WEBVTT 0df04eda-27ac-4d75-8cb3-253f98d67727/326-0 00:00:11.150 --> 00:00:14.203 I'll pass the mic to Tamara Jeppson who will introduce today's speaker Sara Beth Cebry. Sarah Beth joined us in June, starting as a Mendenhall 0df04eda-27ac-4d75-8cb3-253f98d67727/326-1 00:00:14.203 --> 00:00:17.534 postdoc. Did her undergraduate work in civil engineering at 0df04eda-27ac-4d75-8cb3-253f98d67727/326-2 00:00:17.534 --> 00:00:20.753 Worcester Polytechnic Institute, and she went on to be an 0df04eda-27ac-4d75-8cb3-253f98d67727/326-3 00:00:20.753 --> 00:00:23.918 engineer for a couple of years, working on designing and 0df04eda-27ac-4d75-8cb3-253f98d67727/326-4 00:00:23.918 --> 00:00:27.193 analyzing structural aspects of government projects before 0df04eda-27ac-4d75-8cb3-253f98d67727/326-5 00:00:27.193 --> 00:00:28.470 deciding to pursue her 0df04eda-27ac-4d75-8cb3-253f98d67727/336-0 00:00:28.470 --> 00:00:30.710 Graduate degree at Cornell University. 0df04eda-27ac-4d75-8cb3-253f98d67727/354-0 00:00:31.270 --> 00:00:34.003 and her PhD with Greg McCloskey, a former Mendenhall post doc 0df04eda-27ac-4d75-8cb3-253f98d67727/354-1 00:00:34.003 --> 00:00:36.693 here that many of you may know, worked at the Rock Mechanics 0df04eda-27ac-4d75-8cb3-253f98d67727/354-2 00:00:36.693 --> 00:00:36.870 Lab. 0df04eda-27ac-4d75-8cb3-253f98d67727/362-0 00:00:37.760 --> 00:00:40.640 And there she worked with his large-scale laboratory fault 0df04eda-27ac-4d75-8cb3-253f98d67727/362-1 00:00:40.640 --> 00:00:41.080 geometry. 0df04eda-27ac-4d75-8cb3-253f98d67727/404-0 00:00:42.800 --> 00:00:45.887 His large scale laboratory apparatus to examine linkages 0df04eda-27ac-4d75-8cb3-253f98d67727/404-1 00:00:45.887 --> 00:00:49.190 between stress heterogeneity is caused by fluid geometry are 0df04eda-27ac-4d75-8cb3-253f98d67727/404-2 00:00:49.190 --> 00:00:52.548 fluid injection, and the links between those rupture behavior 0df04eda-27ac-4d75-8cb3-253f98d67727/404-3 00:00:52.548 --> 00:00:55.797 and I think should be talking about some of that today with 0df04eda-27ac-4d75-8cb3-253f98d67727/404-4 00:00:55.797 --> 00:00:55.960 us. 0df04eda-27ac-4d75-8cb3-253f98d67727/415-0 00:00:55.960 --> 00:01:00.091 So she's really become an expert in using large experimental 0df04eda-27ac-4d75-8cb3-253f98d67727/415-1 00:01:00.091 --> 00:01:02.800 apparatus to study earthquake behavior. 0df04eda-27ac-4d75-8cb3-253f98d67727/433-0 00:01:03.280 --> 00:01:06.425 We managed to draw her over here to the West Coast to work here 0df04eda-27ac-4d75-8cb3-253f98d67727/433-1 00:01:06.425 --> 00:01:09.080 on the 2M by Axel apparatus in the lab that we have, 0df04eda-27ac-4d75-8cb3-253f98d67727/438-0 00:01:09.880 --> 00:01:11.240 which is currently still in pieces. 0df04eda-27ac-4d75-8cb3-253f98d67727/458-0 00:01:12.220 --> 00:01:15.329 She's very nice to jump. in to starting to get that set up 0df04eda-27ac-4d75-8cb3-253f98d67727/458-1 00:01:15.329 --> 00:01:18.650 again, as well as working with the induced seismicity, looking 0df04eda-27ac-4d75-8cb3-253f98d67727/458-2 00:01:18.650 --> 00:01:21.180 at identifying repeating earthquakes in Kansas. 0df04eda-27ac-4d75-8cb3-253f98d67727/481-0 00:01:22.760 --> 00:01:25.831 So that worked with the laboratory work that she'll be 0df04eda-27ac-4d75-8cb3-253f98d67727/481-1 00:01:25.831 --> 00:01:29.237 doing here to better understand links between laboratory and 0df04eda-27ac-4d75-8cb3-253f98d67727/481-2 00:01:29.237 --> 00:01:32.699 field scale observations of the physical processes that drive 0df04eda-27ac-4d75-8cb3-253f98d67727/481-3 00:01:32.699 --> 00:01:33.760 induced seismicity. 0df04eda-27ac-4d75-8cb3-253f98d67727/484-0 00:01:39.690 --> 00:01:40.210 Thank you. 0df04eda-27ac-4d75-8cb3-253f98d67727/487-0 00:01:45.300 --> 00:01:45.660 Set up. 0df04eda-27ac-4d75-8cb3-253f98d67727/489-0 00:01:50.170 --> 00:01:50.330 OK. 0df04eda-27ac-4d75-8cb3-253f98d67727/495-0 00:01:51.180 --> 00:01:52.940 So thank you for the introduction. 0df04eda-27ac-4d75-8cb3-253f98d67727/507-0 00:01:55.590 --> 00:01:58.683 I'm Sarah Beth seabury. And today I'm going to be talking 0df04eda-27ac-4d75-8cb3-253f98d67727/507-1 00:01:58.683 --> 00:01:59.270 about work. 0df04eda-27ac-4d75-8cb3-253f98d67727/520-0 00:01:59.310 --> 00:02:02.566 Most most it's primarily going to be work that I did during my 0df04eda-27ac-4d75-8cb3-253f98d67727/520-1 00:02:02.566 --> 00:02:03.910 PhD at Cornell University. 0df04eda-27ac-4d75-8cb3-253f98d67727/529-0 00:02:05.440 --> 00:02:07.320 And then just a little bit on what I'm going to do here. 0df04eda-27ac-4d75-8cb3-253f98d67727/531-0 00:02:09.040 --> 00:02:09.120 So. 0df04eda-27ac-4d75-8cb3-253f98d67727/542-0 00:02:10.160 --> 00:02:13.507 I still think I need to really explain to anyone here that 0df04eda-27ac-4d75-8cb3-253f98d67727/542-1 00:02:13.507 --> 00:02:15.720 induce seismicity is a problem, right? 0df04eda-27ac-4d75-8cb3-253f98d67727/562-0 00:02:15.720 --> 00:02:18.761 So we know that human activity can create earthquakes either 0df04eda-27ac-4d75-8cb3-253f98d67727/562-1 00:02:18.761 --> 00:02:21.952 through wastewater disposal, oil and gas operations or enhanced 0df04eda-27ac-4d75-8cb3-253f98d67727/562-2 00:02:21.952 --> 00:02:22.800 geothermal wells. 0df04eda-27ac-4d75-8cb3-253f98d67727/605-0 00:02:24.360 --> 00:02:28.804 And so this has been responsible for like an order of magnitude 0df04eda-27ac-4d75-8cb3-253f98d67727/605-1 00:02:28.804 --> 00:02:33.040 increase in seismicity in the US, Oklahoma and Texas. And so 0df04eda-27ac-4d75-8cb3-253f98d67727/605-2 00:02:33.040 --> 00:02:37.485 one of the ways that this occurs is via direct fluid injection, 0df04eda-27ac-4d75-8cb3-253f98d67727/605-3 00:02:37.485 --> 00:02:39.360 where water is directed or. 0df04eda-27ac-4d75-8cb3-253f98d67727/624-0 00:02:40.150 --> 00:02:43.301 Injected directly onto a fault interface, and so when I talk 0df04eda-27ac-4d75-8cb3-253f98d67727/624-1 00:02:43.301 --> 00:02:46.503 about fluid injection, this is what I'm thinking about in the 0df04eda-27ac-4d75-8cb3-253f98d67727/624-2 00:02:46.503 --> 00:02:46.710 lab. 0df04eda-27ac-4d75-8cb3-253f98d67727/646-0 00:02:48.220 --> 00:02:50.944 They're kind of so despite our observations of induced 0df04eda-27ac-4d75-8cb3-253f98d67727/646-1 00:02:50.944 --> 00:02:53.817 seismicity, there are kind of two mechanisms, like really 0df04eda-27ac-4d75-8cb3-253f98d67727/646-2 00:02:53.817 --> 00:02:55.700 basic mechanisms that come into play. 0df04eda-27ac-4d75-8cb3-253f98d67727/656-0 00:02:56.340 --> 00:02:58.820 The first one is the effective stress value or like a Coulomb 0df04eda-27ac-4d75-8cb3-253f98d67727/656-1 00:02:58.820 --> 00:02:59.300 failure law. 0df04eda-27ac-4d75-8cb3-253f98d67727/679-0 00:02:59.870 --> 00:03:03.483 Where you have some normal stress on the fault and some 0df04eda-27ac-4d75-8cb3-253f98d67727/679-1 00:03:03.483 --> 00:03:07.031 shear stress, and when you increase fluid pressure you 0df04eda-27ac-4d75-8cb3-253f98d67727/679-2 00:03:07.031 --> 00:03:11.031 decrease the effective normal stress and that can cause fault 0df04eda-27ac-4d75-8cb3-253f98d67727/679-3 00:03:11.031 --> 00:03:11.870 reactivation. 0df04eda-27ac-4d75-8cb3-253f98d67727/690-0 00:03:14.040 --> 00:03:16.480 So this governs when a fault is going to slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/704-0 00:03:16.480 --> 00:03:20.297 So this governs when the fault goes from locked to starting to 0df04eda-27ac-4d75-8cb3-253f98d67727/704-1 00:03:20.297 --> 00:03:20.600 slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/730-0 00:03:22.030 --> 00:03:25.416 But it doesn't control how the fault will slip, whether it's 0df04eda-27ac-4d75-8cb3-253f98d67727/730-1 00:03:25.416 --> 00:03:28.746 gonna stay asymic or whether it throws into a large seismic 0df04eda-27ac-4d75-8cb3-253f98d67727/730-2 00:03:28.746 --> 00:03:30.190 event that produces waves. 0df04eda-27ac-4d75-8cb3-253f98d67727/732-0 00:03:33.000 --> 00:03:33.640 Controlled bias. 0df04eda-27ac-4d75-8cb3-253f98d67727/741-0 00:03:33.640 --> 00:03:36.080 What we think of, it's like a critical nucleation length. 0df04eda-27ac-4d75-8cb3-253f98d67727/752-0 00:03:36.760 --> 00:03:40.085 So here if we have distance along the fault and time and 0df04eda-27ac-4d75-8cb3-253f98d67727/752-1 00:03:40.085 --> 00:03:42.360 these are just like snapshots in time. 0df04eda-27ac-4d75-8cb3-253f98d67727/758-0 00:03:44.460 --> 00:03:45.940 Part of the fault starts to slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/776-0 00:03:46.950 --> 00:03:50.774 That slipping patch grows and grows and grows until it hits a 0df04eda-27ac-4d75-8cb3-253f98d67727/776-1 00:03:50.774 --> 00:03:53.550 critical point, which we refer to as H star. 0df04eda-27ac-4d75-8cb3-253f98d67727/783-0 00:03:53.550 --> 00:03:57.030 But it's the critical nucleation length, also known as L sub C. 0df04eda-27ac-4d75-8cb3-253f98d67727/803-0 00:03:59.240 --> 00:04:02.040 And when it hits that critical point, that's when the slipping 0df04eda-27ac-4d75-8cb3-253f98d67727/803-1 00:04:02.040 --> 00:04:03.240 patch starts to accelerate. 0df04eda-27ac-4d75-8cb3-253f98d67727/806-0 00:04:03.240 --> 00:04:06.600 Radiate seismic waves and you get a earthquake. 0df04eda-27ac-4d75-8cb3-253f98d67727/819-0 00:04:08.690 --> 00:04:11.174 But one thing to note about this is that it's inversely 0df04eda-27ac-4d75-8cb3-253f98d67727/819-1 00:04:11.174 --> 00:04:13.170 proportional to the effective normal stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/829-0 00:04:13.650 --> 00:04:17.315 So in theory, as you inject water, you lower that effective 0df04eda-27ac-4d75-8cb3-253f98d67727/829-1 00:04:17.315 --> 00:04:18.170 normal stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/844-0 00:04:18.370 --> 00:04:22.179 It should promote a seismic slip, so it should not promote 0df04eda-27ac-4d75-8cb3-253f98d67727/844-1 00:04:22.179 --> 00:04:22.890 seismicity. 0df04eda-27ac-4d75-8cb3-253f98d67727/854-0 00:04:23.810 --> 00:04:26.973 But that's obviously doesn't agree with the fact that we see 0df04eda-27ac-4d75-8cb3-253f98d67727/854-1 00:04:26.973 --> 00:04:28.010 induced earthquakes. 0df04eda-27ac-4d75-8cb3-253f98d67727/861-0 00:04:30.210 --> 00:04:32.250 So a lot of the questions kind of come out. 0df04eda-27ac-4d75-8cb3-253f98d67727/865-0 00:04:32.250 --> 00:04:34.290 How does this like? 0df04eda-27ac-4d75-8cb3-253f98d67727/875-0 00:04:34.290 --> 00:04:37.210 How do these two kind of fit together with our observations? 0df04eda-27ac-4d75-8cb3-253f98d67727/882-0 00:04:38.760 --> 00:04:41.480 So there have been kind of like one of the common thoughts. 0df04eda-27ac-4d75-8cb3-253f98d67727/897-0 00:04:43.640 --> 00:04:46.301 And I use this kind of figure over here because I think they 0df04eda-27ac-4d75-8cb3-253f98d67727/897-1 00:04:46.301 --> 00:04:47.480 have a really nice cartoon. 0df04eda-27ac-4d75-8cb3-253f98d67727/904-0 00:04:49.200 --> 00:04:53.640 Where you have fluid pressure injecting onto a fault plane. 0df04eda-27ac-4d75-8cb3-253f98d67727/915-0 00:04:55.850 --> 00:04:58.777 Food pressure increases at the center of the fault and starts 0df04eda-27ac-4d75-8cb3-253f98d67727/915-1 00:04:58.777 --> 00:04:59.250 to spread. 0df04eda-27ac-4d75-8cb3-253f98d67727/938-0 00:05:00.800 --> 00:05:04.539 And so that you get your a seismic slip in this kind of 0df04eda-27ac-4d75-8cb3-253f98d67727/938-1 00:05:04.539 --> 00:05:08.680 blue region up here. And then as that a seismic slip happens. 0df04eda-27ac-4d75-8cb3-253f98d67727/957-0 00:05:10.320 --> 00:05:13.426 That's decreasing the critical nucleation length in the 0df04eda-27ac-4d75-8cb3-253f98d67727/957-1 00:05:13.426 --> 00:05:16.644 slipping patch, but outside of it you're increasing shear 0df04eda-27ac-4d75-8cb3-253f98d67727/957-2 00:05:16.644 --> 00:05:17.920 stress from the effect. 0df04eda-27ac-4d75-8cb3-253f98d67727/965-0 00:05:22.950 --> 00:05:24.590 And that is what produces earthquakes. 0df04eda-27ac-4d75-8cb3-253f98d67727/988-0 00:05:24.590 --> 00:05:28.051 So you get a ring of fluid injection, a ring of decreased 0df04eda-27ac-4d75-8cb3-253f98d67727/988-1 00:05:28.051 --> 00:05:31.752 effective normal stress with kind of micro seismicity outside 0df04eda-27ac-4d75-8cb3-253f98d67727/988-2 00:05:31.752 --> 00:05:32.110 of it. 0df04eda-27ac-4d75-8cb3-253f98d67727/1000-0 00:05:34.950 --> 00:05:37.670 Showing this Kappa one but there are lots of other studies. 0df04eda-27ac-4d75-8cb3-253f98d67727/1007-0 00:05:40.000 --> 00:05:42.400 That also support these observations. 0df04eda-27ac-4d75-8cb3-253f98d67727/1021-0 00:05:45.570 --> 00:05:48.970 This is an. This is a good kind of way to think about things, 0df04eda-27ac-4d75-8cb3-253f98d67727/1021-1 00:05:48.970 --> 00:05:50.890 but it leaves some open questions. 0df04eda-27ac-4d75-8cb3-253f98d67727/1031-0 00:05:50.890 --> 00:05:53.770 For example, how do we get large induced seismicity? 0df04eda-27ac-4d75-8cb3-253f98d67727/1043-0 00:05:53.770 --> 00:05:58.330 So we get this micro seismicity so events can start around here. 0df04eda-27ac-4d75-8cb3-253f98d67727/1051-0 00:05:58.530 --> 00:06:00.890 But what kind of controls when they stops? 0df04eda-27ac-4d75-8cb3-253f98d67727/1083-0 00:06:00.890 --> 00:06:04.983 Or how big they are going to get. It also brings up questions 0df04eda-27ac-4d75-8cb3-253f98d67727/1083-1 00:06:04.983 --> 00:06:09.142 like how far can this a seismic slip increase the shear stress 0df04eda-27ac-4d75-8cb3-253f98d67727/1083-2 00:06:09.142 --> 00:06:13.235 beyond? And so how far can the seismicity propagate away from 0df04eda-27ac-4d75-8cb3-253f98d67727/1083-3 00:06:13.235 --> 00:06:14.490 the injection well? 0df04eda-27ac-4d75-8cb3-253f98d67727/1088-0 00:06:15.800 --> 00:06:17.120 Among some other questions. 0df04eda-27ac-4d75-8cb3-253f98d67727/1093-0 00:06:18.920 --> 00:06:21.560 And so a lot of work has been done and. 0df04eda-27ac-4d75-8cb3-253f98d67727/1096-0 00:06:22.190 --> 00:06:22.910 These are these are. 0df04eda-27ac-4d75-8cb3-253f98d67727/1104-0 00:06:24.270 --> 00:06:27.990 Some are based on experimental work or in situ experiments. 0df04eda-27ac-4d75-8cb3-253f98d67727/1131-0 00:06:29.900 --> 00:06:33.397 So a lot of work has been done kind of on the non modeling 0df04eda-27ac-4d75-8cb3-253f98d67727/1131-1 00:06:33.397 --> 00:06:37.250 side. And so this is how I think about things, how I like, group 0df04eda-27ac-4d75-8cb3-253f98d67727/1131-2 00:06:37.250 --> 00:06:40.511 everything together into different scales. So on the Y 0df04eda-27ac-4d75-8cb3-253f98d67727/1131-3 00:06:40.511 --> 00:06:43.060 axis, we have temperature pressure, right. 0df04eda-27ac-4d75-8cb3-253f98d67727/1137-0 00:06:43.060 --> 00:06:45.460 So as you go up higher, you get deeper earthquakes. 0df04eda-27ac-4d75-8cb3-253f98d67727/1170-0 00:06:47.040 --> 00:06:50.594 Down here you have more shallow earthquakes and then on the X 0df04eda-27ac-4d75-8cb3-253f98d67727/1170-1 00:06:50.594 --> 00:06:54.206 axis we have fault size and I'm putting it all relative to the 0df04eda-27ac-4d75-8cb3-253f98d67727/1170-2 00:06:54.206 --> 00:06:57.589 critical nucleation length to account for things like rock 0df04eda-27ac-4d75-8cb3-253f98d67727/1170-3 00:06:57.589 --> 00:06:59.080 analog and such like that. 0df04eda-27ac-4d75-8cb3-253f98d67727/1173-0 00:07:00.760 --> 00:07:01.360 But so. 0df04eda-27ac-4d75-8cb3-253f98d67727/1183-0 00:07:02.630 --> 00:07:07.653 Have large events or sorry large natural faults versus small 0df04eda-27ac-4d75-8cb3-253f98d67727/1183-1 00:07:07.653 --> 00:07:08.230 faults. 