makes it all the
way up. 

239
00:13:38,200 --> 00:13:40,300
Gradually to the surface, at 
some point. 

240
00:13:40,300 --> 00:13:43,800
So how did you pick a point? 
Where the fault plane was at it 

241
00:13:43,800 --> 00:13:48,100
about it said, 820 M down. 
We needed to find a place where 

242
00:13:48,100 --> 00:13:51,600
we could drill across the fault 
at somewhere less than a 

243
00:13:51,600 --> 00:13:54,600
kilometer deep. 
If it's too shallow, maybe we 

244
00:13:54,600 --> 00:13:57,200
start to get to less weight 
acting on things. 

245
00:13:57,200 --> 00:14:00,700
And so, we wanted to find very 
clear position of the fault. 

246
00:14:00,700 --> 00:14:03,500
Less than a kilometer deep 
underneath the ground. 

247
00:14:04,200 --> 00:14:08,000
We also Want to find a place 
where we knew the amount of sip 

248
00:14:08,000 --> 00:14:09,900
fairly well and that it was 
large. 

249
00:14:10,100 --> 00:14:13,800
Here is a position where there 
was clear evidence that it was 

250
00:14:14,000 --> 00:14:17,500
roughly 50 meters of slip. 
The other kind of constraining 

251
00:14:17,500 --> 00:14:22,000
thing was we needed to find a 
place where the water depth was 

252
00:14:22,000 --> 00:14:25,900
less than 7 km. 
And the reason for that is we're

253
00:14:25,900 --> 00:14:28,400
going to put our temperature 
sensors down there and they're 

254
00:14:28,400 --> 00:14:31,000
going to record but we need to 
get them back at some point in 

255
00:14:31,000 --> 00:14:33,800
time. 
There is only one remotely 

256
00:14:33,800 --> 00:14:38,400
operated Essentially an unmanned
submarine that could go to those

257
00:14:38,400 --> 00:14:43,300
depths and pull the sensors out,
get our data back out and its 

258
00:14:43,300 --> 00:14:46,400
maximum operating depth with 
seven kilometers. 

259
00:14:46,700 --> 00:14:51,100
So inside this pipe and you have
your senses, I think you said 55

260
00:14:51,100 --> 00:14:54,000
of them. 
How far apart are they down 

261
00:14:54,000 --> 00:14:58,000
inside that bowl? 
We want to make sure that we can

262
00:14:58,000 --> 00:15:01,300
really see the profile of an 
anomaly. 

263
00:15:01,600 --> 00:15:04,500
And so we made our sensors one 
and a half. 

264
00:15:04,700 --> 00:15:07,900
Meters apart from each other 
anticipating that the full 

265
00:15:07,900 --> 00:15:11,500
anomaly, maybe over some tens of
meters wide. 

266
00:15:11,500 --> 00:15:14,900
And so most of them are about 
one and a half meters apart and 

267
00:15:14,900 --> 00:15:18,000
then X shallower depths we have 
some other ones that have 

268
00:15:18,100 --> 00:15:21,000
further spacing across that 
allow us to get some information

269
00:15:21,000 --> 00:15:24,200
about the background temperature
gradient through the Earth. 

270
00:15:24,400 --> 00:15:28,300
So you then seal the hole and 
left these senses to their own 

271
00:15:28,300 --> 00:15:32,100
devices for about nine months. 
And then you return. 

272
00:15:32,100 --> 00:15:34,500
So how did you pick that time 
interval and what were you? 

273
00:15:34,700 --> 00:15:38,100
During that time with the 
senses, when you first drill the

274
00:15:38,100 --> 00:15:41,900
hole, you get all those broken 
up pieces of rock, out of the 

275
00:15:41,900 --> 00:15:46,300
hole by circulating, cold, ocean
water, so that drilling process 

276
00:15:46,300 --> 00:15:49,700
actually cooled off the whole 
right around the edge of the 

277
00:15:49,700 --> 00:15:53,200
bore hole for a while and it 
would take some time usually a 

278
00:15:53,200 --> 00:15:56,400
few weeks to months to 
re-equilibrate with the 

279
00:15:56,400 --> 00:16:00,500
formation temperatures. 
So then we went away we were 

280
00:16:00,500 --> 00:16:04,500
anxious want to know the answer 
but this is still a very active.

