WEBVTT 00:00:02.381 --> 00:00:05.382 Okay now that you know a little bit about ground water systems. 00:00:05.382 --> 00:00:07.430 Some of the vocabulary associated with them. 00:00:07.430 --> 00:00:10.154 Let's talk about groundwater flow. 00:00:10.154 --> 00:00:14.291 Groundwater is usually not stagnant, okay, it's usually moving. 00:00:14.291 --> 00:00:17.395 It isn't moving fast like a stream but it is usually moving, 00:00:17.395 --> 00:00:21.716 and typical flow rates would be on the order of about a half a meter per day. 00:00:21.716 --> 00:00:26.388 It flows away from areas where it enters aquifers. 00:00:26.388 --> 00:00:31.743 Two places where water exits aquifers. 00:00:31.743 --> 00:00:37.879 We call places where water enters an aquifer recharge areas and places where water 00:00:37.879 --> 00:00:41.883 exits aquifers are referred to as discharge areas. 00:00:41.883 --> 00:00:46.764 So you can say that water flows from recharge areas to discharge areas, 00:00:46.991 --> 00:00:49.099 and that's what's shown on the slide. 00:00:49.393 --> 00:00:55.530 The blue lines depict groundwater flow paths and you can see that some of these 00:00:55.530 --> 00:00:57.404 flow paths are fairly short. 00:00:57.404 --> 00:01:02.809 The shortest ones, groundwater can flow along in a matter of days. 00:01:02.809 --> 00:01:09.247 Others, however, are quite long, uh, water can be isolated from the, um, 00:01:09.247 --> 00:01:13.402 from the surface and aquitards and aquifers for thousands of years, 00:01:13.402 --> 00:01:15.253 or even more. 00:01:15.253 --> 00:01:20.508 Some research, um, recently identified some groundwater that was at least as old 00:01:20.508 --> 00:01:28.484 as 1.5 billion years old, okay, and been isolated in the subsurface for that long, 00:01:28.484 --> 00:01:31.037 which is incredible. 00:01:31.037 --> 00:01:34.139 Okay so that-that would definitely be exceptional. 00:01:34.139 --> 00:01:40.546 So what controls the movement of rocks and sediment, well the equation that we use to 00:01:40.546 --> 00:01:45.719 describe the flow of water through coarse materials like sand was, uh, defined by this 00:01:45.719 --> 00:01:48.037 guy, Henry Darcy. 00:01:48.037 --> 00:01:53.209 And the equation that he used, or that he defined, is known as Darcy's Law. 00:01:53.209 --> 00:01:56.246 So at some point he must have asked a question, what the heck controls the 00:01:56.246 --> 00:01:59.298 movement of water through sand? 00:01:59.298 --> 00:02:03.752 And I imagine that we've all asked that question time or two. 00:02:03.752 --> 00:02:07.856 Although, he probably would've said it in French, cause he was, um, he was 00:02:07.856 --> 00:02:13.322 actually a French engineer, uh, just to give you a little historical context on 00:02:13.481 --> 00:02:15.056 this topic. 00:02:15.165 --> 00:02:18.837 Uh, he was an engineer and he lived 'bout the same period of time as 00:02:18.837 --> 00:02:20.720 Abraham Lincoln. 00:02:20.720 --> 00:02:24.158 During his life he was very famous for bringing a water distribution system to 00:02:24.158 --> 00:02:28.111 Dijon in 1840. 00:02:28.111 --> 00:02:31.799 Okay this was a big deal because very few places at the time had water 00:02:31.799 --> 00:02:33.318 distribution systems. 00:02:33.318 --> 00:02:38.389 Wasn't, it was also at this time that few places had sewer systems, okay. 00:02:38.389 --> 00:02:42.542 So if you were living in a city, a good reliable source of clean water was 00:02:42.542 --> 00:02:44.628 really important. 00:02:44.628 --> 00:02:49.534 Um, for reference, Paris didn't have, oops, Paris didn't have a water 00:02:49.534 --> 00:02:55.690 distribution system until 1865, a full 20 years after the little city of Dijon 00:02:55.690 --> 00:03:00.178 um, got it's water distribution system. 00:03:00.178 --> 00:03:04.298 It wasn't until very late into his life, 2 years before he died, that he carried 00:03:04.298 --> 00:03:08.669 out the experiments that perhaps he is best known for today. 00:03:08.669 --> 00:03:13.191 He performed the experiments in hospital, that might seem like, y'know a really 00:03:13.191 --> 00:03:17.345 odd choice, at the time there probably weren't as many places where, uh, that 00:03:17.345 --> 00:03:21.081 were, y'know, convenient for setting up experiments. 00:03:21.081 --> 00:03:27.557 The experiment that he performed, uh, he published results in his report in 1856, 00:03:27.557 --> 00:03:32.061 and uh, they were just described in a couple of pages in the very back of the 00:03:32.061 --> 00:03:38.205 report, I think one of the appendices for the, um, for the report. 00:03:38.205 --> 00:03:41.493 Uh, so it was very much just an afterthought, but it turned out to be a 00:03:41.493 --> 00:03:45.111 very, uh, a really useful important piece of work. 00:03:45.111 --> 00:03:49.765 So what we're gonna do now is walk through some aspects of Darcy's experiment. 