0df04eda-27ac-4d75-8cb3-253f98d67727/1187-0 00:07:09.760 --> 00:07:10.240 So in the like. 0df04eda-27ac-4d75-8cb3-253f98d67727/1207-0 00:07:11.230 --> 00:07:14.518 Here in the high pressure small fault, we get things like the 0df04eda-27ac-4d75-8cb3-253f98d67727/1207-1 00:07:14.518 --> 00:07:17.965 Tri axial apparatus here, like a lot of the work that Tamara and 0df04eda-27ac-4d75-8cb3-253f98d67727/1207-2 00:07:17.965 --> 00:07:18.390 Dave do. 0df04eda-27ac-4d75-8cb3-253f98d67727/1231-0 00:07:20.000 --> 00:07:23.000 Down here we get lower temperature, smaller faults like 0df04eda-27ac-4d75-8cb3-253f98d67727/1231-1 00:07:23.000 --> 00:07:26.000 the biaxial apparatus that Brian does a lot of work on. 0df04eda-27ac-4d75-8cb3-253f98d67727/1256-0 00:07:27.720 --> 00:07:30.672 And then we get this large scale experiments that can't go to 0df04eda-27ac-4d75-8cb3-253f98d67727/1256-1 00:07:30.672 --> 00:07:33.720 high temperatures or pressures, but you can get a larger fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1259-0 00:07:34.840 --> 00:07:36.600 And so that's more like a shallow fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1266-0 00:07:38.280 --> 00:07:38.720 You also have. 0df04eda-27ac-4d75-8cb3-253f98d67727/1271-0 00:07:38.720 --> 00:07:41.800 For induced seismicity, we have some insitu experiments where. 0df04eda-27ac-4d75-8cb3-253f98d67727/1295-0 00:07:42.340 --> 00:07:46.393 Basically like they drill a hole a kilometer and a half under a 0df04eda-27ac-4d75-8cb3-253f98d67727/1295-1 00:07:46.393 --> 00:07:50.130 mountain and then inject water and measure some seismicity 0df04eda-27ac-4d75-8cb3-253f98d67727/1295-2 00:07:50.130 --> 00:07:51.460 which is pretty cool. 0df04eda-27ac-4d75-8cb3-253f98d67727/1301-0 00:07:53.840 --> 00:07:55.680 And then we have natural faults. 0df04eda-27ac-4d75-8cb3-253f98d67727/1313-0 00:07:58.270 --> 00:08:00.870 Which are much larger and can exist at accurate. 0df04eda-27ac-4d75-8cb3-253f98d67727/1320-0 00:08:01.090 --> 00:08:03.370 Like, obviously they're they're natural faults. 0df04eda-27ac-4d75-8cb3-253f98d67727/1326-0 00:08:03.370 --> 00:08:05.353 That's the right temperature and pressure where things are 0df04eda-27ac-4d75-8cb3-253f98d67727/1326-1 00:08:05.353 --> 00:08:05.690 happening. 0df04eda-27ac-4d75-8cb3-253f98d67727/1338-0 00:08:07.780 --> 00:08:11.140 And so this might be a repeat for a lot of you lab folks. 0df04eda-27ac-4d75-8cb3-253f98d67727/1361-0 00:08:11.140 --> 00:08:15.050 But so there is a reason I separate small scale and large 0df04eda-27ac-4d75-8cb3-253f98d67727/1361-1 00:08:15.050 --> 00:08:18.758 scale lab experiments bias because I work on the large 0df04eda-27ac-4d75-8cb3-253f98d67727/1361-2 00:08:18.758 --> 00:08:19.500 scale side. 0df04eda-27ac-4d75-8cb3-253f98d67727/1379-0 00:08:21.070 --> 00:08:24.612 But we have centimeter size samples, so yay big and then we 0df04eda-27ac-4d75-8cb3-253f98d67727/1379-1 00:08:24.612 --> 00:08:26.030 have meter size samples. 0df04eda-27ac-4d75-8cb3-253f98d67727/1385-0 00:08:26.030 --> 00:08:29.430 So here's an here's a picture of Brian case. 0df04eda-27ac-4d75-8cb3-253f98d67727/1389-0 00:08:29.430 --> 00:08:31.870 You curious from a long time ago? 0df04eda-27ac-4d75-8cb3-253f98d67727/1401-0 00:08:31.870 --> 00:08:35.652 I think it's a fun picture like working with like. That's the 0df04eda-27ac-4d75-8cb3-253f98d67727/1401-1 00:08:35.652 --> 00:08:36.750 size of the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1403-0 00:08:36.750 --> 00:08:38.590 That's the fault surface right there. 0df04eda-27ac-4d75-8cb3-253f98d67727/1433-0 00:08:40.780 --> 00:08:44.388 So these small centimeter scale faults, so we can go up to high 0df04eda-27ac-4d75-8cb3-253f98d67727/1433-1 00:08:44.388 --> 00:08:47.658 temperatures and pressures, which is really cool. But you 0df04eda-27ac-4d75-8cb3-253f98d67727/1433-2 00:08:47.658 --> 00:08:50.703 the sample is treated as a point. So it's just like a 0df04eda-27ac-4d75-8cb3-253f98d67727/1433-3 00:08:50.703 --> 00:08:52.620 single point on the entire fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1474-0 00:08:53.020 --> 00:08:56.199 And then if you want to figure out the behavior of real 0df04eda-27ac-4d75-8cb3-253f98d67727/1474-1 00:08:56.199 --> 00:08:59.776 earthquakes, you take and put that into numerical simulations, 0df04eda-27ac-4d75-8cb3-253f98d67727/1474-2 00:08:59.776 --> 00:09:03.070 and then you can expand from there. On the flip side, the 0df04eda-27ac-4d75-8cb3-253f98d67727/1474-3 00:09:03.070 --> 00:09:06.249 meter scales samples. You can start to see interactions 0df04eda-27ac-4d75-8cb3-253f98d67727/1474-4 00:09:06.249 --> 00:09:08.180 between different fault sections. 0df04eda-27ac-4d75-8cb3-253f98d67727/1478-0 00:09:08.180 --> 00:09:10.100 So the sample is behaving like a continuum. 0df04eda-27ac-4d75-8cb3-253f98d67727/1507-0 00:09:10.850 --> 00:09:14.846 Where you can have one part slipping and another part still 0df04eda-27ac-4d75-8cb3-253f98d67727/1507-1 00:09:14.846 --> 00:09:18.775 remains locked, and so this these meter sized samples in a 0df04eda-27ac-4d75-8cb3-253f98d67727/1507-2 00:09:18.775 --> 00:09:22.904 good place to look at kind of this get a better understanding 0df04eda-27ac-4d75-8cb3-253f98d67727/1507-3 00:09:22.904 --> 00:09:24.370 of this understanding. 0df04eda-27ac-4d75-8cb3-253f98d67727/1530-0 00:09:26.150 --> 00:09:29.559 Of how induced seismicity works, where you have a region of fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/1530-1 00:09:29.559 --> 00:09:32.296 pressure and a region of seismicity, and then locked 0df04eda-27ac-4d75-8cb3-253f98d67727/1530-2 00:09:32.296 --> 00:09:32.710 regions. 0df04eda-27ac-4d75-8cb3-253f98d67727/1547-0 00:09:35.160 --> 00:09:40.075 So specifically the meter scale faults I work on are at Cornell 0df04eda-27ac-4d75-8cb3-253f98d67727/1547-1 00:09:40.075 --> 00:09:40.920 University. 0df04eda-27ac-4d75-8cb3-253f98d67727/1552-0 00:09:40.960 --> 00:09:42.800 Yeah, I did my PhD in a pandemic. 0df04eda-27ac-4d75-8cb3-253f98d67727/1553-0 00:09:42.800 --> 00:09:43.320 It was fun. 0df04eda-27ac-4d75-8cb3-253f98d67727/1581-0 00:09:44.990 --> 00:09:48.680 And so these are just kind of to give you a sense of the scale. 0df04eda-27ac-4d75-8cb3-253f98d67727/1581-1 00:09:48.680 --> 00:09:51.909 This is a three quarter meter fault and then that's the 0df04eda-27ac-4d75-8cb3-253f98d67727/1581-2 00:09:51.909 --> 00:09:53.870 further one is a 3M granite fall. 0df04eda-27ac-4d75-8cb3-253f98d67727/1594-0 00:09:56.130 --> 00:09:59.810 And by using Plexiglas for the smaller fault, we end up again. 0df04eda-27ac-4d75-8cb3-253f98d67727/1599-0 00:09:59.810 --> 00:10:02.690 I'm putting everything in terms of L / H star. 0df04eda-27ac-4d75-8cb3-253f98d67727/1602-0 00:10:04.230 --> 00:10:05.710 Ling for analog materials. 0df04eda-27ac-4d75-8cb3-253f98d67727/1646-0 00:10:07.390 --> 00:10:10.462 Both cases, the entire length of the fall is larger than the 0df04eda-27ac-4d75-8cb3-253f98d67727/1646-1 00:10:10.462 --> 00:10:13.332 critical nucleation length, which means that you can get 0df04eda-27ac-4d75-8cb3-253f98d67727/1646-2 00:10:13.332 --> 00:10:16.001 event that starts and propagates, and in these cases 0df04eda-27ac-4d75-8cb3-253f98d67727/1646-3 00:10:16.001 --> 00:10:19.123 the sample is long enough that it'll terminate all within the 0df04eda-27ac-4d75-8cb3-253f98d67727/1646-4 00:10:19.123 --> 00:10:21.390 sample, and so we can observe each of those. 0df04eda-27ac-4d75-8cb3-253f98d67727/1648-0 00:10:21.630 --> 00:10:22.030 Different. 0df04eda-27ac-4d75-8cb3-253f98d67727/1650-0 00:10:23.790 --> 00:10:24.070 Steps. 0df04eda-27ac-4d75-8cb3-253f98d67727/1656-0 00:10:26.500 --> 00:10:28.580 Way these McCluskey styles. 0df04eda-27ac-4d75-8cb3-253f98d67727/1690-0 00:10:28.580 --> 00:10:31.394 Just kind of what I'm gonna generally term them by axial 0df04eda-27ac-4d75-8cb3-253f98d67727/1690-1 00:10:31.394 --> 00:10:34.505 loading's work is there are two blocks two rectangular blocks, 0df04eda-27ac-4d75-8cb3-253f98d67727/1690-2 00:10:34.505 --> 00:10:37.566 one up here that we'll refer to as the moving block. And then 0df04eda-27ac-4d75-8cb3-253f98d67727/1690-3 00:10:37.566 --> 00:10:40.232 this bottom one is the stationary block and it's kind 0df04eda-27ac-4d75-8cb3-253f98d67727/1690-4 00:10:40.232 --> 00:10:41.220 of held in place on. 0df04eda-27ac-4d75-8cb3-253f98d67727/1692-0 00:10:41.220 --> 00:10:41.700 Two sides. 0df04eda-27ac-4d75-8cb3-253f98d67727/1707-0 00:10:43.690 --> 00:10:46.589 In all of the samples that I'm going to talk about, there's an 0df04eda-27ac-4d75-8cb3-253f98d67727/1707-1 00:10:46.589 --> 00:10:47.050 injection. 0df04eda-27ac-4d75-8cb3-253f98d67727/1713-0 00:10:47.050 --> 00:10:47.610 Well drilled. 0df04eda-27ac-4d75-8cb3-253f98d67727/1723-0 00:10:47.610 --> 00:10:50.740 So if we're not looking into the fault, we're looking at it 0df04eda-27ac-4d75-8cb3-253f98d67727/1723-1 00:10:50.740 --> 00:10:51.210 sideways. 0df04eda-27ac-4d75-8cb3-253f98d67727/1741-0 00:10:51.610 --> 00:10:54.819 So here's your fault interface. We have some sensors up here and 0df04eda-27ac-4d75-8cb3-253f98d67727/1741-1 00:10:54.819 --> 00:10:57.930 then we have a hole that water can go directly onto the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1745-0 00:10:59.690 --> 00:11:01.090 So in each experiment. 0df04eda-27ac-4d75-8cb3-253f98d67727/1764-0 00:11:02.790 --> 00:11:05.606 We do side just push the two blocks together so the moving in 0df04eda-27ac-4d75-8cb3-253f98d67727/1764-1 00:11:05.606 --> 00:11:08.605 the stationary block and then we hold that normal stress constant 0df04eda-27ac-4d75-8cb3-253f98d67727/1764-2 00:11:08.605 --> 00:11:10.150 throughout the entire experiment. 0df04eda-27ac-4d75-8cb3-253f98d67727/1771-0 00:11:12.540 --> 00:11:14.940 Increase sheer stress on the moving block. 0df04eda-27ac-4d75-8cb3-253f98d67727/1778-0 00:11:16.510 --> 00:11:18.470 So we add some stress on it that way. 0df04eda-27ac-4d75-8cb3-253f98d67727/1783-0 00:11:20.880 --> 00:11:22.240 Directly onto the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1785-0 00:11:23.950 --> 00:11:24.270 Their fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1790-0 00:11:24.390 --> 00:11:26.310 Their fault that moving block to slip forward. 0df04eda-27ac-4d75-8cb3-253f98d67727/1805-0 00:11:29.150 --> 00:11:32.738 And so and in these experiments, water is allowed to diffuse 0df04eda-27ac-4d75-8cb3-253f98d67727/1805-1 00:11:32.738 --> 00:11:33.150 freely. 0df04eda-27ac-4d75-8cb3-253f98d67727/1810-0 00:11:34.150 --> 00:11:35.950 So I'm gonna kind of go through some typical results. 0df04eda-27ac-4d75-8cb3-253f98d67727/1831-0 00:11:38.430 --> 00:11:41.624 To understand where the fluid pressure is along the fault, I 0df04eda-27ac-4d75-8cb3-253f98d67727/1831-1 00:11:41.624 --> 00:11:44.190 created like a really simple 2D diffusion model. 0df04eda-27ac-4d75-8cb3-253f98d67727/1842-0 00:11:44.870 --> 00:11:48.139 And so this is the fault interface. So we're pushing on 0df04eda-27ac-4d75-8cb3-253f98d67727/1842-1 00:11:48.139 --> 00:11:49.190 it from over here. 0df04eda-27ac-4d75-8cb3-253f98d67727/1844-0 00:11:49.630 --> 00:11:50.790 This is along the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1884-0 00:11:52.350 --> 00:11:56.093 Lines we're injecting at a single point, so injecting the 0df04eda-27ac-4d75-8cb3-253f98d67727/1884-1 00:11:56.093 --> 00:12:00.288 water and allowing it to diffuse freely creates a region of over 0df04eda-27ac-4d75-8cb3-253f98d67727/1884-2 00:12:00.288 --> 00:12:04.483 pressure at the injection point and then outside of that we have 0df04eda-27ac-4d75-8cb3-253f98d67727/1884-3 00:12:04.483 --> 00:12:07.710 a region that's unaffected by the fluid pressure. 0df04eda-27ac-4d75-8cb3-253f98d67727/1893-0 00:12:09.110 --> 00:12:11.230 Because it's a granite granite fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/1914-0 00:12:11.870 --> 00:12:16.030 The fault diffusivity is very low, and so even if 500 seconds 0df04eda-27ac-4d75-8cb3-253f98d67727/1914-1 00:12:16.030 --> 00:12:19.988 the fluid pressure has only reached a portion of the fault 0df04eda-27ac-4d75-8cb3-253f98d67727/1914-2 00:12:19.988 --> 00:12:20.190 so. 0df04eda-27ac-4d75-8cb3-253f98d67727/1922-0 00:12:21.750 --> 00:12:23.910 We're able to see these fault interactions. 0df04eda-27ac-4d75-8cb3-253f98d67727/1943-0 00:12:26.470 --> 00:12:30.498 Are some typical results what I'm showing here is a stick slip 0df04eda-27ac-4d75-8cb3-253f98d67727/1943-1 00:12:30.498 --> 00:12:34.207 event that has created just by pushing just by externally 0df04eda-27ac-4d75-8cb3-253f98d67727/1943-2 00:12:34.207 --> 00:12:35.550 applied shear stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/1983-0 00:12:35.550 --> 00:12:39.734 So this is more like a normal non fluid triggered event and 0df04eda-27ac-4d75-8cb3-253f98d67727/1983-1 00:12:39.734 --> 00:12:43.988 the way we're gonna interpret this graph. So we have time on 0df04eda-27ac-4d75-8cb3-253f98d67727/1983-2 00:12:43.988 --> 00:12:48.520 the X axis, displacement on the Y axis, and then we have a bunch 0df04eda-27ac-4d75-8cb3-253f98d67727/1983-3 00:12:48.520 --> 00:12:51.310 of slip sensors and I color-coded them. 0df04eda-27ac-4d75-8cb3-253f98d67727/1994-0 00:12:52.110 --> 00:12:54.925 Up here in that picture, just gonna help you get a better 0df04eda-27ac-4d75-8cb3-253f98d67727/1994-1 00:12:54.925 --> 00:12:55.750 understanding so. 0df04eda-27ac-4d75-8cb3-253f98d67727/2003-0 00:12:56.410 --> 00:12:59.250 In this chair triggered event, there's nothing happening. 0df04eda-27ac-4d75-8cb3-253f98d67727/2014-0 00:12:59.570 --> 00:13:03.780 The entire fault is locked, and then all of a sudden the entire 0df04eda-27ac-4d75-8cb3-253f98d67727/2014-1 00:13:03.780 --> 00:13:04.570 fault slips. 0df04eda-27ac-4d75-8cb3-253f98d67727/2022-0 00:13:04.570 --> 00:13:08.742 So red to purple, all sensors show a very similar amount of 0df04eda-27ac-4d75-8cb3-253f98d67727/2022-1 00:13:08.742 --> 00:13:09.090 slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/2043-0 00:13:10.880 --> 00:13:15.556 On the flip side, with the fluid triggered events where we inject 0df04eda-27ac-4d75-8cb3-253f98d67727/2043-1 00:13:15.556 --> 00:13:19.666 water directly into a single point on the fault, we see a 0df04eda-27ac-4d75-8cb3-253f98d67727/2043-2 00:13:19.666 --> 00:13:20.800 swarm of events. 0df04eda-27ac-4d75-8cb3-253f98d67727/2051-0 00:13:21.040 --> 00:13:25.360 So as opposed to just one large event, food injection causes. 0df04eda-27ac-4d75-8cb3-253f98d67727/2069-0 00:13:26.910 --> 00:13:29.671 24 events that slip only a portion of the fault, and three 0df04eda-27ac-4d75-8cb3-253f98d67727/2069-1 00:13:29.671 --> 00:13:31.310 events that slip the entire fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/2092-0 00:13:32.190 --> 00:13:35.817 So if you look here at like this blue line, which corresponds to 0df04eda-27ac-4d75-8cb3-253f98d67727/2092-1 00:13:35.817 --> 00:13:39.222 this blue slip sensor, you see that there does as opposed to 0df04eda-27ac-4d75-8cb3-253f98d67727/2092-2 00:13:39.222 --> 00:13:42.626 one big jump. There are a lot of little jumps and so each of 0df04eda-27ac-4d75-8cb3-253f98d67727/2092-3 00:13:42.626 --> 00:13:43.910 these is an individual. 0df04eda-27ac-4d75-8cb3-253f98d67727/2095-0 00:13:44.700 --> 00:13:45.460 Seismic event. 