281
00:16:04,700 --> 00:16:07,600
Of plate. 
Boundary fault Zone with lots of

282
00:16:07,600 --> 00:16:11,600
huge aftershocks, including a 
magnitude, 7.3 Aftershock, 

283
00:16:11,600 --> 00:16:15,500
pretty much right at this site, 
on a deeper fault below our 

284
00:16:15,500 --> 00:16:18,600
Observatory. 
And so, we were afraid that with

285
00:16:18,600 --> 00:16:21,400
all of these sensors hanging on 
a rope, if we left it too long, 

286
00:16:21,400 --> 00:16:25,100
maybe the fault was moving and 
it would share through the 

287
00:16:25,100 --> 00:16:28,300
observatory and grab hold of the
sensors and no matter how much 

288
00:16:28,300 --> 00:16:30,700
we tugged on them, we wouldn't 
get them back. 

289
00:16:30,900 --> 00:16:34,500
So, when we first went back, we 
couldn't find the observatory. 

290
00:16:34,900 --> 00:16:40,400
Some of that is just due to the 
challenges of navigating in 

291
00:16:40,400 --> 00:16:44,500
seven kilometers of water depth,
you can use GPS in the air on 

292
00:16:44,500 --> 00:16:47,300
the ship but communicating to 
the ROV underneath. 

293
00:16:47,300 --> 00:16:51,400
You just, the smallest little 
bits of imprecision in your 

294
00:16:51,400 --> 00:16:54,900
communication can lead to you 
being several tens of meters 

295
00:16:54,900 --> 00:16:56,300
away from where you think you 
are. 

296
00:16:56,700 --> 00:17:00,300
But luckily some of our Japanese
colleagues offered by us to use 

297
00:17:00,300 --> 00:17:02,900
some of their time with the our 
review few weeks later. 

298
00:17:02,900 --> 00:17:05,700
We went back and we were able 
Able to find it. 

299
00:17:05,700 --> 00:17:08,800
And I grabbed hold of it with 
the ROV and we pulled it all the

300
00:17:08,800 --> 00:17:11,800
way back up to the seafloor and 
we recovered all of it. 

301
00:17:11,800 --> 00:17:15,000
The fault and not moved. 
It had not shared through 

302
00:17:15,099 --> 00:17:19,200
everything which was actually an
important observation in itself.

303
00:17:19,400 --> 00:17:22,599
It meant that a lot of the 
observations on land where GPS 

304
00:17:22,900 --> 00:17:26,200
sensors were showing that Japan 
was still moving to the east, 

305
00:17:26,300 --> 00:17:30,600
maybe as much as a MM per day, 
it wasn't because of slip on the

306
00:17:30,608 --> 00:17:34,500
fault, it's probably due to 
movements within the man. 

307
00:17:35,100 --> 00:17:39,100
The mantle recovering relaxing 
after having such a big 

308
00:17:39,100 --> 00:17:40,800
earthquake. 
Well, that's fascinating. 

309
00:17:40,800 --> 00:17:42,800
So you're saying the actual 
land. 

310
00:17:42,800 --> 00:17:49,600
Mass of Honshu was moving, but 
the sea flow was not what part 

311
00:17:49,600 --> 00:17:53,200
of the sea floor was, but that 
movement was not between the 

312
00:17:53,200 --> 00:17:56,500
overlying plate in a downgoing 
plate, it was between both of 

313
00:17:56,500 --> 00:18:00,800
those things and the mantle 
underneath was turning a little 

314
00:18:00,800 --> 00:18:03,900
bit after the earthquake. 
So what's the GPS location of 

315
00:18:03,900 --> 00:18:06,200
the ball? 
Actually slightly different when

316
00:18:06,200 --> 00:18:09,700
you came back after 9 months. 
Well, we don't have a very good 

317
00:18:09,800 --> 00:18:14,700
GPS location of it. 
The main issue was that the 

318
00:18:14,700 --> 00:18:17,600
position was correct. 
But our communication, for where

319
00:18:17,600 --> 00:18:21,700
we thought we were was slightly 
Miss calibrated, because of the 

320
00:18:21,700 --> 00:18:24,300
wavelengths that you use to 
communicate from the ship to the

321
00:18:24,300 --> 00:18:27,100
ROV. 
It's just a very long path. 