00:03:49.765 --> 00:03:53.757 This will help illustrate some basic controls on the movement of water through porous 00:03:53.757 --> 00:03:57.594 medium, and also the process of science, how you can apply some basic reasoning, 00:03:57.594 --> 00:04:03.016 collect data, and then figure out relationships. 00:04:03.016 --> 00:04:08.821 So what Darcy did was, uh, set up a tube that contained some sand, and that 00:04:08.821 --> 00:04:13.827 tube had some smaller tubes in it called manometers poking into the, near the in 00:04:13.827 --> 00:04:16.146 flow and out flow end, 00:04:16.146 --> 00:04:22.161 and he'd float water through the sand tube and, uh, observed how different variables 00:04:22.161 --> 00:04:24.889 affected flow. 00:04:26.249 --> 00:04:31.955 Hydraulic head is the name given to the height at water rises and the manometers 00:04:31.955 --> 00:04:35.726 relative to some arbitrary data. 00:04:35.726 --> 00:04:39.845 In natural environments we would typically pick sea level to be the datum. 00:04:39.845 --> 00:04:43.366 In a lab experiment you might just pick the bench top where you're carrying out 00:04:43.366 --> 00:04:46.752 the experiment, because it's more convenient. 00:04:46.752 --> 00:04:52.707 Hydraulic head is the sum of two components, the height that water rises in 00:04:52.707 --> 00:04:58.430 the tube as a result of water pressure, we call that pressure head, and then the 00:04:58.430 --> 00:05:04.368 height that the water has because of how far the tube is above the datum. 00:05:04.368 --> 00:05:08.226 Okay, so that would be elevation head. 00:05:10.897 --> 00:05:19.138 What Darcy observed is that water always flows from high head to low head, okay, 00:05:19.138 --> 00:05:22.708 and that the rate of flow through that sand tube is proportional to the 00:05:22.708 --> 00:05:26.461 difference in hydraulic head measured between the manometers, 00:05:26.461 --> 00:05:31.617 in other words, Delta H, uh, the difference between this-this hydraulic 00:05:31.617 --> 00:05:35.970 head and this hydraulic head, is Delta H right here. 00:05:35.970 --> 00:05:38.689 Okay, how about column area? 00:05:38.689 --> 00:05:40.724 How would this affect flow? 00:05:40.724 --> 00:05:43.628 Well this is really-really straight forward, basically if you were to put a 00:05:43.628 --> 00:05:50.811 partition in the column such that the area available to flow, uh, was divided into 00:05:50.811 --> 00:05:56.899 the flow rate, uh, through each half of the sand tube, would be equal to one half 00:05:56.899 --> 00:06:03.823 of the total flow, okay, so from this, Darcy concluded that the rate of flow is 00:06:03.823 --> 00:06:08.980 proportional to the area of sand available. 00:06:10.630 --> 00:06:14.313 Lastly, what about the length of the tube. 00:06:14.313 --> 00:06:19.768 Well Darcy figured out that if you keep the head difference between each end of 00:06:19.768 --> 00:06:25.958 the tubes the same but you lengthen the tube, it effects the flow rate, okay. 00:06:25.958 --> 00:06:33.025 Uh, so imagine, in fact it causes flow rate to decrease, imagine that this sand 00:06:33.025 --> 00:06:38.982 tube is one foot long, and that the difference in head is 6 inches. 00:06:38.982 --> 00:06:40.931 Okay, that's a pretty steep change in 00:06:41.018 --> 00:06:44.547 hydraulic head over the-over the length of that tube, right. 00:06:44.818 --> 00:06:48.239 And so water would want to flow through that fairly quickly. 00:06:48.239 --> 00:06:53.594 But if the tube were 10 feet long that 6 inch drop over 10 feet isn't nearly 00:06:53.594 --> 00:06:55.313 as steep. 00:06:55.313 --> 00:06:58.615 In that case the water wouldn't move through as fast, okay. 00:06:58.615 --> 00:07:05.317 So from this we can conclude that, um, the length, the flow through the tube is 00:07:05.317 --> 00:07:08.087 inversely proportional to length. 00:07:08.087 --> 00:07:15.272 In other words, if all else is the same, as length increases, flow decreases. 00:07:18.897 --> 00:07:24.018 Okay, so these 3 lines just summarized what we just discussed flow is directly 00:07:24.018 --> 00:07:28.540 proportional to the, uh, difference in hydraulic head between each end of the 00:07:28.540 --> 00:07:33.411 tube, it's proportional to the area of the column, and it's inversely proportional 00:07:33.411 --> 00:07:35.514 to the length of the column. 00:07:35.514 --> 00:07:40.000 Okay, this symbol right here is, uh, means proportional, right. 