0df04eda-27ac-4d75-8cb3-253f98d67727/2122-0 00:13:47.180 --> 00:13:51.391 If you look at, say, this orange one down here, which corresponds 0df04eda-27ac-4d75-8cb3-253f98d67727/2122-1 00:13:51.391 --> 00:13:54.901 to a patch of the fault that's far away from the fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/2122-2 00:13:54.901 --> 00:13:58.220 injection, we see only only a few events at a time. 0df04eda-27ac-4d75-8cb3-253f98d67727/2148-0 00:14:00.700 --> 00:14:03.635 It's hard to see in these graphs, but in this case there's 0df04eda-27ac-4d75-8cb3-253f98d67727/2148-1 00:14:03.635 --> 00:14:06.669 also a lot of a seismic slip, whereas in the share triggered 0df04eda-27ac-4d75-8cb3-253f98d67727/2148-2 00:14:06.669 --> 00:14:08.460 event kinda get a nucleation patch. 0df04eda-27ac-4d75-8cb3-253f98d67727/2151-0 00:14:08.460 --> 00:14:09.260 But that's about it. 0df04eda-27ac-4d75-8cb3-253f98d67727/2163-0 00:14:10.830 --> 00:14:14.630 So basically we can categorize fluid triggered events as 0df04eda-27ac-4d75-8cb3-253f98d67727/2163-1 00:14:14.630 --> 00:14:15.230 swarming. 0df04eda-27ac-4d75-8cb3-253f98d67727/2169-0 00:14:17.420 --> 00:14:18.500 As not swarming. 0df04eda-27ac-4d75-8cb3-253f98d67727/2179-0 00:14:18.500 --> 00:14:21.644 So those are just some really nice first order observations 0df04eda-27ac-4d75-8cb3-253f98d67727/2179-1 00:14:21.644 --> 00:14:23.740 that are pretty interesting to look at. 0df04eda-27ac-4d75-8cb3-253f98d67727/2217-0 00:14:25.990 --> 00:14:29.649 OK, so to this point we have a laboratory fault that has a 0df04eda-27ac-4d75-8cb3-253f98d67727/2217-1 00:14:29.649 --> 00:14:33.494 heterogeneous fluid pressure distribution and that can create 0df04eda-27ac-4d75-8cb3-253f98d67727/2217-2 00:14:33.494 --> 00:14:37.215 ruptures which can initiate, propagate and terminate within 0df04eda-27ac-4d75-8cb3-253f98d67727/2217-3 00:14:37.215 --> 00:14:38.270 the sample again. 0df04eda-27ac-4d75-8cb3-253f98d67727/2238-0 00:14:38.270 --> 00:14:41.881 So that puts us in a good place to kind of look at some of these 0df04eda-27ac-4d75-8cb3-253f98d67727/2238-1 00:14:41.881 --> 00:14:45.270 modeling results and see how we agree or disagree with them. 0df04eda-27ac-4d75-8cb3-253f98d67727/2263-0 00:14:47.230 --> 00:14:50.523 With that, I'm gonna try and answer one big question and 0df04eda-27ac-4d75-8cb3-253f98d67727/2263-1 00:14:50.523 --> 00:14:53.874 that's why do some events run away and become large while 0df04eda-27ac-4d75-8cb3-253f98d67727/2263-2 00:14:53.874 --> 00:14:55.030 others remain small. 0df04eda-27ac-4d75-8cb3-253f98d67727/2269-0 00:14:55.550 --> 00:14:57.590 Can answer some of this microsystemicity. 0df04eda-27ac-4d75-8cb3-253f98d67727/2271-0 00:14:59.350 --> 00:14:59.710 Or not. 0df04eda-27ac-4d75-8cb3-253f98d67727/2299-0 00:15:02.090 --> 00:15:05.434 1st I'm basically gonna sum up an entire paper in one slide 0df04eda-27ac-4d75-8cb3-253f98d67727/2299-1 00:15:05.434 --> 00:15:08.333 because I think this is relevant, but I don't wanna 0df04eda-27ac-4d75-8cb3-253f98d67727/2299-2 00:15:08.333 --> 00:15:11.845 spend too much time on it and that small events can jump start 0df04eda-27ac-4d75-8cb3-253f98d67727/2299-3 00:15:11.845 --> 00:15:12.570 large events. 0df04eda-27ac-4d75-8cb3-253f98d67727/2323-0 00:15:12.610 --> 00:15:16.105 So we see small events here where just the blue section of 0df04eda-27ac-4d75-8cb3-253f98d67727/2323-1 00:15:16.105 --> 00:15:19.720 the fault slip. So just part of the fault is slipping and we 0df04eda-27ac-4d75-8cb3-253f98d67727/2323-2 00:15:19.720 --> 00:15:22.090 have ones where the entire fault slips. 0df04eda-27ac-4d75-8cb3-253f98d67727/2332-0 00:15:23.630 --> 00:15:26.286 So to kind of look at them a little bit. Oh, yeah. Sorry, 0df04eda-27ac-4d75-8cb3-253f98d67727/2332-1 00:15:26.286 --> 00:15:26.470 man. 0df04eda-27ac-4d75-8cb3-253f98d67727/2359-0 00:15:26.470 --> 00:15:29.821 Shock. The entire fault ruptures for shock. Only part of the 0df04eda-27ac-4d75-8cb3-253f98d67727/2359-1 00:15:29.821 --> 00:15:32.678 fault. Raptures. And I acknowledge that I am taking 0df04eda-27ac-4d75-8cb3-253f98d67727/2359-2 00:15:32.678 --> 00:15:36.030 these terminologies slightly out of their normal definition. 0df04eda-27ac-4d75-8cb3-253f98d67727/2388-0 00:15:37.900 --> 00:15:41.332 But if we look at the ground motions created by each event 0df04eda-27ac-4d75-8cb3-253f98d67727/2388-1 00:15:41.332 --> 00:15:45.114 and then we compare them side by side, so we have the main shock 0df04eda-27ac-4d75-8cb3-253f98d67727/2388-2 00:15:45.114 --> 00:15:45.580 in blue. 0df04eda-27ac-4d75-8cb3-253f98d67727/2410-0 00:15:45.580 --> 00:15:48.398 So obviously it goes on to become much larger and the four 0df04eda-27ac-4d75-8cb3-253f98d67727/2410-1 00:15:48.398 --> 00:15:51.263 shock in red. So it starts off and then it kind of dies out 0df04eda-27ac-4d75-8cb3-253f98d67727/2410-2 00:15:51.263 --> 00:15:51.980 pretty quickly. 0df04eda-27ac-4d75-8cb3-253f98d67727/2441-0 00:15:52.500 --> 00:15:56.266 We can zoom in on that and see that for the 1st 42 microseconds 0df04eda-27ac-4d75-8cb3-253f98d67727/2441-1 00:15:56.266 --> 00:15:59.856 they match, which also agrees with our other our SLIP sensor 0df04eda-27ac-4d75-8cb3-253f98d67727/2441-2 00:15:59.856 --> 00:16:02.740 measurements and our other measurements as well. 0df04eda-27ac-4d75-8cb3-253f98d67727/2469-0 00:16:04.350 --> 00:16:07.675 And if we do some like back of the envelope calculations with 0df04eda-27ac-4d75-8cb3-253f98d67727/2469-1 00:16:07.675 --> 00:16:10.947 like rupture propagation speed that 42 microseconds is about 0df04eda-27ac-4d75-8cb3-253f98d67727/2469-2 00:16:10.947 --> 00:16:11.430 the size. 0df04eda-27ac-4d75-8cb3-253f98d67727/2472-0 00:16:12.400 --> 00:16:13.280 Of the foreshock. 0df04eda-27ac-4d75-8cb3-253f98d67727/2492-0 00:16:14.910 --> 00:16:18.318 So we're seeing that in a lot of cases the large event starts the 0df04eda-27ac-4d75-8cb3-253f98d67727/2492-1 00:16:18.318 --> 00:16:20.590 exact same way as the event just before it. 0df04eda-27ac-4d75-8cb3-253f98d67727/2522-0 00:16:23.510 --> 00:16:26.426 So we kind of conclude that a main shock and the 4th shock, 0df04eda-27ac-4d75-8cb3-253f98d67727/2522-1 00:16:26.426 --> 00:16:29.342 the same event, but they start the same, but the main shock 0df04eda-27ac-4d75-8cb3-253f98d67727/2522-2 00:16:29.342 --> 00:16:32.403 continues to propagate along the whole fault, whereas the four 0df04eda-27ac-4d75-8cb3-253f98d67727/2522-3 00:16:32.403 --> 00:16:33.230 shock terminates. 0df04eda-27ac-4d75-8cb3-253f98d67727/2545-0 00:16:36.540 --> 00:16:40.740 As that happened and in short, the answer is the initial sheer 0df04eda-27ac-4d75-8cb3-253f98d67727/2545-1 00:16:40.740 --> 00:16:44.873 stress levels. I'm showing a cartoon version of it, but there 0df04eda-27ac-4d75-8cb3-253f98d67727/2545-2 00:16:44.873 --> 00:16:47.940 are tons of studies that support my cartoons. 0df04eda-27ac-4d75-8cb3-253f98d67727/2565-0 00:16:49.510 --> 00:16:54.119 So if we look, we have stress and then versus distance along 0df04eda-27ac-4d75-8cb3-253f98d67727/2565-1 00:16:54.119 --> 00:16:59.030 the fault. So we have some peak stress and some residual stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/2574-0 00:17:00.890 --> 00:17:04.130 So these are like homeless material property. 0df04eda-27ac-4d75-8cb3-253f98d67727/2589-0 00:17:04.780 --> 00:17:07.448 If we have some initial stress distribution, so we're gonna 0df04eda-27ac-4d75-8cb3-253f98d67727/2589-1 00:17:07.448 --> 00:17:09.717 assume the initial shear stress along the fault is 0df04eda-27ac-4d75-8cb3-253f98d67727/2589-2 00:17:09.717 --> 00:17:10.340 heterogeneous. 0df04eda-27ac-4d75-8cb3-253f98d67727/2601-0 00:17:11.910 --> 00:17:14.649 Where the initial stress is greater than the residual and 0df04eda-27ac-4d75-8cb3-253f98d67727/2601-1 00:17:14.649 --> 00:17:15.310 close to peak. 0df04eda-27ac-4d75-8cb3-253f98d67727/2612-0 00:17:17.030 --> 00:17:19.310 You get a region that's favorable for rupture. 0df04eda-27ac-4d75-8cb3-253f98d67727/2615-0 00:17:20.230 --> 00:17:21.750 So if we look at the main shock. 0df04eda-27ac-4d75-8cb3-253f98d67727/2634-0 00:17:23.390 --> 00:17:27.000 It likely occurred in a case like this where a large parts of 0df04eda-27ac-4d75-8cb3-253f98d67727/2634-1 00:17:27.000 --> 00:17:30.494 the fault were favourable for rupture because they had high 0df04eda-27ac-4d75-8cb3-253f98d67727/2634-2 00:17:30.494 --> 00:17:31.310 stress levels. 0df04eda-27ac-4d75-8cb3-253f98d67727/2640-0 00:17:33.030 --> 00:17:35.950 Whereas the poor shock may have occurred. 0df04eda-27ac-4d75-8cb3-253f98d67727/2643-0 00:17:37.090 --> 00:17:38.170 This was much lower. 0df04eda-27ac-4d75-8cb3-253f98d67727/2655-0 00:17:41.510 --> 00:17:44.630 And so to get a better understanding of this and to 0df04eda-27ac-4d75-8cb3-253f98d67727/2655-1 00:17:44.630 --> 00:17:46.430 kind of play around with what? 0df04eda-27ac-4d75-8cb3-253f98d67727/2661-0 00:17:48.230 --> 00:17:50.790 To get yeah. To look at it more. Sorry. 0df04eda-27ac-4d75-8cb3-253f98d67727/2664-0 00:17:50.790 --> 00:17:51.750 And that's the size of the rapture. 0df04eda-27ac-4d75-8cb3-253f98d67727/2672-0 00:17:53.510 --> 00:17:54.670 We paired 2 cases. 0df04eda-27ac-4d75-8cb3-253f98d67727/2675-0 00:17:54.670 --> 00:17:56.910 Well, actually 3 cases, but I'm gonna talk about two. 0df04eda-27ac-4d75-8cb3-253f98d67727/2700-0 00:17:58.590 --> 00:18:01.806 One where the background share stress was really high, so the 0df04eda-27ac-4d75-8cb3-253f98d67727/2700-1 00:18:01.806 --> 00:18:05.125 entire fault was almost ready to host an earthquake on its own. 0df04eda-27ac-4d75-8cb3-253f98d67727/2700-2 00:18:05.125 --> 00:18:06.630 Even without fluid injection. 0df04eda-27ac-4d75-8cb3-253f98d67727/2729-0 00:18:08.210 --> 00:18:11.251 And that's shown up here and then we're gonna compare with 0df04eda-27ac-4d75-8cb3-253f98d67727/2729-1 00:18:11.251 --> 00:18:14.344 the low stress case where the entire fault is very far from 0df04eda-27ac-4d75-8cb3-253f98d67727/2729-2 00:18:14.344 --> 00:18:17.488 hosting an earthquake. In this case, we actually even backed 0df04eda-27ac-4d75-8cb3-253f98d67727/2729-3 00:18:17.488 --> 00:18:20.530 the stress off some from the residual shear stress levels. 0df04eda-27ac-4d75-8cb3-253f98d67727/2741-0 00:18:22.270 --> 00:18:25.630 And the way we did that was on our large scale lab fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/2757-0 00:18:26.230 --> 00:18:29.194 We changed how much we're pressing on this moving block. 0df04eda-27ac-4d75-8cb3-253f98d67727/2757-1 00:18:29.194 --> 00:18:31.950 So in the high stress case, we're pushing very hard. 0df04eda-27ac-4d75-8cb3-253f98d67727/2759-0 00:18:32.150 --> 00:18:33.230 So it's almost ready. 0df04eda-27ac-4d75-8cb3-253f98d67727/2777-0 00:18:34.830 --> 00:18:38.619 It's an earthquake and in the low stress case, we actually did 0df04eda-27ac-4d75-8cb3-253f98d67727/2777-1 00:18:38.619 --> 00:18:42.528 a few sheer triggered stick slop events and then back the stress 0df04eda-27ac-4d75-8cb3-253f98d67727/2777-2 00:18:42.528 --> 00:18:43.070 off some. 0df04eda-27ac-4d75-8cb3-253f98d67727/2797-0 00:18:44.790 --> 00:18:48.225 And so those are the conditions under which we injected fluid to 0df04eda-27ac-4d75-8cb3-253f98d67727/2797-1 00:18:48.225 --> 00:18:51.608 see how these background stress levels can affect the resulting 0df04eda-27ac-4d75-8cb3-253f98d67727/2797-2 00:18:51.608 --> 00:18:52.190 seismicity. 0df04eda-27ac-4d75-8cb3-253f98d67727/2799-0 00:18:55.420 --> 00:18:56.260 In high stress case. 0df04eda-27ac-4d75-8cb3-253f98d67727/2805-0 00:18:57.830 --> 00:18:58.590 We injected water. 0df04eda-27ac-4d75-8cb3-253f98d67727/2830-0 00:18:59.760 --> 00:19:03.714 We got a small region of a seismic slip and then three 0df04eda-27ac-4d75-8cb3-253f98d67727/2830-1 00:19:03.714 --> 00:19:07.237 seconds later default accelerated and we had the 0df04eda-27ac-4d75-8cb3-253f98d67727/2830-2 00:19:07.237 --> 00:19:10.760 entire fault slipped in one large dynamic event. 0df04eda-27ac-4d75-8cb3-253f98d67727/2837-0 00:19:12.310 --> 00:19:15.230 In comparison, we have the low stress case. 0df04eda-27ac-4d75-8cb3-253f98d67727/2849-0 00:19:19.310 --> 00:19:24.750 Had a large region of a seismic slip and then 500 seconds later. 0df04eda-27ac-4d75-8cb3-253f98d67727/2858-0 00:19:26.310 --> 00:19:28.230 A small part of the fault slipped dynamically. 0df04eda-27ac-4d75-8cb3-253f98d67727/2882-0 00:19:30.580 --> 00:19:35.150 So high stress, really fast or shortly after fluid injection we 0df04eda-27ac-4d75-8cb3-253f98d67727/2882-1 00:19:35.150 --> 00:19:39.720 had a large event, low stress, hundreds of seconds later we had 0df04eda-27ac-4d75-8cb3-253f98d67727/2882-2 00:19:39.720 --> 00:19:43.220 a dynamic event, but it was limited in its size. 0df04eda-27ac-4d75-8cb3-253f98d67727/2887-0 00:19:46.380 --> 00:19:48.060 Kind of two interesting cases. 0df04eda-27ac-4d75-8cb3-253f98d67727/2906-0 00:19:49.630 --> 00:19:53.302 But what I'm gonna look at a little bit is the a seismic slip 0df04eda-27ac-4d75-8cb3-253f98d67727/2906-1 00:19:53.302 --> 00:19:55.790 prior to the initiation of dynamic event. 0df04eda-27ac-4d75-8cb3-253f98d67727/2913-0 00:19:55.950 --> 00:19:57.670 And that happened in both cases. 0df04eda-27ac-4d75-8cb3-253f98d67727/2934-0 00:19:57.670 --> 00:20:01.397 So even when the fault was almost ready to slip, we still 0df04eda-27ac-4d75-8cb3-253f98d67727/2934-1 00:20:01.397 --> 00:20:05.382 had a region of a seismic slip and some kind of accelerations 0df04eda-27ac-4d75-8cb3-253f98d67727/2934-2 00:20:05.382 --> 00:20:07.310 and decelerations before that. 0df04eda-27ac-4d75-8cb3-253f98d67727/2938-0 00:20:08.150 --> 00:20:09.510 Sorry, I'm getting ahead of myself, OK? 0df04eda-27ac-4d75-8cb3-253f98d67727/2955-0 00:20:09.510 --> 00:20:13.350 So what we have on the X axis is time and then on the Y axis we 0df04eda-27ac-4d75-8cb3-253f98d67727/2955-1 00:20:13.350 --> 00:20:15.150 have distance along the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/2959-0 00:20:16.150 --> 00:20:17.030 At each location. 0df04eda-27ac-4d75-8cb3-253f98d67727/2991-0 00:20:17.690 --> 00:20:22.299 I'm plotting slip rate which is the color plot, so the darker 0df04eda-27ac-4d75-8cb3-253f98d67727/2991-1 00:20:22.299 --> 00:20:26.387 blue is slow slip, yellow is fast slip to the point of 0df04eda-27ac-4d75-8cb3-253f98d67727/2991-2 00:20:26.387 --> 00:20:31.071 dynamic or almost dynamic, and then the black lines are stress 0df04eda-27ac-4d75-8cb3-253f98d67727/2991-3 00:20:31.071 --> 00:20:33.450 measurements from strain gauges. 0df04eda-27ac-4d75-8cb3-253f98d67727/3000-0 00:20:34.130 --> 00:20:37.330 So we have 16 strain gauges and 16 slip sensors. 0df04eda-27ac-4d75-8cb3-253f98d67727/3011-0 00:20:37.330 --> 00:20:40.910 So we kind of get this nice map of what's going on spatially 0df04eda-27ac-4d75-8cb3-253f98d67727/3011-1 00:20:40.910 --> 00:20:41.850 along the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/3043-0 00:20:44.030 --> 00:20:48.955 So this little faucet indicates where we're injecting water. And 0df04eda-27ac-4d75-8cb3-253f98d67727/3043-1 00:20:48.955 --> 00:20:53.426 so we see in there that slow slip kind of starts to happen 0df04eda-27ac-4d75-8cb3-253f98d67727/3043-2 00:20:53.426 --> 00:20:58.276 and expands outwards. And that's indicated by the lighter color 0df04eda-27ac-4d75-8cb3-253f98d67727/3043-3 00:20:58.276 --> 00:21:00.550 maps or the lighter color map. 0df04eda-27ac-4d75-8cb3-253f98d67727/3055-0 00:21:02.180 --> 00:21:05.380 And then we can also see that in the high stress case. 0df04eda-27ac-4d75-8cb3-253f98d67727/3067-0 00:21:05.380 --> 00:21:09.144 So this one on the left, the slow slip begins earlier than 0df04eda-27ac-4d75-8cb3-253f98d67727/3067-1 00:21:09.144 --> 00:21:10.420 the low stress case. 0df04eda-27ac-4d75-8cb3-253f98d67727/3076-0 00:21:10.420 --> 00:21:13.100 So this happens after a about a second. 