322
00:18:27,100 --> 00:18:31,600
Any little bit of imprecision 
just adds up and if your 1020 

323
00:18:31,600 --> 00:18:35,400
meters away from where you think
you are down there, You can't 

324
00:18:35,400 --> 00:18:38,200
see very far ahead of you with 
an ROV light. 

325
00:18:38,200 --> 00:18:40,900
Doesn't travel that well, 
through the water and at these 

326
00:18:40,900 --> 00:18:44,200
steps, this is the deepest 
darkest trenches, it is very 

327
00:18:44,200 --> 00:18:45,700
dark down there. 
Okay. 

328
00:18:45,700 --> 00:18:49,200
Well, let's talk about what the 
temperature sensors had logged. 

329
00:18:49,200 --> 00:18:52,600
During those nine months in the 
Bohol, what you found out as is 

330
00:18:52,600 --> 00:18:54,900
the case, pretty much everywhere
on Earth the temperature 

331
00:18:54,900 --> 00:18:58,400
increases as you go deeper, it's
roughly about three degrees on 

332
00:18:58,400 --> 00:19:01,100
the sea floor, and then the 
temperature, it seems to 

333
00:19:01,100 --> 00:19:04,800
increase down to about 25 
degrees Celsius, kind of I'm 

334
00:19:04,800 --> 00:19:08,300
temperature down at the bottom 
of the observatory and if we 

335
00:19:08,300 --> 00:19:11,800
remove that background gradient,
we see the anomalous 

336
00:19:11,800 --> 00:19:15,000
temperatures at first. 
It was cold because of that 

337
00:19:15,000 --> 00:19:18,800
drilling disturbance. 
But then we started to see a 

338
00:19:18,800 --> 00:19:22,500
relatively big temperature, 
anomaly of about Point 3, 

339
00:19:22,800 --> 00:19:27,200
degrees Celsius centered right 
on the fault Zone. 

340
00:19:27,400 --> 00:19:31,100
The same position where we had 
logged in, have all these 

341
00:19:31,100 --> 00:19:34,600
geophysical images of the fault,
we've actually taken. 

342
00:19:34,900 --> 00:19:37,700
Accor sample out from the Vault 
itself. 

343
00:19:37,800 --> 00:19:40,600
Right there is where we see a 
very large temperature. 

344
00:19:40,600 --> 00:19:44,400
Anomaly, that we interpret to be
the frictional heat signature 

345
00:19:44,500 --> 00:19:48,200
from the magnitude 9 earthquake.
How wide is the Fault Zone down 

346
00:19:48,200 --> 00:19:50,200
there? 
Very interesting. 

347
00:19:50,600 --> 00:19:53,600
It's very thin compared to a lot
of other fault zones. 

348
00:19:53,600 --> 00:19:57,400
So, fault Zone has its main 
core. 

349
00:19:57,500 --> 00:20:01,400
It's roughly a couple of meters 
or less than 4 meters, thick and

350
00:20:01,400 --> 00:20:04,600
filled with dense, clay and then
around it. 

351
00:20:04,700 --> 00:20:08,900
There are other subsidiary 
faults and fractures that really

352
00:20:08,900 --> 00:20:11,800
like a knife edge on these 
scales that were talking about. 

353
00:20:11,800 --> 00:20:14,400
So you have your temperature 
signal and you already said you 

354
00:20:14,400 --> 00:20:18,500
had to subtract out the thermal 
gradient associated with the 

355
00:20:18,500 --> 00:20:21,000
steady state heat flow, that's 
coming up from the mantle to the

356
00:20:21,000 --> 00:20:24,000
surface. 
But whether any other effects 

357
00:20:24,000 --> 00:20:26,400
that you had to account for an 
order to really understand the 

358
00:20:26,408 --> 00:20:28,400
contribution of the earthquake 
to the temperature. 