00:07:40.000 --> 00:07:43.764 So this means inversely proportional, because 1 over L. 00:07:43.835 --> 00:07:48.806 So if we put this together, okay, this is what we get. 00:07:48.806 --> 00:07:55.564 Now we can replace this proportional sign, with a sign, with an equal sign, by adding 00:07:55.564 --> 00:08:02.754 a constant of proportionality, 'K', and when we do that, this is what we 00:08:02.754 --> 00:08:05.041 get, okay. 00:08:05.041 --> 00:08:09.428 And if we just rearrange this a little bit, we end up with this form of the 00:08:09.428 --> 00:08:13.649 equation, and that is Darcy's Law. 00:08:13.649 --> 00:08:16.384 So it really is not that complicated. 00:08:16.384 --> 00:08:19.939 If you understood each part, each of the parts that we went through in the previous 00:08:19.939 --> 00:08:24.335 slides, this just combines them all into one equation. 00:08:24.335 --> 00:08:28.156 Um, one of the things that might seem a little mysterious is this 'K'. 00:08:28.156 --> 00:08:30.442 What the heck is 'K'? 00:08:30.442 --> 00:08:34.930 Well, 'K' is hydraulic conductivity. 00:08:34.930 --> 00:08:37.124 So let me explain this a little bit. 00:08:37.124 --> 00:08:42.391 Um, basically you can think of it as, y'know, basically the same thing as 00:08:42.391 --> 00:08:47.607 permeability, it's a little bit different, but think about it as permeability. 00:08:47.607 --> 00:08:54.865 Aquifers have high hydraulic conductivity, um, because they can transmit water 00:08:54.865 --> 00:09:00.621 relatively easily, water can flow through them, they're fairly permeable, right. 00:09:00.621 --> 00:09:06.126 Aquitards have low hydraulic conductivity they're relatively impermeable. 00:09:06.126 --> 00:09:09.947 Water does not flow through them very easily. 00:09:09.947 --> 00:09:14.842 In reality, hydraulic conductivity is a little bit more then permeability. 00:09:14.842 --> 00:09:18.129 It combines permeability with properties of the fluid. 00:09:18.129 --> 00:09:22.532 But in any case just think about it as a measure of how easily water can flow 00:09:22.532 --> 00:09:26.220 through a porous meeting. 00:09:26.220 --> 00:09:30.256 Okay, so how do geoscientists use Darcy's Law and this information that I just 00:09:30.256 --> 00:09:33.545 gave you? 00:09:33.545 --> 00:09:38.151 Essentially you can think of wells, uh, as the same thing as those manometers. 00:09:38.151 --> 00:09:42.672 They fill the same roll as the manometers I showed you in Darcy's experiment. 00:09:42.672 --> 00:09:47.793 So we can go out and measure the elevation of water in a well, and that tells us the 00:09:47.793 --> 00:09:54.566 hydraulic head, where that water, where that well is open and an aquifer. 00:09:54.566 --> 00:10:01.189 Okay, so, so we can use these measurements to help determine what direction ground 00:10:01.189 --> 00:10:06.978 water is flowing in an aquifer, okay, so in the, uh, in the illustration shown here, 00:10:06.978 --> 00:10:11.094 this simple illustration, we would conclude that ground water is flowing from the 00:10:11.094 --> 00:10:12.645 left to the right. 00:10:12.645 --> 00:10:14.214 Towards well B. 00:10:14.214 --> 00:10:18.418 Because hydraulic head, uh, decreases in that direction. 00:10:18.418 --> 00:10:27.008 Remember ground water always flows from high head to low head, okay. 00:10:27.008 --> 00:10:31.948 And we can use this to help understand flow rates, by assessing ground water 00:10:31.948 --> 00:10:36.319 flow and combining it with, uh, knowledge of geological properties of 00:10:36.319 --> 00:10:40.640 aquifers we can evaluate how much water is available in aquifers and how that 00:10:40.640 --> 00:10:46.163 changes over time, okay. 00:10:47.143 --> 00:10:48.561 How do we use this? 00:10:48.561 --> 00:10:49.829 How is this useful? 00:10:49.829 --> 00:10:53.967 Well given the extent to which we rely on ground water as a source of drinking 00:10:53.967 --> 00:10:58.580 water and irrigation water, this information is extremely important, 00:10:58.787 --> 00:11:03.244 because it helps us manage critical water sources more effectively. 00:11:04.161 --> 00:11:07.485 This is a huge, uh, this is a big deal. 00:11:07.835 --> 00:11:11.855 It's really important, these water sources are extremely important so we need to be 00:11:11.855 --> 00:11:14.058 able to manage them effectively. 00:11:14.058 --> 00:11:17.845 One of the examples, um, that I'm going to focus on in the le-in the next 00:11:17.845 --> 00:11:19.897 lecture, is shown here. 00:11:19.897 --> 00:11:22.516 It is the high planes aquifer. 00:11:22.516 --> 00:11:26.670 Okay, an aquifer that plays a vital role in sustaining human populations in the 00:11:26.670 --> 00:11:30.441 Great Plains, and an aquifer that's up against some serious challenges 00:11:30.441 --> 00:11:32.642 in the future. 00:11:32.642 --> 00:11:35.630 So I look forward to talking about that with you in more detail in the 00:11:35.630 --> 00:11:37.230 next lecture. 00:11:37.230 --> 00:11:39.790 Thank you for your attention.