0df04eda-27ac-4d75-8cb3-253f98d67727/3083-0 00:21:13.100 --> 00:21:16.856 This one happens actually before the injection reaches peak 0df04eda-27ac-4d75-8cb3-253f98d67727/3083-1 00:21:16.856 --> 00:21:17.420 pressure. 0df04eda-27ac-4d75-8cb3-253f98d67727/3103-0 00:21:21.730 --> 00:21:25.580 Also look at the strain gauges and see that the A seismic 0df04eda-27ac-4d75-8cb3-253f98d67727/3103-1 00:21:25.580 --> 00:21:27.970 slipping patch is releasing stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/3108-0 00:21:28.330 --> 00:21:31.490 So in the slipping region, shear stress is decreasing. 0df04eda-27ac-4d75-8cb3-253f98d67727/3127-0 00:21:33.920 --> 00:21:37.400 Outside the slipping region, it's it's increasing. So you 0df04eda-27ac-4d75-8cb3-253f98d67727/3127-1 00:21:37.400 --> 00:21:41.300 have a region of a seismic slip decreasing stress and increasing 0df04eda-27ac-4d75-8cb3-253f98d67727/3127-2 00:21:41.300 --> 00:21:43.040 stress on the locked regions. 0df04eda-27ac-4d75-8cb3-253f98d67727/3136-0 00:21:46.050 --> 00:21:49.652 And maybe an easier way to look at it is just looking at a 0df04eda-27ac-4d75-8cb3-253f98d67727/3136-1 00:21:49.652 --> 00:21:50.690 snapshot in time. 0df04eda-27ac-4d75-8cb3-253f98d67727/3172-0 00:21:52.590 --> 00:21:57.950 So what we have here is distance along the fault. So and then on 0df04eda-27ac-4d75-8cb3-253f98d67727/3172-1 00:21:57.950 --> 00:22:03.311 the Y axis we have poor pressure in blue slip in the orange with 0df04eda-27ac-4d75-8cb3-253f98d67727/3172-2 00:22:03.311 --> 00:22:08.177 the circles and then change in shear stress with the green 0df04eda-27ac-4d75-8cb3-253f98d67727/3172-3 00:22:08.177 --> 00:22:08.590 axis. 0df04eda-27ac-4d75-8cb3-253f98d67727/3193-0 00:22:10.570 --> 00:22:14.098 And so on. The high stress case, these are each taken as a 0df04eda-27ac-4d75-8cb3-253f98d67727/3193-1 00:22:14.098 --> 00:22:16.850 snapshot in time just before the large event. 0df04eda-27ac-4d75-8cb3-253f98d67727/3218-0 00:22:17.650 --> 00:22:20.489 So we have a low stress case that produces a dynamic event 0df04eda-27ac-4d75-8cb3-253f98d67727/3218-1 00:22:20.489 --> 00:22:23.281 and a high stress case that produces a dynamic event, and 0df04eda-27ac-4d75-8cb3-253f98d67727/3218-2 00:22:23.281 --> 00:22:26.410 we're looking at the fault state just before that dynamic event. 0df04eda-27ac-4d75-8cb3-253f98d67727/3234-0 00:22:28.830 --> 00:22:31.827 And we're looking to see how much the fluid pressure has 0df04eda-27ac-4d75-8cb3-253f98d67727/3234-1 00:22:31.827 --> 00:22:33.510 changed, the fault stress state. 0df04eda-27ac-4d75-8cb3-253f98d67727/3261-0 00:22:34.510 --> 00:22:38.549 So in the high stress case in both cases, sorry, in both cases 0df04eda-27ac-4d75-8cb3-253f98d67727/3261-1 00:22:38.549 --> 00:22:42.461 fluid pressure reaches a similar peak and in the high stress 0df04eda-27ac-4d75-8cb3-253f98d67727/3261-2 00:22:42.461 --> 00:22:46.373 case, because this is only three seconds after fluid is been 0df04eda-27ac-4d75-8cb3-253f98d67727/3261-3 00:22:46.373 --> 00:22:46.950 injected. 0df04eda-27ac-4d75-8cb3-253f98d67727/3267-0 00:22:48.510 --> 00:22:49.950 That region is very limited. 0df04eda-27ac-4d75-8cb3-253f98d67727/3274-0 00:22:50.070 --> 00:22:52.270 So the water hasn't had time to diffuse away. 0df04eda-27ac-4d75-8cb3-253f98d67727/3282-0 00:22:53.910 --> 00:22:57.790 As such, the slipping region is smaller because that we haven't. 0df04eda-27ac-4d75-8cb3-253f98d67727/3312-0 00:22:58.450 --> 00:23:01.799 There hasn't been as much a seismic slit and the change in 0df04eda-27ac-4d75-8cb3-253f98d67727/3312-1 00:23:01.799 --> 00:23:05.488 sheer stress, so sheer stress is increasing in the locked region 0df04eda-27ac-4d75-8cb3-253f98d67727/3312-2 00:23:05.488 --> 00:23:09.007 and decreasing in the center, where the fluids being injected 0df04eda-27ac-4d75-8cb3-253f98d67727/3312-3 00:23:09.007 --> 00:23:10.370 from the A seismic slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/3318-0 00:23:12.030 --> 00:23:13.790 And it changes some a little bit. 0df04eda-27ac-4d75-8cb3-253f98d67727/3332-0 00:23:13.790 --> 00:23:17.066 So the fault does have to get itself to the point where it can 0df04eda-27ac-4d75-8cb3-253f98d67727/3332-1 00:23:17.066 --> 00:23:18.470 initiate a dynamic rupture. 0df04eda-27ac-4d75-8cb3-253f98d67727/3338-0 00:23:19.030 --> 00:23:22.510 But once that rupture is initiated, it's able to go. 0df04eda-27ac-4d75-8cb3-253f98d67727/3351-0 00:23:24.190 --> 00:23:27.390 Dynamic and rupture the entire fault. If we look at the low 0df04eda-27ac-4d75-8cb3-253f98d67727/3351-1 00:23:27.390 --> 00:23:28.030 stress case. 0df04eda-27ac-4d75-8cb3-253f98d67727/3365-0 00:23:29.170 --> 00:23:32.069 The main things I kinda want you to see are that there's a lot 0df04eda-27ac-4d75-8cb3-253f98d67727/3365-1 00:23:32.069 --> 00:23:32.530 more slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/3384-0 00:23:33.410 --> 00:23:36.236 There's a lot more change in sheer stress and the fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/3384-1 00:23:36.236 --> 00:23:39.366 pressure is higher. The fluid pressure is just higher because 0df04eda-27ac-4d75-8cb3-253f98d67727/3384-2 00:23:39.366 --> 00:23:39.770 of time. 0df04eda-27ac-4d75-8cb3-253f98d67727/3398-0 00:23:39.810 --> 00:23:42.418 We've let it sit longer, so the fluid pressure can diffuse 0df04eda-27ac-4d75-8cb3-253f98d67727/3398-1 00:23:42.418 --> 00:23:44.010 further and further along the fall. 0df04eda-27ac-4d75-8cb3-253f98d67727/3432-0 00:23:45.890 --> 00:23:49.140 Causes more aesisism, which causes more stress 0df04eda-27ac-4d75-8cb3-253f98d67727/3432-1 00:23:49.140 --> 00:23:53.566 redistribution, which is how we can get a dynamic slip event in 0df04eda-27ac-4d75-8cb3-253f98d67727/3432-2 00:23:53.566 --> 00:23:57.715 a case where the background shear stress should not be able 0df04eda-27ac-4d75-8cb3-253f98d67727/3432-3 00:23:57.715 --> 00:24:01.450 to host an event. It's because that where clustering. 0df04eda-27ac-4d75-8cb3-253f98d67727/3434-0 00:24:01.970 --> 00:24:03.650 Yeah, we're redistributing the shear stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/3475-0 00:24:06.790 --> 00:24:10.430 And so this kind of supports observations in Oklahoma, which 0df04eda-27ac-4d75-8cb3-253f98d67727/3475-1 00:24:10.430 --> 00:24:13.892 is kind of thought to not be super high stress in the 1st 0df04eda-27ac-4d75-8cb3-253f98d67727/3475-2 00:24:13.892 --> 00:24:17.414 place. But we do see seismicity there, whereas I think the 0df04eda-27ac-4d75-8cb3-253f98d67727/3475-3 00:24:17.414 --> 00:24:21.174 higher stress case is a little bit more like the 2017 event in 0df04eda-27ac-4d75-8cb3-253f98d67727/3475-4 00:24:21.174 --> 00:24:21.950 Pohang which. 0df04eda-27ac-4d75-8cb3-253f98d67727/3492-0 00:24:21.950 --> 00:24:25.614 Was Pohang South Korea, which is kind of they were thinking that 0df04eda-27ac-4d75-8cb3-253f98d67727/3492-1 00:24:25.614 --> 00:24:27.870 the stress in the area was really high. 0df04eda-27ac-4d75-8cb3-253f98d67727/3500-0 00:24:27.870 --> 00:24:29.030 So they see very quickly. 0df04eda-27ac-4d75-8cb3-253f98d67727/3501-0 00:24:29.030 --> 00:24:29.950 They see one big event. 0df04eda-27ac-4d75-8cb3-253f98d67727/3508-0 00:24:33.130 --> 00:24:36.370 Our observations of a seismic stress redistribution. 0df04eda-27ac-4d75-8cb3-253f98d67727/3531-0 00:24:38.160 --> 00:24:40.866 Observations from the centimeter scale and the computational 0df04eda-27ac-4d75-8cb3-253f98d67727/3531-1 00:24:40.866 --> 00:24:43.440 scale, which is always cool when things kind of match up. 0df04eda-27ac-4d75-8cb3-253f98d67727/3561-0 00:24:44.440 --> 00:24:48.730 Again, this Kappa figure that I've been showing you, as well 0df04eda-27ac-4d75-8cb3-253f98d67727/3561-1 00:24:48.730 --> 00:24:53.020 as some computational modeling from which show a decrease in 0df04eda-27ac-4d75-8cb3-253f98d67727/3561-2 00:24:53.020 --> 00:24:57.240 share stress and an increase in lock regions and then some. 0df04eda-27ac-4d75-8cb3-253f98d67727/3570-0 00:24:58.790 --> 00:25:01.441 Results the centimeter scale, which show accelerations in 0df04eda-27ac-4d75-8cb3-253f98d67727/3570-1 00:25:01.441 --> 00:25:01.670 slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/3588-0 00:25:05.470 --> 00:25:10.146 What that large dynamic event is, so we have so in each case 0df04eda-27ac-4d75-8cb3-253f98d67727/3588-1 00:25:10.146 --> 00:25:13.750 produces an event that radiates seismic waves. 0df04eda-27ac-4d75-8cb3-253f98d67727/3590-0 00:25:16.180 --> 00:25:17.260 Slips quickly. 0df04eda-27ac-4d75-8cb3-253f98d67727/3634-0 00:25:18.830 --> 00:25:22.784 Based on our thresholds for the lab, what we use for defining 0df04eda-27ac-4d75-8cb3-253f98d67727/3634-1 00:25:22.784 --> 00:25:26.674 seismic versus a seismic, but they're very different events. 0df04eda-27ac-4d75-8cb3-253f98d67727/3634-2 00:25:26.674 --> 00:25:30.628 And So what this is showing, this is distance along the fault 0df04eda-27ac-4d75-8cb3-253f98d67727/3634-3 00:25:30.628 --> 00:25:34.518 on the X axis and then slip on the Y axis and each line is a 0df04eda-27ac-4d75-8cb3-253f98d67727/3634-4 00:25:34.518 --> 00:25:34.710 SN. 0df04eda-27ac-4d75-8cb3-253f98d67727/3665-0 00:25:34.750 --> 00:25:38.079 In time. So when the lines are closely spaced together like 0df04eda-27ac-4d75-8cb3-253f98d67727/3665-1 00:25:38.079 --> 00:25:41.353 they are here that indicate slow slip. So the fall is only 0df04eda-27ac-4d75-8cb3-253f98d67727/3665-2 00:25:41.353 --> 00:25:44.350 slipping a little bit between each snapshot and time. 0df04eda-27ac-4d75-8cb3-253f98d67727/3671-0 00:25:45.310 --> 00:25:46.790 But when there's space far apart. 0df04eda-27ac-4d75-8cb3-253f98d67727/3675-0 00:25:46.790 --> 00:25:47.990 Kind of like they are here. 0df04eda-27ac-4d75-8cb3-253f98d67727/3696-0 00:25:49.170 --> 00:25:52.777 That's showing fast slip, so it slips a lot between each 0df04eda-27ac-4d75-8cb3-253f98d67727/3696-1 00:25:52.777 --> 00:25:56.068 snapshot and this lets us see how the slip is being 0df04eda-27ac-4d75-8cb3-253f98d67727/3696-2 00:25:56.068 --> 00:25:57.650 distributed on the phone. 0df04eda-27ac-4d75-8cb3-253f98d67727/3703-0 00:25:57.650 --> 00:25:59.570 Kinda how the rupture patterns are moving. 0df04eda-27ac-4d75-8cb3-253f98d67727/3741-0 00:26:01.230 --> 00:26:05.752 As well as looking at critical nucleation length, which I 0df04eda-27ac-4d75-8cb3-253f98d67727/3741-1 00:26:05.752 --> 00:26:10.352 showed later, so in the high stress case, First off, these 0df04eda-27ac-4d75-8cb3-253f98d67727/3741-2 00:26:10.352 --> 00:26:14.953 are the same Y scale, so the high stress case slips almost 0df04eda-27ac-4d75-8cb3-253f98d67727/3741-3 00:26:14.953 --> 00:26:18.150 four times as much as a low stress case. 0df04eda-27ac-4d75-8cb3-253f98d67727/3749-0 00:26:18.150 --> 00:26:21.950 So it's much bigger event and also slips the entire fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/3760-0 00:26:23.650 --> 00:26:27.335 In the low stress case, it only slips a portion of the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/3760-1 00:26:27.335 --> 00:26:27.930 They both. 0df04eda-27ac-4d75-8cb3-253f98d67727/3789-0 00:26:29.470 --> 00:26:32.365 The high stress case starts closer to the point of fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/3789-1 00:26:32.365 --> 00:26:35.362 injection, whereas the low stress case starts a little bit 0df04eda-27ac-4d75-8cb3-253f98d67727/3789-2 00:26:35.362 --> 00:26:38.004 further away because you've had that a seismic slip 0df04eda-27ac-4d75-8cb3-253f98d67727/3789-3 00:26:38.004 --> 00:26:39.630 redistributing the shear stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/3802-0 00:26:43.380 --> 00:26:47.279 So why touch on that a little bit, talk a little bit about why 0df04eda-27ac-4d75-8cb3-253f98d67727/3802-1 00:26:47.279 --> 00:26:49.260 the aesthetic slip is necessary. 0df04eda-27ac-4d75-8cb3-253f98d67727/3831-0 00:26:50.830 --> 00:26:53.676 And I'm gonna go back to this cartoon because I think it's 0df04eda-27ac-4d75-8cb3-253f98d67727/3831-1 00:26:53.676 --> 00:26:56.666 often a little bit easier to digest with stress on the Y axis 0df04eda-27ac-4d75-8cb3-253f98d67727/3831-2 00:26:56.666 --> 00:26:59.030 and then distance along the fault on the X axis. 0df04eda-27ac-4d75-8cb3-253f98d67727/3850-0 00:26:59.830 --> 00:27:03.245 So in the high stress case, the fault is nearly ready to host an 0df04eda-27ac-4d75-8cb3-253f98d67727/3850-1 00:27:03.245 --> 00:27:06.030 earthquake in the low stress case, it's far from it. 0df04eda-27ac-4d75-8cb3-253f98d67727/3857-0 00:27:06.030 --> 00:27:07.889 So we're just going to focus on the high stress case for a 0df04eda-27ac-4d75-8cb3-253f98d67727/3857-1 00:27:07.889 --> 00:27:08.110 minute. 0df04eda-27ac-4d75-8cb3-253f98d67727/3866-0 00:27:08.870 --> 00:27:12.747 Inject fluid pressure that decreases your peak and your 0df04eda-27ac-4d75-8cb3-253f98d67727/3866-1 00:27:12.747 --> 00:27:14.270 residual shear stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/3886-0 00:27:15.690 --> 00:27:21.097 Which creates more a larger region for favorable for rupture 0df04eda-27ac-4d75-8cb3-253f98d67727/3886-1 00:27:21.097 --> 00:27:26.416 and so sorry as we learn from the Coulomb stress initiation 0df04eda-27ac-4d75-8cb3-253f98d67727/3886-2 00:27:26.416 --> 00:27:28.810 starts when the background. 0df04eda-27ac-4d75-8cb3-253f98d67727/3902-0 00:27:30.590 --> 00:27:34.754 Normal stress is decreased such that the initial shear stress is 0df04eda-27ac-4d75-8cb3-253f98d67727/3902-1 00:27:34.754 --> 00:27:37.830 higher, and that's what creates slip right? So. 0df04eda-27ac-4d75-8cb3-253f98d67727/3913-0 00:27:39.430 --> 00:27:42.438 Wood pressure is required to decrease that peak beneath the 0df04eda-27ac-4d75-8cb3-253f98d67727/3913-1 00:27:42.438 --> 00:27:43.190 initial stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/3922-0 00:27:45.760 --> 00:27:48.520 And we can get an event that ruptures the entire fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/3928-0 00:27:50.070 --> 00:27:51.510 In the low stress case, however. 0df04eda-27ac-4d75-8cb3-253f98d67727/3936-0 00:27:53.640 --> 00:27:54.880 Decrease the fluid pressure. 0df04eda-27ac-4d75-8cb3-253f98d67727/3977-0 00:27:54.880 --> 00:27:58.634 We have to decrease it a lot more to get even initiate slip 0df04eda-27ac-4d75-8cb3-253f98d67727/3977-1 00:27:58.634 --> 00:28:02.452 and then also that only creates a really small region that's 0df04eda-27ac-4d75-8cb3-253f98d67727/3977-2 00:28:02.452 --> 00:28:06.332 favorable for rapture. And if that region is smaller than the 0df04eda-27ac-4d75-8cb3-253f98d67727/3977-3 00:28:06.332 --> 00:28:10.400 critical nucleation length, it's gonna continue to be a seismic. 