359
00:20:28,400 --> 00:20:33,700
Normally we didn't know if that 
anomaly was due to fluid flow or

360
00:20:33,700 --> 00:20:37,400
to determine Properties. 
We did lots of measurements on 

361
00:20:37,400 --> 00:20:41,400
those core samples that we got 
to make sure that that anomaly 

362
00:20:41,400 --> 00:20:44,700
that we saw could not be due to 
differences in thermal 

363
00:20:44,700 --> 00:20:46,800
conductivity or other Rock 
property. 

364
00:20:47,100 --> 00:20:51,100
We also looked at the data very 
closely to see is it very 

365
00:20:51,100 --> 00:20:53,500
smooth? 
And does it look like the 

366
00:20:53,500 --> 00:20:57,000
temperature is diffusing, as we 
would expect or are there? 

367
00:20:57,000 --> 00:21:00,500
Lots of signatures of water 
moving through, open faults and 

368
00:21:00,500 --> 00:21:03,600
fractures and in the plate, 
boundary fault itself. 

369
00:21:03,600 --> 00:21:05,800
We did not see any Indications 
of that. 

370
00:21:06,000 --> 00:21:10,300
But we did see water flowing 
through fractures away from the 

371
00:21:10,300 --> 00:21:12,800
main fault and other faults and 
fractures. 

372
00:21:13,100 --> 00:21:16,400
And that gave us a whole other 
insight into earthquake 

373
00:21:16,400 --> 00:21:19,000
mechanics. 
During the nine months that you 

374
00:21:19,000 --> 00:21:21,000
are logging the temperature down
at that bull. 

375
00:21:21,000 --> 00:21:23,300
Whole, did you see this 
temperature? 

376
00:21:23,300 --> 00:21:26,400
Normally start to diffuse away 
through thermal conductivity? 

377
00:21:26,400 --> 00:21:28,900
Did it Peter out. 
It was hard in that time, 

378
00:21:28,900 --> 00:21:31,500
because we were still seeing a 
lot of the effects of the 

379
00:21:31,500 --> 00:21:34,900
drilling disturbance, but 
generally the shape of it, The 

380
00:21:34,900 --> 00:21:38,900
relative stable behavior of It 
Through Time, suggested to us 

381
00:21:38,900 --> 00:21:43,000
that it was a very conductive 
signature just a moment ago. 

382
00:21:43,000 --> 00:21:45,900
You were saying it was actually 
quite significant that you 

383
00:21:45,900 --> 00:21:49,000
managed to pull your whole sense
of string out of the whole 

384
00:21:49,000 --> 00:21:52,600
intact without any of its 
snagging or getting caught. 

385
00:21:53,000 --> 00:21:55,800
I assumed you meant the 
possibility that the whole was 

386
00:21:55,800 --> 00:21:57,600
deformed during those nine 
months. 

387
00:21:57,900 --> 00:22:00,800
The whole could have been shared
across the fault, could have 

388
00:22:00,800 --> 00:22:04,200
still been moving and we didn't 
see that some of the other 

389
00:22:04,200 --> 00:22:06,500
things. 
Is that we measured while we 

390
00:22:06,500 --> 00:22:11,300
were down there before we 
install the observatory was take

391
00:22:11,300 --> 00:22:17,600
the resistivity image 3D 360 
degree image of the walls and we

392
00:22:17,600 --> 00:22:22,600
could see how the tectonic 
stresses were deforming that 

393
00:22:22,600 --> 00:22:26,300
hole after we drilled it. 
So when we drilled it was a 

394
00:22:26,308 --> 00:22:29,600
cylinder but we could see from 
those images that in some 

395
00:22:29,600 --> 00:22:33,400
places, the tectonic stresses 
were forcing it a little bit to 

396
00:22:33,400 --> 00:22:37,100
collapse in certain places. 
Where the hole was becoming more

397
00:22:37,100 --> 00:22:39,600
oval shaped. 
And that told us about the 

398
00:22:39,600 --> 00:22:43,600
magnitude of the stress, has 
down near the fault Beyond. 

399
00:22:43,600 --> 00:22:46,400
Just what we see in the 
temperature, that told us what 

400
00:22:46,800 --> 00:22:48,800
the stresses were during the 
earthquake. 