0df04eda-27ac-4d75-8cb3-253f98d67727/4010-0 00:28:11.230 --> 00:28:15.543 So it's not until we slip the fault even more that we create a 0df04eda-27ac-4d75-8cb3-253f98d67727/4010-1 00:28:15.543 --> 00:28:20.061 region of the fault that's large enough to host dynamic slip, and 0df04eda-27ac-4d75-8cb3-253f98d67727/4010-2 00:28:20.061 --> 00:28:24.032 then we can get an event that initiates there and slips a 0df04eda-27ac-4d75-8cb3-253f98d67727/4010-3 00:28:24.032 --> 00:28:25.470 portion of the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/4017-0 00:28:27.040 --> 00:28:29.160 Again, this this is the cartoon version. 0df04eda-27ac-4d75-8cb3-253f98d67727/4049-0 00:28:30.870 --> 00:28:34.892 Can take snapshots in time leading up, so I'm gonna use the 0df04eda-27ac-4d75-8cb3-253f98d67727/4049-1 00:28:34.892 --> 00:28:38.982 low stress case because it was 500 seconds, so it gives us a 0df04eda-27ac-4d75-8cb3-253f98d67727/4049-2 00:28:38.982 --> 00:28:43.206 lot of nice time points that we can look at and we can see how 0df04eda-27ac-4d75-8cb3-253f98d67727/4049-3 00:28:43.206 --> 00:28:47.430 the fault conditions change with continued fluid injection so. 0df04eda-27ac-4d75-8cb3-253f98d67727/4060-0 00:28:47.430 --> 00:28:50.270 At 10 seconds, the fluid pressure is fairly narrow. 0df04eda-27ac-4d75-8cb3-253f98d67727/4082-0 00:28:50.310 --> 00:28:53.249 There's a little bit of slip and a little bit of stress 0df04eda-27ac-4d75-8cb3-253f98d67727/4082-1 00:28:53.249 --> 00:28:56.083 redistribution, but at 100 seconds the fluid pressure 0df04eda-27ac-4d75-8cb3-253f98d67727/4082-2 00:28:56.083 --> 00:28:58.550 continues to diffuse and it continues to grow. 0df04eda-27ac-4d75-8cb3-253f98d67727/4095-0 00:28:59.360 --> 00:29:02.291 A seismic slitting patch continues to grow and we 0df04eda-27ac-4d75-8cb3-253f98d67727/4095-1 00:29:02.291 --> 00:29:03.640 continue to get higher. 0df04eda-27ac-4d75-8cb3-253f98d67727/4100-0 00:29:04.610 --> 00:29:06.370 Stress levels on the locked regions. 0df04eda-27ac-4d75-8cb3-253f98d67727/4121-0 00:29:07.920 --> 00:29:11.540 And then 500 seconds later, we have an even larger fluid patch, 0df04eda-27ac-4d75-8cb3-253f98d67727/4121-1 00:29:11.540 --> 00:29:13.520 even larger. A seismic slip patch. 0df04eda-27ac-4d75-8cb3-253f98d67727/4133-0 00:29:14.080 --> 00:29:17.898 And we've built up more shear stress as well as a larger 0df04eda-27ac-4d75-8cb3-253f98d67727/4133-1 00:29:17.898 --> 00:29:19.640 region of increased shear. 0df04eda-27ac-4d75-8cb3-253f98d67727/4147-0 00:29:23.000 --> 00:29:27.640 So all that's kinda to conclude the stress levels control 0df04eda-27ac-4d75-8cb3-253f98d67727/4147-1 00:29:27.640 --> 00:29:28.920 earthquake size. 0df04eda-27ac-4d75-8cb3-253f98d67727/4155-0 00:29:31.870 --> 00:29:34.390 So when you have high stress, you create a large event. 0df04eda-27ac-4d75-8cb3-253f98d67727/4161-0 00:29:34.750 --> 00:29:39.095 Low stress is a small event and this is supported by modeling as 0df04eda-27ac-4d75-8cb3-253f98d67727/4161-1 00:29:39.095 --> 00:29:39.430 well. 0df04eda-27ac-4d75-8cb3-253f98d67727/4176-0 00:29:41.160 --> 00:29:45.611 So in this case they have the initial criticality of the 0df04eda-27ac-4d75-8cb3-253f98d67727/4176-1 00:29:45.611 --> 00:29:46.080 fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/4187-0 00:29:46.080 --> 00:29:49.148 So how close the fault is to hosting an earthquake on its 0df04eda-27ac-4d75-8cb3-253f98d67727/4187-1 00:29:49.148 --> 00:29:49.360 own? 0df04eda-27ac-4d75-8cb3-253f98d67727/4212-0 00:29:49.800 --> 00:29:53.497 And then they do a seismic versus total moment ratio. 0df04eda-27ac-4d75-8cb3-253f98d67727/4212-1 00:29:53.497 --> 00:29:57.947 Basically the closer you are to initiating an earthquake on your 0df04eda-27ac-4d75-8cb3-253f98d67727/4212-2 00:29:57.947 --> 00:30:00.480 own, you get lots more seismic slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/4234-0 00:30:02.920 --> 00:30:06.429 Sorry, when the fault is far from initiating an earthquake on 0df04eda-27ac-4d75-8cb3-253f98d67727/4234-1 00:30:06.429 --> 00:30:08.920 its own, you get a lot more a seismic slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/4242-0 00:30:12.560 --> 00:30:14.635 Check that I was going to talk about critical nucleation 0df04eda-27ac-4d75-8cb3-253f98d67727/4242-1 00:30:14.635 --> 00:30:15.400 lengths a little bit. 0df04eda-27ac-4d75-8cb3-253f98d67727/4253-0 00:30:15.400 --> 00:30:17.470 So if this is not your thing, you can ignore the next two 0df04eda-27ac-4d75-8cb3-253f98d67727/4253-1 00:30:17.470 --> 00:30:17.720 slides. 0df04eda-27ac-4d75-8cb3-253f98d67727/4280-0 00:30:18.240 --> 00:30:22.031 But what we do find is that fluid pressure did increase H * 0df04eda-27ac-4d75-8cb3-253f98d67727/4280-1 00:30:22.031 --> 00:30:25.190 S increase the critical nucleation length. If you 0df04eda-27ac-4d75-8cb3-253f98d67727/4280-2 00:30:25.190 --> 00:30:29.361 remember the critical nucleation length is inversely proportional 0df04eda-27ac-4d75-8cb3-253f98d67727/4280-3 00:30:29.361 --> 00:30:31.320 to the effective normal stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/4313-0 00:30:32.980 --> 00:30:37.508 So again, I'm showing these snapshots in time on these pink 0df04eda-27ac-4d75-8cb3-253f98d67727/4313-1 00:30:37.508 --> 00:30:42.037 purple pots with the fast slip as large gaps, small slip or 0df04eda-27ac-4d75-8cb3-253f98d67727/4313-2 00:30:42.037 --> 00:30:46.340 slow slip as like a where they're really close together. 0df04eda-27ac-4d75-8cb3-253f98d67727/4322-0 00:30:47.180 --> 00:30:51.500 So on the left is this is just a sheer triggered event. 0df04eda-27ac-4d75-8cb3-253f98d67727/4337-0 00:30:51.500 --> 00:30:55.433 Default is wet, but there's no fluid pressure, so we see that 0df04eda-27ac-4d75-8cb3-253f98d67727/4337-1 00:30:55.433 --> 00:30:57.780 we kind of get a gradual initiation. 0df04eda-27ac-4d75-8cb3-253f98d67727/4352-0 00:30:58.560 --> 00:31:01.395 Outside of a pretty small slipping patch, so you only get 0df04eda-27ac-4d75-8cb3-253f98d67727/4352-1 00:31:01.395 --> 00:31:03.840 critical nucleation length of about half a meter. 0df04eda-27ac-4d75-8cb3-253f98d67727/4372-0 00:31:05.300 --> 00:31:09.080 Right. Is where we have the high stress case with fluid being 0df04eda-27ac-4d75-8cb3-253f98d67727/4372-1 00:31:09.080 --> 00:31:11.580 injected right here at about 2.3 meters. 0df04eda-27ac-4d75-8cb3-253f98d67727/4386-0 00:31:12.060 --> 00:31:16.476 So we see a large slow slipping region and then it initiates out 0df04eda-27ac-4d75-8cb3-253f98d67727/4386-1 00:31:16.476 --> 00:31:17.020 of that. 0df04eda-27ac-4d75-8cb3-253f98d67727/4404-0 00:31:18.560 --> 00:31:21.700 So slipping region and we'll call the critical nucleation 0df04eda-27ac-4d75-8cb3-253f98d67727/4404-1 00:31:21.700 --> 00:31:23.000 length about 1.2 meters. 0df04eda-27ac-4d75-8cb3-253f98d67727/4412-0 00:31:25.690 --> 00:31:29.303 So that kinda matches up with the theory behind the critical 0df04eda-27ac-4d75-8cb3-253f98d67727/4412-1 00:31:29.303 --> 00:31:30.370 nucleation length. 0df04eda-27ac-4d75-8cb3-253f98d67727/4416-0 00:31:33.410 --> 00:31:34.050 There's the equation. 0df04eda-27ac-4d75-8cb3-253f98d67727/4418-0 00:31:34.050 --> 00:31:35.250 I should have put these slides. 0df04eda-27ac-4d75-8cb3-253f98d67727/4453-0 00:31:37.040 --> 00:31:40.818 But one thing that we did find interesting and probably warrant 0df04eda-27ac-4d75-8cb3-253f98d67727/4453-1 00:31:40.818 --> 00:31:44.654 a little bit more investigation is that in the high stress case, 0df04eda-27ac-4d75-8cb3-253f98d67727/4453-2 00:31:44.654 --> 00:31:48.019 it actually had a larger critical nucleation length than 0df04eda-27ac-4d75-8cb3-253f98d67727/4453-3 00:31:48.019 --> 00:31:49.200 the low stress case. 0df04eda-27ac-4d75-8cb3-253f98d67727/4469-0 00:31:50.880 --> 00:31:53.964 And so that is something that doesn't match up with a lot of 0df04eda-27ac-4d75-8cb3-253f98d67727/4469-1 00:31:53.964 --> 00:31:56.240 the modeling studies that we've seen so far. 0df04eda-27ac-4d75-8cb3-253f98d67727/4493-0 00:31:57.960 --> 00:32:01.411 And it may kind of tie into well. So it definitely ties into 0df04eda-27ac-4d75-8cb3-253f98d67727/4493-1 00:32:01.411 --> 00:32:04.693 the fact that nucleation is sensitive to details that are 0df04eda-27ac-4d75-8cb3-253f98d67727/4493-2 00:32:04.693 --> 00:32:04.920 not. 0df04eda-27ac-4d75-8cb3-253f98d67727/4500-0 00:32:06.510 --> 00:32:08.990 Like fully considered in this equation. 0df04eda-27ac-4d75-8cb3-253f98d67727/4503-0 00:32:08.990 --> 00:32:10.510 So things like healing. 0df04eda-27ac-4d75-8cb3-253f98d67727/4539-0 00:32:12.080 --> 00:32:14.931 Or loading rate right? Because in the high stress case it's 0df04eda-27ac-4d75-8cb3-253f98d67727/4539-1 00:32:14.931 --> 00:32:17.925 being loaded slower from the A seismic slip, whereas sorry the 0df04eda-27ac-4d75-8cb3-253f98d67727/4539-2 00:32:17.925 --> 00:32:20.681 low stress case is being effectively being loaded slower. 0df04eda-27ac-4d75-8cb3-253f98d67727/4539-3 00:32:20.681 --> 00:32:23.200 High stress case is effectively being loaded faster. 0df04eda-27ac-4d75-8cb3-253f98d67727/4551-0 00:32:24.800 --> 00:32:26.887 Because we're looking when you're looking at the slip rates 0df04eda-27ac-4d75-8cb3-253f98d67727/4551-1 00:32:26.887 --> 00:32:28.000 of the A seismic slipping patch. 0df04eda-27ac-4d75-8cb3-253f98d67727/4556-0 00:32:30.240 --> 00:32:31.520 And it's also kind of an interesting. 0df04eda-27ac-4d75-8cb3-253f98d67727/4573-0 00:32:33.200 --> 00:32:36.040 The nucleation length might have a time scale associated with it 0df04eda-27ac-4d75-8cb3-253f98d67727/4573-1 00:32:36.040 --> 00:32:37.920 as well that we're not considering, right? 0df04eda-27ac-4d75-8cb3-253f98d67727/4580-0 00:32:38.080 --> 00:32:40.240 These are both showing the same window in time. 0df04eda-27ac-4d75-8cb3-253f98d67727/4601-0 00:32:41.470 --> 00:32:44.973 So if we expanded the time window case, would we see more 0df04eda-27ac-4d75-8cb3-253f98d67727/4601-1 00:32:44.973 --> 00:32:47.390 of a critical nucleation length or not? 0df04eda-27ac-4d75-8cb3-253f98d67727/4608-0 00:32:48.150 --> 00:32:50.590 That was kind of an open-ended question from this work. 0df04eda-27ac-4d75-8cb3-253f98d67727/4642-0 00:32:53.570 --> 00:32:57.082 So to conclude, we found that fault Heterogeneities can 0df04eda-27ac-4d75-8cb3-253f98d67727/4642-1 00:32:57.082 --> 00:33:00.658 promote small events fault heterogeneities such as fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/4642-2 00:33:00.658 --> 00:33:04.233 injection can promote small events, some of which can go 0df04eda-27ac-4d75-8cb3-253f98d67727/4642-3 00:33:04.233 --> 00:33:04.610 large. 0df04eda-27ac-4d75-8cb3-253f98d67727/4652-0 00:33:04.610 --> 00:33:07.300 And this is really important for earthquake hazard prediction to 0df04eda-27ac-4d75-8cb3-253f98d67727/4652-1 00:33:07.300 --> 00:33:09.370 kind of understanding where the events can occur. 0df04eda-27ac-4d75-8cb3-253f98d67727/4675-0 00:33:10.920 --> 00:33:14.081 We also see that a seismic and seismic slip both result from 0df04eda-27ac-4d75-8cb3-253f98d67727/4675-1 00:33:14.081 --> 00:33:16.880 fluid injections under a variety of fault conditions. 0df04eda-27ac-4d75-8cb3-253f98d67727/4691-0 00:33:17.200 --> 00:33:20.318 This is kind of important for earthquake mechanics and 0df04eda-27ac-4d75-8cb3-253f98d67727/4691-1 00:33:20.318 --> 00:33:23.889 understanding how, like a fault that is far from critical, can 0df04eda-27ac-4d75-8cb3-253f98d67727/4691-2 00:33:23.889 --> 00:33:24.400 actually. 0df04eda-27ac-4d75-8cb3-253f98d67727/4696-0 00:33:25.000 --> 00:33:26.760 Produce dynamic events. 0df04eda-27ac-4d75-8cb3-253f98d67727/4727-0 00:33:28.320 --> 00:33:31.046 We also see that stress levels on the fall play a really 0df04eda-27ac-4d75-8cb3-253f98d67727/4727-1 00:33:31.046 --> 00:33:34.013 critical role in determining when rupture stopped, and that's 0df04eda-27ac-4d75-8cb3-253f98d67727/4727-2 00:33:34.013 --> 00:33:36.739 important for magnitude estimation. Is knowing when your 0df04eda-27ac-4d75-8cb3-253f98d67727/4727-3 00:33:36.739 --> 00:33:37.840 event is going to stop. 0df04eda-27ac-4d75-8cb3-253f98d67727/4738-0 00:33:39.960 --> 00:33:42.080 So this was all work that I did during my pH. 0df04eda-27ac-4d75-8cb3-253f98d67727/4751-0 00:33:44.280 --> 00:33:47.640 Here's a post doc and so kind of for my plan. 0df04eda-27ac-4d75-8cb3-253f98d67727/4767-0 00:33:48.280 --> 00:33:51.984 Tamra already mentioned a lot of this already, but I'm planning 0df04eda-27ac-4d75-8cb3-253f98d67727/4767-1 00:33:51.984 --> 00:33:55.400 to do continue this fluid injection study on the 2M scale. 0df04eda-27ac-4d75-8cb3-253f98d67727/4769-0 00:33:57.960 --> 00:33:58.400 And. 0df04eda-27ac-4d75-8cb3-253f98d67727/4786-0 00:33:59.210 --> 00:34:02.714 Answer Some open questions and kind of be able to see different 0df04eda-27ac-4d75-8cb3-253f98d67727/4786-1 00:34:02.714 --> 00:34:06.217 set up. Possibly look. Yeah, we have a whole bunch of different 0df04eda-27ac-4d75-8cb3-253f98d67727/4786-2 00:34:06.217 --> 00:34:09.010 things to do, including getting it up and running. 0df04eda-27ac-4d75-8cb3-253f98d67727/4798-0 00:34:10.560 --> 00:34:13.411 And while that's happening, I'm kinda doing like a little 0df04eda-27ac-4d75-8cb3-253f98d67727/4798-1 00:34:13.411 --> 00:34:14.640 calling at my side quest. 0df04eda-27ac-4d75-8cb3-253f98d67727/4818-0 00:34:16.280 --> 00:34:19.435 In observational seismology, looking at looking for induced 0df04eda-27ac-4d75-8cb3-253f98d67727/4818-1 00:34:19.435 --> 00:34:20.960 repeaters in southern Kansas. 0df04eda-27ac-4d75-8cb3-253f98d67727/4833-0 00:34:21.760 --> 00:34:26.416 So southern Kansas down here and this is a lot like Elizabeth 0df04eda-27ac-4d75-8cb3-253f98d67727/4833-1 00:34:26.416 --> 00:34:29.120 Cochran and Justin Rubenstein have. 0df04eda-27ac-4d75-8cb3-253f98d67727/4847-0 00:34:29.730 --> 00:34:33.210 A really nice catalog for about four years. 0df04eda-27ac-4d75-8cb3-253f98d67727/4850-0 00:34:33.210 --> 00:34:35.810 There's 100,000 events. 0df04eda-27ac-4d75-8cb3-253f98d67727/4859-0 00:34:37.360 --> 00:34:40.160 And so there's a lot in there to look for repeaters. 0df04eda-27ac-4d75-8cb3-253f98d67727/4880-0 00:34:41.920 --> 00:34:44.999 And the entire catalog is currently running. Hopefully as 0df04eda-27ac-4d75-8cb3-253f98d67727/4880-1 00:34:44.999 --> 00:34:47.920 we speak or it's finished. That would be exciting too. 0df04eda-27ac-4d75-8cb3-253f98d67727/4909-0 00:34:49.600 --> 00:34:52.681 But if we look at just, we've done a I've done a lot of 0df04eda-27ac-4d75-8cb3-253f98d67727/4909-1 00:34:52.681 --> 00:34:55.598 preliminary steps to make sure everything's working. 0df04eda-27ac-4d75-8cb3-253f98d67727/4909-2 00:34:55.598 --> 00:34:59.120 Everything's running well and if we just look at like 6 months. 0df04eda-27ac-4d75-8cb3-253f98d67727/4914-0 00:35:01.650 --> 00:35:02.170 You see that? 0df04eda-27ac-4d75-8cb3-253f98d67727/4917-0 00:35:02.170 --> 00:35:04.090 There's already a lot of events, so. 0df04eda-27ac-4d75-8cb3-253f98d67727/4927-0 00:35:05.640 --> 00:35:07.360 This being fluid injected in Kansas, I didn't. 0df04eda-27ac-4d75-8cb3-253f98d67727/4928-0 00:35:07.520 --> 00:35:08.240 That's probably background. 0df04eda-27ac-4d75-8cb3-253f98d67727/4930-0 00:35:08.240 --> 00:35:08.800 I should have covered. 0df04eda-27ac-4d75-8cb3-253f98d67727/4944-0 00:35:10.800 --> 00:35:16.440 And so this is the injection monthly barrels over time. 0df04eda-27ac-4d75-8cb3-253f98d67727/4957-0 00:35:18.080 --> 00:35:22.323 When there's definitely a lot of fluid being injected, there's a 0df04eda-27ac-4d75-8cb3-253f98d67727/4957-1 00:35:22.323 --> 00:35:23.760 lot of seismic events. 0df04eda-27ac-4d75-8cb3-253f98d67727/4961-0 00:35:26.910 --> 00:35:30.750 And we can look sorry, yeah. 0df04eda-27ac-4d75-8cb3-253f98d67727/4966-0 00:35:31.470 --> 00:35:32.950 And so we can look through all this. 0df04eda-27ac-4d75-8cb3-253f98d67727/4972-0 00:35:34.520 --> 00:35:35.360 And we find repeaters. 0df04eda-27ac-4d75-8cb3-253f98d67727/4982-0 00:35:35.440 --> 00:35:39.663 So kind of the pink and yellow events are the locations of 0df04eda-27ac-4d75-8cb3-253f98d67727/4982-1 00:35:39.663 --> 00:35:40.880 repeating events. 0df04eda-27ac-4d75-8cb3-253f98d67727/4991-0 00:35:42.330 --> 00:35:44.570 We plot them all on a magnitude vs time. 0df04eda-27ac-4d75-8cb3-253f98d67727/4995-0 00:35:44.570 --> 00:35:46.690 It looks very crazy and very chaotic. 0df04eda-27ac-4d75-8cb3-253f98d67727/5001-0 00:35:49.200 --> 00:35:50.440 Still kinda looking through. 0df04eda-27ac-4d75-8cb3-253f98d67727/5014-0 00:35:50.440 --> 00:35:52.764 Well, still waiting for the whole catalog to run to then 0df04eda-27ac-4d75-8cb3-253f98d67727/5014-1 00:35:52.764 --> 00:35:54.640 start to figure out what a lot of this means. 0df04eda-27ac-4d75-8cb3-253f98d67727/5031-0 00:35:54.920 --> 00:35:59.257 But some interesting things I've found so far are that everything 0df04eda-27ac-4d75-8cb3-253f98d67727/5031-1 00:35:59.257 --> 00:36:02.280 seems to be a lot of the repeaters are pairs. 0df04eda-27ac-4d75-8cb3-253f98d67727/5040-0 00:36:02.720 --> 00:36:04.800 So you kind of if you have a repeating earthquake, right? 0df04eda-27ac-4d75-8cb3-253f98d67727/5067-0 00:36:04.800 --> 00:36:08.250 It's the same section of the fault that slips over and over 0df04eda-27ac-4d75-8cb3-253f98d67727/5067-1 00:36:08.250 --> 00:36:11.642 in the same way such that you get the same magnitude, same 0df04eda-27ac-4d75-8cb3-253f98d67727/5067-2 00:36:11.642 --> 00:36:14.000 location, same, very similar wave forms. 0df04eda-27ac-4d75-8cb3-253f98d67727/5077-0 00:36:14.800 --> 00:36:17.786 And so if you have like a a size, if it's if a fault is 0df04eda-27ac-4d75-8cb3-253f98d67727/5077-1 00:36:17.786 --> 00:36:18.480 being loaded. 0df04eda-27ac-4d75-8cb3-253f98d67727/5085-0 00:36:19.360 --> 00:36:22.015 And what they see in a lot of other places that you get it 0df04eda-27ac-4d75-8cb3-253f98d67727/5085-1 00:36:22.015 --> 00:36:22.240 like. 0df04eda-27ac-4d75-8cb3-253f98d67727/5106-0 00:36:23.800 --> 00:36:28.472 A very regular recurrence time of these events, and so far I 0df04eda-27ac-4d75-8cb3-253f98d67727/5106-1 00:36:28.472 --> 00:36:31.920 haven't seen like a regular recurrence time. 0df04eda-27ac-4d75-8cb3-253f98d67727/5114-0 00:36:31.920 --> 00:36:36.361 Over the time Windows I'm looking at, I've primarily seen 0df04eda-27ac-4d75-8cb3-253f98d67727/5114-1 00:36:36.361 --> 00:36:37.280 event pairs. 0df04eda-27ac-4d75-8cb3-253f98d67727/5135-0 00:36:37.280 --> 00:36:41.291 So like if we look at this pinkish, reddish one right here, 0df04eda-27ac-4d75-8cb3-253f98d67727/5135-1 00:36:41.291 --> 00:36:45.302 it's two events that are pretty similar and they occur like 0df04eda-27ac-4d75-8cb3-253f98d67727/5135-2 00:36:45.302 --> 00:36:46.640 hours to days apart. 0df04eda-27ac-4d75-8cb3-253f98d67727/5143-0 00:36:48.240 --> 00:36:51.282 Despite the fact that I'm looking over a six month window 0df04eda-27ac-4d75-8cb3-253f98d67727/5143-1 00:36:51.282 --> 00:36:51.440 so. 0df04eda-27ac-4d75-8cb3-253f98d67727/5155-0 00:36:52.230 --> 00:36:55.835 I don't know what it means, but it's interesting and hopefully 0df04eda-27ac-4d75-8cb3-253f98d67727/5155-1 00:36:55.835 --> 00:36:59.326 they'll find out if you have thoughts, I'd love to chat with 0df04eda-27ac-4d75-8cb3-253f98d67727/5155-2 00:36:59.326 --> 00:37:00.070 you about it. 0df04eda-27ac-4d75-8cb3-253f98d67727/5167-0 00:37:01.800 --> 00:37:03.920 And kind of other things I find interesting. 0df04eda-27ac-4d75-8cb3-253f98d67727/5171-0 00:37:03.920 --> 00:37:05.400 I would love to chat with you all about. 0df04eda-27ac-4d75-8cb3-253f98d67727/5182-0 00:37:07.120 --> 00:37:10.520 Are looking at things like asperities and creep behavior. 0df04eda-27ac-4d75-8cb3-253f98d67727/5197-0 00:37:10.800 --> 00:37:13.929 So if you have two seismic patches linked by like a 0df04eda-27ac-4d75-8cb3-253f98d67727/5197-1 00:37:13.929 --> 00:37:17.240 creeping region in between them, how do they interact? 0df04eda-27ac-4d75-8cb3-253f98d67727/5203-0 00:37:17.240 --> 00:37:21.160 How does one disparity trigger the other or not? 0df04eda-27ac-4d75-8cb3-253f98d67727/5206-0 00:37:22.090 --> 00:37:23.210 Is it just a seismic? 0df04eda-27ac-4d75-8cb3-253f98d67727/5235-0 00:37:24.840 --> 00:37:28.080 I've also I'm interested in like looking at like fault geometry 0df04eda-27ac-4d75-8cb3-253f98d67727/5235-1 00:37:28.080 --> 00:37:31.016 and how can different fault geometries like if you have a 0df04eda-27ac-4d75-8cb3-253f98d67727/5235-2 00:37:31.016 --> 00:37:32.080 pretty much a radial. 0df04eda-27ac-4d75-8cb3-253f98d67727/5245-0 00:37:33.720 --> 00:37:36.560 Very like theoretical like Brune event. 0df04eda-27ac-4d75-8cb3-253f98d67727/5262-0 00:37:36.720 --> 00:37:39.080 How is it different than if you've got like a long, skinny 0df04eda-27ac-4d75-8cb3-253f98d67727/5262-1 00:37:39.080 --> 00:37:41.400 rupture that's definitely propagating from one end to the 0df04eda-27ac-4d75-8cb3-253f98d67727/5262-2 00:37:41.400 --> 00:37:41.640 other. 0df04eda-27ac-4d75-8cb3-253f98d67727/5305-0 00:37:44.510 --> 00:37:49.112 And then also kinda looking at source properties. So like if we 0df04eda-27ac-4d75-8cb3-253f98d67727/5305-1 00:37:49.112 --> 00:37:53.713 put a normal stress bump in the middle of a fault we in the lab 0df04eda-27ac-4d75-8cb3-253f98d67727/5305-2 00:37:53.713 --> 00:37:58.172 we find that that can increase peak ground acceleration by an 0df04eda-27ac-4d75-8cb3-253f98d67727/5305-3 00:37:58.172 --> 00:38:02.630 order of magnitude and kind of looking at what this means or. 0df04eda-27ac-4d75-8cb3-253f98d67727/5315-0 00:38:02.630 --> 00:38:05.630 How we can relate this to other things in the Earth so. 0df04eda-27ac-4d75-8cb3-253f98d67727/5320-0 00:38:07.880 --> 00:38:09.360 And end it there. Thank you. 0df04eda-27ac-4d75-8cb3-253f98d67727/5330-0 00:38:32.610 --> 00:38:36.290 Yep. So it's able to escape out the top and bottom. 0df04eda-27ac-4d75-8cb3-253f98d67727/5332-0 00:38:37.570 --> 00:38:37.690 Umm. 0df04eda-27ac-4d75-8cb3-253f98d67727/5339-0 00:38:38.490 --> 00:38:39.690 Ignore the text. 0df04eda-27ac-4d75-8cb3-253f98d67727/5347-0 00:38:40.210 --> 00:38:43.658 You got kind of a puddle on the top of your phone that I out 0df04eda-27ac-4d75-8cb3-253f98d67727/5347-1 00:38:43.658 --> 00:38:44.450 lined in blue. 0df04eda-27ac-4d75-8cb3-253f98d67727/5364-0 00:38:46.410 --> 00:38:50.351 So that's kind of unrealistic. If anyone has ideas on how to 0df04eda-27ac-4d75-8cb3-253f98d67727/5364-1 00:38:50.351 --> 00:38:52.290 contain it all I'm interested. 0df04eda-27ac-4d75-8cb3-253f98d67727/5380-0 00:39:04.990 --> 00:39:08.295 What? What it would change and I'm gonna show my engineering 0df04eda-27ac-4d75-8cb3-253f98d67727/5380-1 00:39:08.295 --> 00:39:10.030 background here, so I apologize. 0df04eda-27ac-4d75-8cb3-253f98d67727/5396-0 00:39:10.470 --> 00:39:14.790 What it changes is changes from a 2D rupture to a 1D rupture. 0df04eda-27ac-4d75-8cb3-253f98d67727/5420-0 00:39:15.350 --> 00:39:18.522 So that's one issue with when you inject into the center of 0df04eda-27ac-4d75-8cb3-253f98d67727/5420-1 00:39:18.522 --> 00:39:21.959 the fall, it kinda behaves like a 2D rupture until it propagates 0df04eda-27ac-4d75-8cb3-253f98d67727/5420-2 00:39:21.959 --> 00:39:25.395 until it breaks through the top and bottom and then you get like 0df04eda-27ac-4d75-8cb3-253f98d67727/5420-3 00:39:25.395 --> 00:39:26.030 a 1D effect. 0df04eda-27ac-4d75-8cb3-253f98d67727/5442-0 00:39:26.470 --> 00:39:29.439 And so if you actually had uniform flow pressure across the 0df04eda-27ac-4d75-8cb3-253f98d67727/5442-1 00:39:29.439 --> 00:39:32.657 entire fault or the depth of the fault, it would just be 1D from 0df04eda-27ac-4d75-8cb3-253f98d67727/5442-2 00:39:32.657 --> 00:39:33.350 the beginning. 0df04eda-27ac-4d75-8cb3-253f98d67727/5450-0 00:39:34.890 --> 00:39:36.810 As opposed to kind of going through this weird. 0df04eda-27ac-4d75-8cb3-253f98d67727/5457-0 00:39:38.010 --> 00:39:40.410 Slightly 2D in this region and 1D out here. 0df04eda-27ac-4d75-8cb3-253f98d67727/5465-0 00:39:41.490 --> 00:39:45.170 But I don't fundamentally change any of the conclusions. 0df04eda-27ac-4d75-8cb3-253f98d67727/5471-0 00:39:49.020 --> 00:39:51.220 Basically about this kind of 2D versus 1D issue. 0df04eda-27ac-4d75-8cb3-253f98d67727/5490-0 00:39:52.770 --> 00:39:55.509 So in some of your earlier plots, when you had the sort of 0df04eda-27ac-4d75-8cb3-253f98d67727/5490-1 00:39:55.509 --> 00:39:56.810 rainbow color-coded sensors. 0df04eda-27ac-4d75-8cb3-253f98d67727/5492-0 00:39:58.610 --> 00:39:59.810 Showing the difference. 0df04eda-27ac-4d75-8cb3-253f98d67727/5496-0 00:40:05.520 --> 00:40:07.120 The sort of Turk. 0df04eda-27ac-4d75-8cb3-253f98d67727/5498-0 00:40:10.850 --> 00:40:11.010 Ish. 0df04eda-27ac-4d75-8cb3-253f98d67727/5516-0 00:40:18.870 --> 00:40:24.253 One adjacent one is that capturing this is me forgetting 0df04eda-27ac-4d75-8cb3-253f98d67727/5516-1 00:40:24.253 --> 00:40:29.070 how Rainbow Order works in the plot in retrospect. 0df04eda-27ac-4d75-8cb3-253f98d67727/5520-0 00:40:29.110 --> 00:40:31.310 And Oh yeah, I apologize. 0df04eda-27ac-4d75-8cb3-253f98d67727/5539-0 00:40:31.310 --> 00:40:35.122 So that one actually should have been like over here. And yes, I 0df04eda-27ac-4d75-8cb3-253f98d67727/5539-1 00:40:35.122 --> 00:40:38.817 apologize for. So I guess maybe to generalize a question about 0df04eda-27ac-4d75-8cb3-253f98d67727/5539-2 00:40:38.817 --> 00:40:40.870 it though, that's related to this. 0df04eda-27ac-4d75-8cb3-253f98d67727/5551-0 00:40:44.540 --> 00:40:49.500 What degree are you capturing that transition between kind of 0df04eda-27ac-4d75-8cb3-253f98d67727/5551-1 00:40:49.500 --> 00:40:49.740 2D? 0df04eda-27ac-4d75-8cb3-253f98d67727/5557-0 00:40:57.020 --> 00:41:00.740 Yeah. So that is something. So I. 0df04eda-27ac-4d75-8cb3-253f98d67727/5572-0 00:41:03.270 --> 00:41:07.040 One of the studies I looked at it was on Plexiglas. And so 0df04eda-27ac-4d75-8cb3-253f98d67727/5572-1 00:41:07.040 --> 00:41:08.510 because plexiglass has. 0df04eda-27ac-4d75-8cb3-253f98d67727/5579-0 00:41:10.330 --> 00:41:13.530 It's more compliant, it mimics fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/5589-0 00:41:13.530 --> 00:41:16.690 That's 10 times harder. There's a lot of hand waving, literally. 0df04eda-27ac-4d75-8cb3-253f98d67727/5629-0 00:41:17.450 --> 00:41:21.081 And so it's a fault. That's in theory 10 times larger and so 0df04eda-27ac-4d75-8cb3-253f98d67727/5629-1 00:41:21.081 --> 00:41:24.832 also in theory 10 times deeper. And in that case, we were able 0df04eda-27ac-4d75-8cb3-253f98d67727/5629-2 00:41:24.832 --> 00:41:28.046 to see with the our ground motions, our piezoelectric 0df04eda-27ac-4d75-8cb3-253f98d67727/5629-3 00:41:28.046 --> 00:41:31.559 sensors, we were able to see events that did not propagate 0df04eda-27ac-4d75-8cb3-253f98d67727/5629-4 00:41:31.559 --> 00:41:32.690 the top and bottom. 0df04eda-27ac-4d75-8cb3-253f98d67727/5632-0 00:41:32.690 --> 00:41:33.130 Of the fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/5650-0 00:41:35.400 --> 00:41:38.945 And they still showed a lot of resemblances to the ones that 0df04eda-27ac-4d75-8cb3-253f98d67727/5650-1 00:41:38.945 --> 00:41:42.200 did kind of transition into that from the 2D to the 1D. 0df04eda-27ac-4d75-8cb3-253f98d67727/5665-0 00:41:44.610 --> 00:41:47.260 We didn't look into it much more than the fact that there are 0df04eda-27ac-4d75-8cb3-253f98d67727/5665-1 00:41:47.260 --> 00:41:49.953 some that don't break the edges of the fault and that they are 0df04eda-27ac-4d75-8cb3-253f98d67727/5665-2 00:41:49.953 --> 00:41:50.210 still. 0df04eda-27ac-4d75-8cb3-253f98d67727/5669-0 00:41:52.220 --> 00:41:53.580 Dave similarly so. 0df04eda-27ac-4d75-8cb3-253f98d67727/5674-0 00:41:57.160 --> 00:41:59.280 Future studies looking at that even more so. 0df04eda-27ac-4d75-8cb3-253f98d67727/5684-0 00:42:00.890 --> 00:42:03.999 Oh yeah, I'm sorry the question. OK. Next question, next 0df04eda-27ac-4d75-8cb3-253f98d67727/5684-1 00:42:03.999 --> 00:42:04.490 question. 0df04eda-27ac-4d75-8cb3-253f98d67727/5687-0 00:42:10.340 --> 00:42:10.940 Randy white. 0df04eda-27ac-4d75-8cb3-253f98d67727/5703-0 00:42:13.920 --> 00:42:18.116 On volcanoes and it's sort of the same problem. Inverted, we 0df04eda-27ac-4d75-8cb3-253f98d67727/5703-1 00:42:18.116 --> 00:42:20.800 have large amounts of magma coming up. 0df04eda-27ac-4d75-8cb3-253f98d67727/5746-0 00:42:22.410 --> 00:42:25.774 And we used to say that we didn't understand almost 0df04eda-27ac-4d75-8cb3-253f98d67727/5746-1 00:42:25.774 --> 00:42:29.850 anything until now. I feel like you can explain things that we 0df04eda-27ac-4d75-8cb3-253f98d67727/5746-2 00:42:29.850 --> 00:42:33.667 were unclear about what was happening, what we seem to see 0df04eda-27ac-4d75-8cb3-253f98d67727/5746-3 00:42:33.667 --> 00:42:37.549 is that as the magma comes up, there's a volume problem. So 0df04eda-27ac-4d75-8cb3-253f98d67727/5746-4 00:42:37.549 --> 00:42:39.490 it's shoved inside ways Earth. 0df04eda-27ac-4d75-8cb3-253f98d67727/5762-0 00:42:39.810 --> 00:42:43.136 It produces usually a few kilometers away and they have an 0df04eda-27ac-4d75-8cb3-253f98d67727/5762-1 00:42:43.136 --> 00:42:44.490 opening component which. 0df04eda-27ac-4d75-8cb3-253f98d67727/5763-0 00:42:46.980 --> 00:42:47.660 Swarming. 0df04eda-27ac-4d75-8cb3-253f98d67727/5765-0 00:42:48.550 --> 00:42:49.430 Induced events. 0df04eda-27ac-4d75-8cb3-253f98d67727/5777-0 00:42:50.970 --> 00:42:53.050 So it appears what we were wondering. 0df04eda-27ac-4d75-8cb3-253f98d67727/5791-0 00:42:53.050 --> 00:42:55.770 It seemed like the seismicity was migrating and we were 0df04eda-27ac-4d75-8cb3-253f98d67727/5791-1 00:42:55.770 --> 00:42:57.810 wondering if that's the fluids migrating. 0df04eda-27ac-4d75-8cb3-253f98d67727/5795-0 00:42:57.810 --> 00:42:59.810 Well, it seems like a single aquifer. 0df04eda-27ac-4d75-8cb3-253f98d67727/5806-0 00:43:01.530 --> 00:43:05.284 May exist in a single location and that's causing what you're 0df04eda-27ac-4d75-8cb3-253f98d67727/5806-1 00:43:05.284 --> 00:43:05.890 saying is. 0df04eda-27ac-4d75-8cb3-253f98d67727/5825-0 00:43:07.610 --> 00:43:12.378 Increasingly large a seismic slip area, and that's why the 0df04eda-27ac-4d75-8cb3-253f98d67727/5825-1 00:43:12.378 --> 00:43:15.530 seismicity is moving outwards. That's. 0df04eda-27ac-4d75-8cb3-253f98d67727/5836-0 00:43:17.160 --> 00:43:21.880 Secondly, these intrusions come up many of them, maybe. 0df04eda-27ac-4d75-8cb3-253f98d67727/5845-0 00:43:21.880 --> 00:43:24.360 Let's say a week apart. In the case of Monster attack. 0df04eda-27ac-4d75-8cb3-253f98d67727/5858-0 00:43:26.090 --> 00:43:30.603 So each time the initial stress will be less because it was 0df04eda-27ac-4d75-8cb3-253f98d67727/5858-1 00:43:30.603 --> 00:43:33.010 reduced by the previous episode. 0df04eda-27ac-4d75-8cb3-253f98d67727/5865-0 00:43:34.730 --> 00:43:36.410 So that implies that there should be. 0df04eda-27ac-4d75-8cb3-253f98d67727/5877-0 00:43:38.010 --> 00:43:41.010 Increasing delay time between the onset of the size. 0df04eda-27ac-4d75-8cb3-253f98d67727/5882-0 00:43:43.450 --> 00:43:45.890 Cool. Is that something you observe? 