401
00:22:49,000 --> 00:22:53,000
So after the earthquake, we 
could see that the amount of 

402
00:22:53,100 --> 00:22:56,000
shear stress on the fault, was 
essentially zero. 

403
00:22:56,600 --> 00:23:00,400
So, not only did this fall Sip 
and have no brakes on it, and 

404
00:23:00,400 --> 00:23:03,600
that the stress on the fault, 
went to a value that was very 

405
00:23:03,700 --> 00:23:06,000
small. 
That after the earthquake at 

406
00:23:06,000 --> 00:23:08,700
least in the year afterwards had
not built up a lot of stress, 

407
00:23:08,900 --> 00:23:11,100
that's interesting. 
So the coefficient of friction 

408
00:23:11,100 --> 00:23:15,200
was very low and at the same 
time all the stress was relieved

409
00:23:15,200 --> 00:23:19,700
perhaps because of that in part.
So did you manage to get some 

410
00:23:19,700 --> 00:23:23,400
quantitative results from this 
that you were able to put in 

411
00:23:23,400 --> 00:23:26,800
perspective with the parameters 
that we've observed another 

412
00:23:26,800 --> 00:23:29,800
false around the world? 
Yeah, I guess I jumped ahead of 

413
00:23:29,808 --> 00:23:33,100
myself there and so I told you 
that we saw this point three 

414
00:23:33,400 --> 00:23:36,700
degrees Celsius I'm sure know me
but I didn't tell you what it 

415
00:23:36,700 --> 00:23:42,100
meant and so we could use that 
heat anomaly and the width of it

416
00:23:42,100 --> 00:23:45,600
to constrain and with the 
thermal properties of the Rocks 

417
00:23:45,600 --> 00:23:49,900
down there to constrain how much
heat must have been deposited on

418
00:23:49,900 --> 00:23:53,400
the fault during the earthquake.
And I had said that the fault 

419
00:23:53,400 --> 00:23:57,700
Zone was about two meters thick 
but they're in that two meters. 

420
00:23:57,700 --> 00:24:02,600
Thick, there are lots of 
thousands, tens of thousands of 

421
00:24:02,800 --> 00:24:06,600
little sip surfaces. 
From probably tens of thousands 

422
00:24:06,900 --> 00:24:10,000
of past earthquakes across that 
fault. 

423
00:24:10,600 --> 00:24:15,100
And so each of them are, as thin
as even a few millimeters. 

424
00:24:15,400 --> 00:24:19,800
And so, most of the slip can be 
in a very thin zone, or it could

425
00:24:19,800 --> 00:24:23,200
be distributed across those two 
meters, it's unknown, and it's 

426
00:24:23,200 --> 00:24:26,500
not really that relevant for the
calculation, we do. 

427
00:24:27,200 --> 00:24:30,800
But what we found by figuring 
out how much heat energy was on 

428
00:24:30,800 --> 00:24:33,600
the fault. 
Now, he energy per unit area 

429
00:24:33,800 --> 00:24:37,300
related to the Stress or the 
shear resistance times the 

430
00:24:37,308 --> 00:24:41,000
displacement, we take that 
defied up by 50 meters of slip. 

431
00:24:41,300 --> 00:24:43,900
We get the average Shear 
resistance on the fault. 

432
00:24:44,100 --> 00:24:47,000
We know that the average Shear 
resistance is related to the 

433
00:24:47,000 --> 00:24:50,400
friction coefficient times, the 
normal stress, which is related 

434
00:24:50,400 --> 00:24:53,100
to the weight of the Rocks. 
Calculate the weight of the 

435
00:24:53,100 --> 00:24:56,400
rides based on their density and
we end up with a friction 

436
00:24:56,400 --> 00:24:59,000
coefficient. 
That is point zero eight. 

437
00:24:59,300 --> 00:25:02,100
Which is outrageously small, 
most rocks. 

438
00:25:02,300 --> 00:25:04,500
Have a friction coefficient of 
point 6. 

439
00:25:04,600 --> 00:25:08,200
It's two point, eight. 
So it is told us that the fault 

440
00:25:08,200 --> 00:25:11,700
had no brakes for very little 
resistance to slip. 

441
00:25:11,700 --> 00:25:16,300
Once the rupture got into this 
shallow part, I might we explain

442
00:25:16,500 --> 00:25:18,700
such a very low coefficient of 
friction. 