0df04eda-27ac-4d75-8cb3-253f98d67727/5885-0 00:43:46.050 --> 00:43:47.130 Sorry, we observe, OK. 0df04eda-27ac-4d75-8cb3-253f98d67727/5893-0 00:43:50.050 --> 00:43:52.610 Like to sign up to talk to you for about a week. 0df04eda-27ac-4d75-8cb3-253f98d67727/5897-0 00:43:54.170 --> 00:43:55.610 I don't know. That'll be enough time. 0df04eda-27ac-4d75-8cb3-253f98d67727/5901-0 00:43:57.210 --> 00:43:57.450 Yeah. So. 0df04eda-27ac-4d75-8cb3-253f98d67727/5907-0 00:43:57.970 --> 00:44:00.770 Randy pointed out some similarities between. 0df04eda-27ac-4d75-8cb3-253f98d67727/5929-0 00:44:02.370 --> 00:44:05.401 This work and kind of the fluid injection and volcanoes where 0df04eda-27ac-4d75-8cb3-253f98d67727/5929-1 00:44:05.401 --> 00:44:07.650 you have the magma and magma is fluid, right? 0df04eda-27ac-4d75-8cb3-253f98d67727/5932-0 00:44:07.650 --> 00:44:09.010 Sorry, excuse me, I don't know much about. 0df04eda-27ac-4d75-8cb3-253f98d67727/5940-0 00:44:10.690 --> 00:44:12.290 Coming through and also creating swarms of events. 0df04eda-27ac-4d75-8cb3-253f98d67727/5945-0 00:44:13.930 --> 00:44:14.890 In that case as well, sorry. 0df04eda-27ac-4d75-8cb3-253f98d67727/5961-0 00:44:16.530 --> 00:44:20.394 This is water, seduced by movement, OK. And then after. So 0df04eda-27ac-4d75-8cb3-253f98d67727/5961-1 00:44:20.394 --> 00:44:22.490 I forgot it. Two more questions. 0df04eda-27ac-4d75-8cb3-253f98d67727/5980-0 00:44:23.620 --> 00:44:27.796 After a number of these episodes, I guess you've reduced 0df04eda-27ac-4d75-8cb3-253f98d67727/5980-1 00:44:27.796 --> 00:44:31.460 the stress enough that fault will no longer move. 0df04eda-27ac-4d75-8cb3-253f98d67727/5994-0 00:44:33.010 --> 00:44:36.343 Because we see that all right, after maybe eight or eight of 0df04eda-27ac-4d75-8cb3-253f98d67727/5994-1 00:44:36.343 --> 00:44:38.530 these. Now another fault starts moving. 0df04eda-27ac-4d75-8cb3-253f98d67727/6016-0 00:44:38.610 --> 00:44:43.977 So we may have had tectonically loaded but less than the first 0df04eda-27ac-4d75-8cb3-253f98d67727/6016-1 00:44:43.977 --> 00:44:47.130 one, so it starts moving eventually. 0df04eda-27ac-4d75-8cb3-253f98d67727/6031-0 00:44:47.690 --> 00:44:52.006 Initially we see what we call the Magar formula, the intruded 0df04eda-27ac-4d75-8cb3-253f98d67727/6031-1 00:44:52.006 --> 00:44:54.930 volumes proportional to the size of this. 0df04eda-27ac-4d75-8cb3-253f98d67727/6049-0 00:44:56.140 --> 00:44:59.392 But eventually we see that formula falling apart, worse and 0df04eda-27ac-4d75-8cb3-253f98d67727/6049-1 00:44:59.392 --> 00:45:00.260 worse and worse. 0df04eda-27ac-4d75-8cb3-253f98d67727/6057-0 00:45:00.700 --> 00:45:04.340 So apparently we're getting more and more a seismic slip. 0df04eda-27ac-4d75-8cb3-253f98d67727/6064-0 00:45:06.370 --> 00:45:07.850 Yes, that makes sense to me. 0df04eda-27ac-4d75-8cb3-253f98d67727/6102-0 00:45:07.850 --> 00:45:11.432 So one of the questions was that during the fluids near 0df04eda-27ac-4d75-8cb3-253f98d67727/6102-1 00:45:11.432 --> 00:45:15.590 volcanoes, you kind of get it'll fall the Magar for a little bit 0df04eda-27ac-4d75-8cb3-253f98d67727/6102-2 00:45:15.590 --> 00:45:19.556 that eventually starts to fall apart and with continued fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/6102-3 00:45:19.556 --> 00:45:23.650 injection, eventually one fall will stop slipping. But like one 0df04eda-27ac-4d75-8cb3-253f98d67727/6102-4 00:45:23.650 --> 00:45:25.250 nearby, will start again. 0df04eda-27ac-4d75-8cb3-253f98d67727/6137-0 00:45:26.740 --> 00:45:31.198 And that does agree with what I've observed. So in my lab, in 0df04eda-27ac-4d75-8cb3-253f98d67727/6137-1 00:45:31.198 --> 00:45:35.080 the lab experiments, we kind of go beyond some of the 0df04eda-27ac-4d75-8cb3-253f98d67727/6137-2 00:45:35.080 --> 00:45:38.604 assumptions from Magar, particularly in that the 0df04eda-27ac-4d75-8cb3-253f98d67727/6137-3 00:45:38.604 --> 00:45:43.349 earthquakes go outside the where the region of fluid pressure is, 0df04eda-27ac-4d75-8cb3-253f98d67727/6137-4 00:45:43.349 --> 00:45:46.010 right. So the a side mix slip creat. 0df04eda-27ac-4d75-8cb3-253f98d67727/6159-0 00:45:46.820 --> 00:45:49.929 Regions beyond that are unaffected by fluid pressure 0df04eda-27ac-4d75-8cb3-253f98d67727/6159-1 00:45:49.929 --> 00:45:52.100 directly that can create seismicity. 0df04eda-27ac-4d75-8cb3-253f98d67727/6161-0 00:45:52.260 --> 00:45:54.100 So that's probably one of the biggest. 0df04eda-27ac-4d75-8cb3-253f98d67727/6164-0 00:45:55.010 --> 00:45:55.770 Deviation. 0df04eda-27ac-4d75-8cb3-253f98d67727/6178-0 00:45:56.990 --> 00:46:01.599 If the intrusion is really, really slow, really slow, we can 0df04eda-27ac-4d75-8cb3-253f98d67727/6178-1 00:46:01.599 --> 00:46:03.790 we get a lot of that leakage. 0df04eda-27ac-4d75-8cb3-253f98d67727/6189-0 00:46:03.790 --> 00:46:09.224 So keep the leakage. OK, cool, cool and volcanoes. Water also 0df04eda-27ac-4d75-8cb3-253f98d67727/6189-1 00:46:09.224 --> 00:46:09.750 leaks. 0df04eda-27ac-4d75-8cb3-253f98d67727/6192-0 00:46:09.750 --> 00:46:12.350 Everywhere is the conclusion so. 0df04eda-27ac-4d75-8cb3-253f98d67727/6205-0 00:46:34.790 --> 00:46:36.910 Curious about for that case A case B. 0df04eda-27ac-4d75-8cb3-253f98d67727/6207-0 00:46:39.500 --> 00:46:40.220 Address initially. 0df04eda-27ac-4d75-8cb3-253f98d67727/6212-0 00:46:42.400 --> 00:46:43.920 Which I don't know much about these areas. 0df04eda-27ac-4d75-8cb3-253f98d67727/6214-0 00:46:44.720 --> 00:46:45.240 That have. 0df04eda-27ac-4d75-8cb3-253f98d67727/6216-0 00:46:52.080 --> 00:46:53.360 If you think that. 0df04eda-27ac-4d75-8cb3-253f98d67727/6220-0 00:46:56.740 --> 00:46:58.860 Do you think that there may be? 0df04eda-27ac-4d75-8cb3-253f98d67727/6231-0 00:47:04.260 --> 00:47:06.599 I guess like have you ever thought about those areas and if 0df04eda-27ac-4d75-8cb3-253f98d67727/6231-1 00:47:06.599 --> 00:47:07.340 they could be like? 0df04eda-27ac-4d75-8cb3-253f98d67727/6238-0 00:47:08.690 --> 00:47:12.210 Not exactly K speed, but even like a lower initial speed. 0df04eda-27ac-4d75-8cb3-253f98d67727/6271-0 00:47:13.120 --> 00:47:15.973 Yeah. So the question was well, the first question was that I 0df04eda-27ac-4d75-8cb3-253f98d67727/6271-1 00:47:15.973 --> 00:47:18.826 kind of compared like the high stress case to PO Hong and the 0df04eda-27ac-4d75-8cb3-253f98d67727/6271-2 00:47:18.826 --> 00:47:21.541 low stress case to Oklahoma. And I compared it to Oklahoma 0df04eda-27ac-4d75-8cb3-253f98d67727/6271-3 00:47:21.541 --> 00:47:24.302 because I read it in a paper once and I think everyone here 0df04eda-27ac-4d75-8cb3-253f98d67727/6271-4 00:47:24.302 --> 00:47:24.440 in. 0df04eda-27ac-4d75-8cb3-253f98d67727/6284-0 00:47:24.440 --> 00:47:27.391 This room would know better than me and exactly what the stress 0df04eda-27ac-4d75-8cb3-253f98d67727/6284-1 00:47:27.391 --> 00:47:28.360 state in Oklahoma is. 0df04eda-27ac-4d75-8cb3-253f98d67727/6287-0 00:47:29.970 --> 00:47:30.930 On my reading list is a. 0df04eda-27ac-4d75-8cb3-253f98d67727/6294-0 00:47:30.930 --> 00:47:32.450 What's the stress state in Kansas paper? 0df04eda-27ac-4d75-8cb3-253f98d67727/6297-0 00:47:32.450 --> 00:47:34.770 So yeah, still learning. 0df04eda-27ac-4d75-8cb3-253f98d67727/6315-0 00:47:35.730 --> 00:47:38.774 And then the second part of the question was what about places 0df04eda-27ac-4d75-8cb3-253f98d67727/6315-1 00:47:38.774 --> 00:47:41.770 that don't create seismicity, where you have fluid injection? 0df04eda-27ac-4d75-8cb3-253f98d67727/6320-0 00:47:42.050 --> 00:47:44.650 But no produced seismicity and I don't know. 0df04eda-27ac-4d75-8cb3-253f98d67727/6329-0 00:47:45.730 --> 00:47:48.930 I think even lower stress could definitely be a possibility. 0df04eda-27ac-4d75-8cb3-253f98d67727/6361-0 00:47:52.050 --> 00:47:55.768 I think high permeability could be a possibility, so as opposed 0df04eda-27ac-4d75-8cb3-253f98d67727/6361-1 00:47:55.768 --> 00:47:58.963 to building up a region of really high fluid pressure, 0df04eda-27ac-4d75-8cb3-253f98d67727/6361-2 00:47:58.963 --> 00:48:02.507 everything's just kind of more evenly dispersed, which would 0df04eda-27ac-4d75-8cb3-253f98d67727/6361-3 00:48:02.507 --> 00:48:04.250 promote a seismic slip, right? 0df04eda-27ac-4d75-8cb3-253f98d67727/6396-0 00:48:04.250 --> 00:48:08.056 So in my experiments everything was very heterogeneous and I 0df04eda-27ac-4d75-8cb3-253f98d67727/6396-1 00:48:08.056 --> 00:48:11.924 found that when I increase that heterogeneity. So like when I 0df04eda-27ac-4d75-8cb3-253f98d67727/6396-2 00:48:11.924 --> 00:48:15.480 made it even more dramatic versus letting it diffuse and 0df04eda-27ac-4d75-8cb3-253f98d67727/6396-3 00:48:15.480 --> 00:48:17.290 being like kind of more even. 0df04eda-27ac-4d75-8cb3-253f98d67727/6400-0 00:48:18.130 --> 00:48:18.730 The more dramatic. 0df04eda-27ac-4d75-8cb3-253f98d67727/6423-0 00:48:19.550 --> 00:48:24.051 Seismicity so that those would be my two first guesses, but 0df04eda-27ac-4d75-8cb3-253f98d67727/6423-1 00:48:24.051 --> 00:48:28.253 there might also be things like in the rock or in other 0df04eda-27ac-4d75-8cb3-253f98d67727/6423-2 00:48:28.253 --> 00:48:32.230 geological factors that I don't know much about. So. 0df04eda-27ac-4d75-8cb3-253f98d67727/6425-0 00:48:40.490 --> 00:48:40.610 Yes. 0df04eda-27ac-4d75-8cb3-253f98d67727/6427-0 00:48:44.810 --> 00:48:45.650 No. 0df04eda-27ac-4d75-8cb3-253f98d67727/6433-0 00:48:48.050 --> 00:48:50.810 What stress are you talking about so? 0df04eda-27ac-4d75-8cb3-253f98d67727/6438-0 00:48:52.610 --> 00:48:54.130 These machines are are messy. 0df04eda-27ac-4d75-8cb3-253f98d67727/6460-0 00:48:55.850 --> 00:48:59.526 We are theoretically being like, yes, everything is about uniform 0df04eda-27ac-4d75-8cb3-253f98d67727/6460-1 00:48:59.526 --> 00:49:01.810 along the fault without fluid injection. 0df04eda-27ac-4d75-8cb3-253f98d67727/6462-0 00:49:02.050 --> 00:49:03.130 That's not actually the case. 0df04eda-27ac-4d75-8cb3-253f98d67727/6494-0 00:49:04.810 --> 00:49:08.423 You get kind of like au shape normal stress distribution and 0df04eda-27ac-4d75-8cb3-253f98d67727/6494-1 00:49:08.423 --> 00:49:12.155 then when you just apply normal stress, if you think about you 0df04eda-27ac-4d75-8cb3-253f98d67727/6494-2 00:49:12.155 --> 00:49:15.650 take like a a steel block and press it into rubber, right? 0df04eda-27ac-4d75-8cb3-253f98d67727/6511-0 00:49:16.310 --> 00:49:18.819 It's gonna like curve up on the edges and you're gonna get 0df04eda-27ac-4d75-8cb3-253f98d67727/6511-1 00:49:18.819 --> 00:49:20.350 stress concentrations on the sides. 0df04eda-27ac-4d75-8cb3-253f98d67727/6523-0 00:49:21.270 --> 00:49:24.204 This is rock and rock, but you still get stress concentrations 0df04eda-27ac-4d75-8cb3-253f98d67727/6523-1 00:49:24.204 --> 00:49:24.950 in the same way. 0df04eda-27ac-4d75-8cb3-253f98d67727/6539-0 00:49:25.830 --> 00:49:29.929 And then when we apply shear stress to this block because 0df04eda-27ac-4d75-8cb3-253f98d67727/6539-1 00:49:29.929 --> 00:49:33.887 we're only pushing at one end, you kind of like, get an 0df04eda-27ac-4d75-8cb3-253f98d67727/6539-2 00:49:33.887 --> 00:49:35.230 overturning moment. 0df04eda-27ac-4d75-8cb3-253f98d67727/6543-0 00:49:35.230 --> 00:49:37.310 So the rock wants to rotate a little bit. 0df04eda-27ac-4d75-8cb3-253f98d67727/6562-0 00:49:38.850 --> 00:49:42.227 A lot of these things are solved by the diatribe style triangles 0df04eda-27ac-4d75-8cb3-253f98d67727/6562-1 00:49:42.227 --> 00:49:44.930 where you get a slightly more uniform stress state. 0df04eda-27ac-4d75-8cb3-253f98d67727/6572-0 00:49:47.420 --> 00:49:49.597 That's kind of getting into trade-offs of different 0df04eda-27ac-4d75-8cb3-253f98d67727/6572-1 00:49:49.597 --> 00:49:50.100 apparatuses. 0df04eda-27ac-4d75-8cb3-253f98d67727/6574-0 00:50:00.520 --> 00:50:01.040 So. 0df04eda-27ac-4d75-8cb3-253f98d67727/6578-0 00:50:12.100 --> 00:50:12.700 Yes. 0df04eda-27ac-4d75-8cb3-253f98d67727/6588-0 00:50:18.810 --> 00:50:22.490 So there are multiple, yes can repeat it. 0df04eda-27ac-4d75-8cb3-253f98d67727/6614-0 00:50:22.810 --> 00:50:26.754 So he's asking if the stress along the fault is not uniform. 0df04eda-27ac-4d75-8cb3-253f98d67727/6614-1 00:50:26.754 --> 00:50:30.892 Where am I injecting relative to that uniformness and how is it 0df04eda-27ac-4d75-8cb3-253f98d67727/6614-2 00:50:30.892 --> 00:50:32.250 affecting everything? 0df04eda-27ac-4d75-8cb3-253f98d67727/6642-0 00:50:32.610 --> 00:50:36.067 So I have a multi part answer to this in one of the studies when 0df04eda-27ac-4d75-8cb3-253f98d67727/6642-1 00:50:36.067 --> 00:50:39.366 I was doing the smaller scale in the PMA, it's easier to like 0df04eda-27ac-4d75-8cb3-253f98d67727/6642-2 00:50:39.366 --> 00:50:42.610 lift it out and mess around with the fault and resurface the 0df04eda-27ac-4d75-8cb3-253f98d67727/6642-3 00:50:42.610 --> 00:50:42.930 fault. 0df04eda-27ac-4d75-8cb3-253f98d67727/6647-0 00:50:43.170 --> 00:50:45.250 And so I actually put talc patches on the edges. 0df04eda-27ac-4d75-8cb3-253f98d67727/6659-0 00:50:46.050 --> 00:50:48.498 To relieve those stress concentrations on the end and 0df04eda-27ac-4d75-8cb3-253f98d67727/6659-1 00:50:48.498 --> 00:50:50.130 create a more uniform stress state. 0df04eda-27ac-4d75-8cb3-253f98d67727/6662-0 00:50:52.250 --> 00:50:52.890 And it's still. 0df04eda-27ac-4d75-8cb3-253f98d67727/6665-0 00:50:54.130 --> 00:50:55.210 Swarming like behavior. 0df04eda-27ac-4d75-8cb3-253f98d67727/6671-0 00:50:56.850 --> 00:50:58.690 #1, S and #2. 0df04eda-27ac-4d75-8cb3-253f98d67727/6692-0 00:51:00.370 --> 00:51:04.506 One kind of trick we can play with the granite is we can 0df04eda-27ac-4d75-8cb3-253f98d67727/6692-1 00:51:04.506 --> 00:51:08.570 create a confined region like just about right here of. 0df04eda-27ac-4d75-8cb3-253f98d67727/6714-0 00:51:10.210 --> 00:51:13.709 A patch that's favorable for rupture, whereas like the red to 0df04eda-27ac-4d75-8cb3-253f98d67727/6714-1 00:51:13.709 --> 00:51:17.038 yellow and then the purple over here are not favorable for 0df04eda-27ac-4d75-8cb3-253f98d67727/6714-2 00:51:17.038 --> 00:51:17.490 rupture. 0df04eda-27ac-4d75-8cb3-253f98d67727/6728-0 00:51:19.210 --> 00:51:23.127 Just because of a Poisson effect within the granite blocks and I 0df04eda-27ac-4d75-8cb3-253f98d67727/6728-1 00:51:23.127 --> 00:51:23.730 have done. 0df04eda-27ac-4d75-8cb3-253f98d67727/6765-0 00:51:25.570 --> 00:51:29.459 Just in playing around, it's not published or anything, but where 0df04eda-27ac-4d75-8cb3-253f98d67727/6765-1 00:51:29.459 --> 00:51:33.055 I if if the Blues and Greens are favorable for rupture, what 0df04eda-27ac-4d75-8cb3-253f98d67727/6765-2 00:51:33.055 --> 00:51:36.650 happens if I inject directly into the middle of that region? 0df04eda-27ac-4d75-8cb3-253f98d67727/6771-0 00:51:37.010 --> 00:51:39.130 Versus what happens when I inject over here at the orange? 0df04eda-27ac-4d75-8cb3-253f98d67727/6786-0 00:51:40.690 --> 00:51:43.393 And kind of interestingly, it's not super repeatable, but there 0df04eda-27ac-4d75-8cb3-253f98d67727/6786-1 00:51:43.393 --> 00:51:44.450 are a lot of cases where. 