443
00:25:19,100 --> 00:25:22,700
Those sediments in The Fault 
Zone that are really slippery. 

444
00:25:23,200 --> 00:25:26,700
They already have a low friction
coefficient lot smaller than 

445
00:25:26,700 --> 00:25:30,800
most rocks in general, and 
perhaps a combination of the 

446
00:25:30,800 --> 00:25:34,200
rupture, going through them and 
other effects associated with 

447
00:25:34,200 --> 00:25:38,000
the generic A tree of the fault 
being very shallow, or very 

448
00:25:38,000 --> 00:25:43,200
horizontally dipping together, 
may have allowed the rupture to 

449
00:25:43,200 --> 00:25:48,100
find a week playing in a set of 
diffusing out or rupturing into 

450
00:25:48,100 --> 00:25:51,100
Hard Rock's. 
It affects found this easy 

451
00:25:51,100 --> 00:25:54,800
Pathway to just continue to slip
all the way to the sea floor. 

452
00:25:55,400 --> 00:26:00,500
So, you mentioned clay, I guess 
Clay is a sort of lubricant as 

453
00:26:00,500 --> 00:26:03,500
compared to say other materials 
like more, silica Rich, 

454
00:26:03,500 --> 00:26:06,000
materials that many. 
Any sediments are formed. 

455
00:26:06,000 --> 00:26:07,300
Is that right? 
Yeah. 

456
00:26:07,300 --> 00:26:12,600
In the lab granular, materials 
Sands or crystalline materials, 

457
00:26:12,800 --> 00:26:15,800
have very high friction 
coefficients of REM point six 

458
00:26:16,000 --> 00:26:19,400
point eight, when you put them 
under stress, but Clays are 

459
00:26:19,400 --> 00:26:21,800
interesting. 
Their material structure is 

460
00:26:21,800 --> 00:26:23,700
different in their play D 
minerals. 

461
00:26:24,000 --> 00:26:27,800
They tend to be a bit weaker in 
general and these particular 

462
00:26:27,800 --> 00:26:32,500
Clays are sure smectite clay, 
which is largely Ash, not a lot 

463
00:26:32,500 --> 00:26:36,100
of sediments from River. 
As I said, these are some of the

464
00:26:36,100 --> 00:26:40,500
oldest Oceanic rocks, 130, 
million years old or older, they

465
00:26:40,500 --> 00:26:44,000
are probably deposit out in the 
middle of the ocean, far away 

466
00:26:44,000 --> 00:26:48,200
from any land at such great. 
Depths that all the animal life 

467
00:26:48,200 --> 00:26:51,500
has dissolved when they get to 
these great depths where their 

468
00:26:51,500 --> 00:26:53,700
deposit. 
So, pretty much all this 

469
00:26:53,900 --> 00:26:57,500
material that sediment is ash 
from volcanoes that have gone 

470
00:26:57,500 --> 00:27:00,300
through the atmosphere and found
their way to the bottom of the 

471
00:27:00,300 --> 00:27:04,900
ocean. 
So, ash from volcanoes, Is not 

472
00:27:04,900 --> 00:27:07,900
in itself, necessarily clay-rich
right is what happens. 

473
00:27:07,900 --> 00:27:12,300
Once it goes down at depth, and 
you're below the depth at which 

474
00:27:12,300 --> 00:27:15,100
carbon will read is also no 
carbonates are intact down. 

475
00:27:15,100 --> 00:27:18,200
There, is that what happens? 
That's right, these soft 

476
00:27:18,200 --> 00:27:21,500
particles and Ash when they go 
down and they're exposed to 

477
00:27:21,500 --> 00:27:24,500
water and they can break down 
into these clay minerals. 

478
00:27:24,800 --> 00:27:28,500
So obviously enough Quake, like 
this one has enormous 

479
00:27:28,500 --> 00:27:33,600
destructive potential. 
Do these Studies have practical 

480
00:27:33,600 --> 00:27:37,500
implications? 
For earthquake preparedness or 

481
00:27:37,500 --> 00:27:41,000
maybe even for prospecting for 
economically important minerals 

482
00:27:41,000 --> 00:27:44,300
that are deposited by the kinds 
of transient hydrothermal. 