0df04eda-27ac-4d75-8cb3-253f98d67727/6820-0 00:51:46.210 --> 00:51:50.491 The like red through yellow will start to creep and it'll load up 0df04eda-27ac-4d75-8cb3-253f98d67727/6820-1 00:51:50.491 --> 00:51:54.318 this favorable blue and green region and then it'll create 0df04eda-27ac-4d75-8cb3-253f98d67727/6820-2 00:51:54.318 --> 00:51:58.015 actually pretty big seismic event. Whereas when I inject 0df04eda-27ac-4d75-8cb3-253f98d67727/6820-3 00:51:58.015 --> 00:52:00.610 into this blue-green favourable region. 0df04eda-27ac-4d75-8cb3-253f98d67727/6824-0 00:52:01.530 --> 00:52:03.090 It creeps and relieves all the stress. 0df04eda-27ac-4d75-8cb3-253f98d67727/6838-0 00:52:04.610 --> 00:52:08.011 And so you actually get a smaller event which not super 0df04eda-27ac-4d75-8cb3-253f98d67727/6838-1 00:52:08.011 --> 00:52:09.530 repeatable not published. 0df04eda-27ac-4d75-8cb3-253f98d67727/6843-0 00:52:09.530 --> 00:52:10.770 Take this all with a grain of salt. 0df04eda-27ac-4d75-8cb3-253f98d67727/6849-0 00:52:11.690 --> 00:52:13.810 But that was kind of a cool, like, counterintuitive. 0df04eda-27ac-4d75-8cb3-253f98d67727/6851-0 00:52:16.010 --> 00:52:16.210 Yeah. 0df04eda-27ac-4d75-8cb3-253f98d67727/6857-0 00:52:17.590 --> 00:52:19.030 Everything for the most part. 0df04eda-27ac-4d75-8cb3-253f98d67727/6874-0 00:52:19.030 --> 00:52:21.863 What I've shown is after those Poisson stresses have been 0df04eda-27ac-4d75-8cb3-253f98d67727/6874-1 00:52:21.863 --> 00:52:24.550 relieved, so everything is as uniform as I can get it. 0df04eda-27ac-4d75-8cb3-253f98d67727/6881-0 00:52:35.610 --> 00:52:37.010 The question is what happened to E1? 0df04eda-27ac-4d75-8cb3-253f98d67727/6883-0 00:52:37.010 --> 00:52:38.290 There's also an E8. 0df04eda-27ac-4d75-8cb3-253f98d67727/6908-0 00:52:39.850 --> 00:52:43.541 So this is from what I was saying where I put the talc 0df04eda-27ac-4d75-8cb3-253f98d67727/6908-1 00:52:43.541 --> 00:52:47.770 patches at the end. So E one and E8 were on the creeping like. 0df04eda-27ac-4d75-8cb3-253f98d67727/6918-0 00:52:51.290 --> 00:52:54.357 Materially imposed creeping regions unaffected by fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/6918-1 00:52:54.357 --> 00:52:54.850 pressure. 0df04eda-27ac-4d75-8cb3-253f98d67727/6945-0 00:52:55.170 --> 00:52:58.205 And that was just I took them off because they don't make a 0df04eda-27ac-4d75-8cb3-253f98d67727/6945-1 00:52:58.205 --> 00:53:01.341 lot of sense within the context of what we're looking at, but 0df04eda-27ac-4d75-8cb3-253f98d67727/6945-2 00:53:01.341 --> 00:53:04.073 they were useful for me experimentally to confirm how 0df04eda-27ac-4d75-8cb3-253f98d67727/6945-3 00:53:04.073 --> 00:53:05.490 everything was being loaded. 0df04eda-27ac-4d75-8cb3-253f98d67727/6964-0 00:53:21.700 --> 00:53:24.414 Yes. So the question is how to identify fluid versus sheer 0df04eda-27ac-4d75-8cb3-253f98d67727/6964-1 00:53:24.414 --> 00:53:26.300 triggered events in the natural setting. 0df04eda-27ac-4d75-8cb3-253f98d67727/6981-0 00:53:27.850 --> 00:53:31.557 So one way I've heard of is swarmy versus not swarmy and 0df04eda-27ac-4d75-8cb3-253f98d67727/6981-1 00:53:31.557 --> 00:53:34.810 kind of looking at some of those characteristics. 0df04eda-27ac-4d75-8cb3-253f98d67727/7007-0 00:53:36.850 --> 00:53:39.524 I have not spent a lot of time on it, but I think one thing 0df04eda-27ac-4d75-8cb3-253f98d67727/7007-1 00:53:39.524 --> 00:53:42.333 that will be cool to do is put get a little bit more of ground 0df04eda-27ac-4d75-8cb3-253f98d67727/7007-2 00:53:42.333 --> 00:53:42.690 motions. 0df04eda-27ac-4d75-8cb3-253f98d67727/7021-0 00:53:42.690 --> 00:53:45.309 I haven't really done a thorough comparison of ground motions 0df04eda-27ac-4d75-8cb3-253f98d67727/7021-1 00:53:45.309 --> 00:53:47.970 between fluid pressure or fluid triggered and shear triggered. 0df04eda-27ac-4d75-8cb3-253f98d67727/7025-0 00:53:49.690 --> 00:53:50.970 So hopefully in the next. 0df04eda-27ac-4d75-8cb3-253f98d67727/7030-0 00:53:51.710 --> 00:53:52.590 Two years at least. 0df04eda-27ac-4d75-8cb3-253f98d67727/7033-0 00:53:52.590 --> 00:53:54.190 Try and play around with that a little bit more. 0df04eda-27ac-4d75-8cb3-253f98d67727/7042-0 00:53:57.690 --> 00:53:59.730 I don't have much of A better answer for that than. 0df04eda-27ac-4d75-8cb3-253f98d67727/7046-0 00:54:06.110 --> 00:54:07.310 You get a second shot later. 0df04eda-27ac-4d75-8cb3-253f98d67727/7049-0 00:54:09.410 --> 00:54:10.050 Follow up on this. 0df04eda-27ac-4d75-8cb3-253f98d67727/7060-0 00:54:10.520 --> 00:54:15.069 Previous question for the swarming events in your lab 0df04eda-27ac-4d75-8cb3-253f98d67727/7060-1 00:54:15.069 --> 00:54:16.080 simulations. 0df04eda-27ac-4d75-8cb3-253f98d67727/7078-0 00:54:17.650 --> 00:54:22.857 There was much more a seismic slip relative to the, say, the 0df04eda-27ac-4d75-8cb3-253f98d67727/7078-1 00:54:22.857 --> 00:54:24.650 seismic event itself. 0df04eda-27ac-4d75-8cb3-253f98d67727/7082-0 00:54:24.810 --> 00:54:29.090 So the a seismic versus a seismic moment. 0df04eda-27ac-4d75-8cb3-253f98d67727/7098-0 00:54:30.770 --> 00:54:34.738 Could be a potentially distinguishing factor and also 0df04eda-27ac-4d75-8cb3-253f98d67727/7098-1 00:54:34.738 --> 00:54:37.090 relate to predictability or not. 0df04eda-27ac-4d75-8cb3-253f98d67727/7100-0 00:54:39.730 --> 00:54:40.170 Earthquake. 0df04eda-27ac-4d75-8cb3-253f98d67727/7129-0 00:54:40.970 --> 00:54:44.334 Yeah. So one of the comments was that in the Swarmy case and in 0df04eda-27ac-4d75-8cb3-253f98d67727/7129-1 00:54:44.334 --> 00:54:47.645 the Floyd Trigger case, there's a lot more a seismic slip than 0df04eda-27ac-4d75-8cb3-253f98d67727/7129-2 00:54:47.645 --> 00:54:49.170 in the shared triggered case. 0df04eda-27ac-4d75-8cb3-253f98d67727/7135-0 00:54:49.170 --> 00:54:51.890 I'm gonna turn that question back around on you all. 0df04eda-27ac-4d75-8cb3-253f98d67727/7142-0 00:54:52.450 --> 00:54:53.730 Can we measure that in the earth? 0df04eda-27ac-4d75-8cb3-253f98d67727/7150-0 00:54:53.850 --> 00:54:56.450 Cuz I do think that would be a really good way to tell. 0df04eda-27ac-4d75-8cb3-253f98d67727/7155-0 00:54:57.970 --> 00:54:59.250 Fluid triggered versus shared triggering. 0df04eda-27ac-4d75-8cb3-253f98d67727/7168-0 00:55:00.930 --> 00:55:03.751 Home intensures have been used, but you need a really good 0df04eda-27ac-4d75-8cb3-253f98d67727/7168-1 00:55:03.751 --> 00:55:05.090 network to show the opening. 0df04eda-27ac-4d75-8cb3-253f98d67727/7170-0 00:55:08.060 --> 00:55:08.460 OK. 0df04eda-27ac-4d75-8cb3-253f98d67727/7172-0 00:55:09.750 --> 00:55:10.550 Someone added that. 0df04eda-27ac-4d75-8cb3-253f98d67727/7188-0 00:55:12.090 --> 00:55:14.869 You need a really good network to be able to get the moment 0df04eda-27ac-4d75-8cb3-253f98d67727/7188-1 00:55:14.869 --> 00:55:16.490 tensors to get the opening verses. 0df04eda-27ac-4d75-8cb3-253f98d67727/7191-0 00:55:18.130 --> 00:55:19.010 Sheer moments. 0df04eda-27ac-4d75-8cb3-253f98d67727/7194-0 00:55:20.610 --> 00:55:21.690 Just to add on that. 0df04eda-27ac-4d75-8cb3-253f98d67727/7206-0 00:55:28.450 --> 00:55:33.160 Meters or surface geodetic measurements can address the A 0df04eda-27ac-4d75-8cb3-253f98d67727/7206-1 00:55:33.160 --> 00:55:33.810 seismic. 0df04eda-27ac-4d75-8cb3-253f98d67727/7207-0 00:55:35.450 --> 00:55:35.770 Or. 0df04eda-27ac-4d75-8cb3-253f98d67727/7220-0 00:55:36.510 --> 00:55:40.614 Most earthquakes for which we have observations at any a 0df04eda-27ac-4d75-8cb3-253f98d67727/7220-1 00:55:40.614 --> 00:55:41.910 seismic precursor. 0df04eda-27ac-4d75-8cb3-253f98d67727/7230-0 00:55:43.530 --> 00:55:46.720 But it would be interesting to have a similar kind of 0df04eda-27ac-4d75-8cb3-253f98d67727/7230-1 00:55:46.720 --> 00:55:47.370 experiment. 0df04eda-27ac-4d75-8cb3-253f98d67727/7242-0 00:55:56.750 --> 00:56:00.217 It was also pointed out that there are bore holes, strain 0df04eda-27ac-4d75-8cb3-253f98d67727/7242-1 00:56:00.217 --> 00:56:02.070 meters and surface deformation. 0df04eda-27ac-4d75-8cb3-253f98d67727/7243-0 00:56:02.070 --> 00:56:02.790 Was that the other one? 0df04eda-27ac-4d75-8cb3-253f98d67727/7265-0 00:56:04.330 --> 00:56:07.396 Geodetic measurements that can get at a seismic slip in some 0df04eda-27ac-4d75-8cb3-253f98d67727/7265-1 00:56:07.396 --> 00:56:10.664 cases, but kind of the key like the caveat being like the A size 0df04eda-27ac-4d75-8cb3-253f98d67727/7265-2 00:56:10.664 --> 00:56:11.770 slope is really small. 0df04eda-27ac-4d75-8cb3-253f98d67727/7273-0 00:56:11.770 --> 00:56:15.029 It's a really small component, so it's harder to measure that 0df04eda-27ac-4d75-8cb3-253f98d67727/7273-1 00:56:15.029 --> 00:56:15.450 as well. 0df04eda-27ac-4d75-8cb3-253f98d67727/7280-0 00:56:19.270 --> 00:56:21.990 Yeah. Well, I was gonna move to the to the post doc part. 0df04eda-27ac-4d75-8cb3-253f98d67727/7291-0 00:56:23.530 --> 00:56:26.374 The end of the talk you brought up repeating events and in 0df04eda-27ac-4d75-8cb3-253f98d67727/7291-1 00:56:26.374 --> 00:56:27.290 particular for the. 0df04eda-27ac-4d75-8cb3-253f98d67727/7315-0 00:56:33.750 --> 00:56:37.783 You don't see any sort of systematic shared recurrence 0df04eda-27ac-4d75-8cb3-253f98d67727/7315-1 00:56:37.783 --> 00:56:42.183 interval among the different pairs you've identified, but I 0df04eda-27ac-4d75-8cb3-253f98d67727/7315-2 00:56:42.183 --> 00:56:46.950 wonder what other variables you might expect current time to be. 0df04eda-27ac-4d75-8cb3-253f98d67727/7323-0 00:56:48.530 --> 00:56:49.650 Related correlated with here. 0df04eda-27ac-4d75-8cb3-253f98d67727/7342-0 00:56:49.650 --> 00:56:53.311 So for example, is the recurrence time different or 0df04eda-27ac-4d75-8cb3-253f98d67727/7342-1 00:56:53.311 --> 00:56:57.184 systematically related to the amount of pressure fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/7342-2 00:56:57.184 --> 00:56:59.930 pressure that has been applied so far? 0df04eda-27ac-4d75-8cb3-253f98d67727/7353-0 00:56:59.930 --> 00:57:02.885 And if you can look at that or related to the magnitude of 0df04eda-27ac-4d75-8cb3-253f98d67727/7353-1 00:57:02.885 --> 00:57:05.290 magnitude of the events or something like that? 0df04eda-27ac-4d75-8cb3-253f98d67727/7357-0 00:57:06.640 --> 00:57:07.440 Looking at something. 0df04eda-27ac-4d75-8cb3-253f98d67727/7371-0 00:57:09.160 --> 00:57:12.595 More than just two event, you know, if you look at a set of 0df04eda-27ac-4d75-8cb3-253f98d67727/7371-1 00:57:12.595 --> 00:57:15.000 repeaters more than just two, do you see? 0df04eda-27ac-4d75-8cb3-253f98d67727/7373-0 00:57:16.890 --> 00:57:17.170 The same. 0df04eda-27ac-4d75-8cb3-253f98d67727/7376-0 00:57:23.910 --> 00:57:25.230 OK, the question was. 0df04eda-27ac-4d75-8cb3-253f98d67727/7383-0 00:57:26.770 --> 00:57:28.930 To try and summarize, it is looking at the repeaters. 0df04eda-27ac-4d75-8cb3-253f98d67727/7400-0 00:57:30.610 --> 00:57:33.879 I find a lot of pairs and so there's no like set recurrence 0df04eda-27ac-4d75-8cb3-253f98d67727/7400-1 00:57:33.879 --> 00:57:34.370 interval. 0df04eda-27ac-4d75-8cb3-253f98d67727/7410-0 00:57:34.730 --> 00:57:37.690 So what does the recurrence interval related to? And if 0df04eda-27ac-4d75-8cb3-253f98d67727/7410-1 00:57:37.690 --> 00:57:39.170 there was one that was like? 0df04eda-27ac-4d75-8cb3-253f98d67727/7414-0 00:57:40.810 --> 00:57:42.090 Went throughout the entire duration. 0df04eda-27ac-4d75-8cb3-253f98d67727/7419-0 00:57:43.690 --> 00:57:45.210 Kind of. What would be expect. 0df04eda-27ac-4d75-8cb3-253f98d67727/7427-0 00:57:46.810 --> 00:57:48.650 Ed, if you have a fault that's being loaded. 0df04eda-27ac-4d75-8cb3-253f98d67727/7435-0 00:57:51.370 --> 00:57:52.290 A creeping region. 0df04eda-27ac-4d75-8cb3-253f98d67727/7451-0 00:57:52.290 --> 00:57:55.826 Your recurrence interval will be regular and it will be 0df04eda-27ac-4d75-8cb3-253f98d67727/7451-1 00:57:55.826 --> 00:57:58.290 correlated to the loading rate, right? 0df04eda-27ac-4d75-8cb3-253f98d67727/7464-0 00:57:58.290 --> 00:58:00.781 So if the same patch is being loaded really fast, you have a 0df04eda-27ac-4d75-8cb3-253f98d67727/7464-1 00:58:00.781 --> 00:58:02.170 really short recurrence interval. 0df04eda-27ac-4d75-8cb3-253f98d67727/7482-0 00:58:02.450 --> 00:58:05.341 And if it's being loaded really slowly, you have a long 0df04eda-27ac-4d75-8cb3-253f98d67727/7482-1 00:58:05.341 --> 00:58:08.181 recurrence interval, whether that's from fluid, from a 0df04eda-27ac-4d75-8cb3-253f98d67727/7482-2 00:58:08.181 --> 00:58:09.730 seismic slip tectonic loading. 0df04eda-27ac-4d75-8cb3-253f98d67727/7493-0 00:58:11.290 --> 00:58:14.410 Taking that out is a little bit harder to understand. 0df04eda-27ac-4d75-8cb3-253f98d67727/7495-0 00:58:14.410 --> 00:58:15.370 Is my understanding. 0df04eda-27ac-4d75-8cb3-253f98d67727/7499-0 00:58:17.770 --> 00:58:18.410 I don't. 0df04eda-27ac-4d75-8cb3-253f98d67727/7507-0 00:58:18.410 --> 00:58:19.770 So I'm still running the full catalog. 0df04eda-27ac-4d75-8cb3-253f98d67727/7514-0 00:58:19.770 --> 00:58:22.170 This is only six months out of like 48 months. 0df04eda-27ac-4d75-8cb3-253f98d67727/7523-0 00:58:23.360 --> 00:58:26.080 But in these six months, I don't really see anything. 0df04eda-27ac-4d75-8cb3-253f98d67727/7526-0 00:58:27.610 --> 00:58:28.250 Recurring regularly. 0df04eda-27ac-4d75-8cb3-253f98d67727/7530-0 00:58:29.850 --> 00:58:30.490 So I don't know. 0df04eda-27ac-4d75-8cb3-253f98d67727/7551-0 00:58:32.690 --> 00:58:35.997 Instead, if you ever basically repeaters with like an hour 0df04eda-27ac-4d75-8cb3-253f98d67727/7551-1 00:58:35.997 --> 00:58:39.193 duration, perhaps that is something related to the fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/7551-2 00:58:39.193 --> 00:58:40.090 pressure, right? 0df04eda-27ac-4d75-8cb3-253f98d67727/7567-0 00:58:40.090 --> 00:58:42.829 And so maybe that's why it stops, because your fluid 0df04eda-27ac-4d75-8cb3-253f98d67727/7567-1 00:58:42.829 --> 00:58:45.672 pressure kind of affects it enough that it's no longer 0df04eda-27ac-4d75-8cb3-253f98d67727/7567-2 00:58:45.672 --> 00:58:46.810 really the same patch. 0df04eda-27ac-4d75-8cb3-253f98d67727/7570-0 00:58:48.090 --> 00:58:49.650 This is this is all speculation. 0df04eda-27ac-4d75-8cb3-253f98d67727/7585-0 00:58:51.250 --> 00:58:53.941 Or that that region is no longer get what that could mean is that 0df04eda-27ac-4d75-8cb3-253f98d67727/7585-1 00:58:53.941 --> 00:58:55.410 region is no longer getting loaded. 0df04eda-27ac-4d75-8cb3-253f98d67727/7595-0 00:58:56.610 --> 00:58:59.570 I see it pretty uniformly for different magnitudes. 0df04eda-27ac-4d75-8cb3-253f98d67727/7611-0 00:59:00.050 --> 00:59:04.365 So even like small magnitudes like this purple one versus this 0df04eda-27ac-4d75-8cb3-253f98d67727/7611-1 00:59:04.365 --> 00:59:05.530 pink one up here. 0df04eda-27ac-4d75-8cb3-253f98d67727/7620-0 00:59:06.290 --> 00:59:11.292 So like magnitude under one to magnitude almost two, I still 0df04eda-27ac-4d75-8cb3-253f98d67727/7620-1 00:59:11.292 --> 00:59:12.850 see like happening. 0df04eda-27ac-4d75-8cb3-253f98d67727/7624-0 00:59:14.410 --> 00:59:15.210 Few hours apart. 0df04eda-27ac-4d75-8cb3-253f98d67727/7628-0 00:59:19.600 --> 00:59:20.640 I don't know. 0df04eda-27ac-4d75-8cb3-253f98d67727/7631-0 00:59:20.640 --> 00:59:22.120 Talk more about it if you have other ideas. 0df04eda-27ac-4d75-8cb3-253f98d67727/7639-0 00:59:30.160 --> 00:59:32.320 Not then. Go and thank Sarah Beth one more time. 0df04eda-27ac-4d75-8cb3-253f98d67727/7643-0 00:59:35.350 --> 00:59:37.750 Thank you.