483
00:27:44,300 --> 00:27:46,900
Fluid flows, that you saw 
further up in the old borehole 

484
00:27:46,900 --> 00:27:51,900
Observatory certainly. 
So we saw that other faults and 

485
00:27:51,900 --> 00:27:57,500
fractures would respond to after
shots pulses of fluid flow 

486
00:27:57,500 --> 00:27:59,900
through them. 
They were opening up. 

487
00:27:59,900 --> 00:28:03,000
And that's a very similar 
process to how we think a lot of

488
00:28:03,300 --> 00:28:05,800
ore minerals. 
Are precipitated. 

489
00:28:06,000 --> 00:28:09,500
That's also another process that
can change. 

490
00:28:09,500 --> 00:28:11,900
The fluid pressure. 
Change the stress State as the 

491
00:28:11,900 --> 00:28:14,800
fluids move through. 
They can redistribute fluid 

492
00:28:14,800 --> 00:28:17,800
pressures, which affects stress 
State, and those changes in, 

493
00:28:17,800 --> 00:28:20,800
stresses can trigger subsequent 
earthquakes. 

494
00:28:21,000 --> 00:28:24,200
So, that tells us a lot about 
the processes that can affect 

495
00:28:24,200 --> 00:28:26,800
aftershocks. 
But just in general, 

496
00:28:26,900 --> 00:28:31,000
understanding something about 
our initial question was the 

497
00:28:31,000 --> 00:28:34,100
shallow part locked in building 
up a lot of stress really 

498
00:28:34,100 --> 00:28:36,600
strong. 
Or it was it really weak and 

499
00:28:36,600 --> 00:28:41,400
just sit along for the ride that
can have direct and important 

500
00:28:41,400 --> 00:28:45,100
implications for earthquake and 
tsunami Hazard preparedness. 

501
00:28:45,500 --> 00:28:48,700
Perhaps one of the more 
analogous parts of the world 

502
00:28:48,700 --> 00:28:51,800
would be the Pacific northwest 
coast of the United States and 

503
00:28:51,800 --> 00:28:56,600
Cascadia where people talk about
a huge earthquake with tsunami 

504
00:28:56,600 --> 00:28:59,500
potential waiting to happen. 
Is that a similar situation? 

505
00:28:59,500 --> 00:29:03,600
There it is a similar situation.
This is a place that also like 

506
00:29:03,600 --> 00:29:06,000
the northern part of Japan. 
Japan has not had a lot of 

507
00:29:06,100 --> 00:29:10,200
earthquakes in modern era. 
People had thought that Cascadia

508
00:29:10,200 --> 00:29:12,800
doesn't have big earthquakes, 
it's just quiet. 

509
00:29:12,800 --> 00:29:15,800
Maybe it's just always gradually
sliding, not building up any 

510
00:29:15,800 --> 00:29:21,000
stress but Native American 
stories and also now, paleo 

511
00:29:21,000 --> 00:29:24,700
seismological records evidence 
in the Rock record of past 

512
00:29:24,700 --> 00:29:28,900
tsunamis that it does have big 
earthquakes, including a 

513
00:29:28,900 --> 00:29:32,700
magnitude 9 earthquake in 
January 1700 there. 

514
00:29:32,700 --> 00:29:34,400
The geology is a little bit 
different. 

515
00:29:34,500 --> 00:29:37,600
But instead of having lots of 
ash and clay, there are a lot of

516
00:29:37,600 --> 00:29:40,400
sediments. 
It's not as easy to drill into 

517
00:29:40,400 --> 00:29:42,400
the fall. 
Although we could perhaps do 

518
00:29:42,400 --> 00:29:45,600
some follow-up survey shins to 
learn more about the seismic 

519
00:29:45,600 --> 00:29:48,900
potential there as well. 
Patrick Fulton. 

520
00:29:49,000 --> 00:29:53,000
Thank you very much. 
Thank you for more about geology

521
00:29:53,000 --> 00:29:57,000
b, as well as pictures and 
illustrations, that support this

522
00:29:57,000 --> 00:29:59,600
podcast, go to geology B.com.
