1 00:00:05,830 --> 00:00:11,360 Welcome! My name is Hubert Savenije and I am a hydrologist. 2 00:00:11,360 --> 00:00:17,240 The most visible and most intriguing part of the hydrological cycle is the runoff. 3 00:00:17,240 --> 00:00:23,840 Every person has at some stage looked in fascination at flowing water, or been inspired by the 4 00:00:23,840 --> 00:00:28,920 beauty or violence of a stream 5 00:00:28,920 --> 00:00:35,410 Flowing water seems alive. And it is an inseparable part of our life. 6 00:00:35,410 --> 00:00:39,190 Water has been essential to create and support our societies 7 00:00:39,190 --> 00:00:45,220 and sometime it threatens it with its destructive force 8 00:00:45,220 --> 00:00:50,549 As we saw earlier, it took philosophers and scientists some time before they realised 9 00:00:50,549 --> 00:00:55,610 that river runoff is completely dependent on precipitation 10 00:00:55,610 --> 00:01:01,440 At first they thought that there was not enough precipitation to feed the rivers, but in fact 11 00:01:01,440 --> 00:01:03,479 there is a lot more than that. 12 00:01:03,479 --> 00:01:10,479 Globally, less than 40% of the precipitation leads to runoff. 13 00:01:11,120 --> 00:01:17,020 As precipitated moisture travels through the terrestrial cycle, it is stepwise partitioned 14 00:01:17,020 --> 00:01:20,030 into other fluxes. 15 00:01:20,030 --> 00:01:23,970 The first partitioning point is the surface. 16 00:01:23,970 --> 00:01:30,970 If rain falls on water or on saturated land, then it runs off directly to the open water. 17 00:01:31,130 --> 00:01:35,300 We call this saturation excess overland flow. 18 00:01:35,300 --> 00:01:38,159 Above land, rainfall is intercepted by: 19 00:01:38,159 --> 00:01:43,470 leaves, the litter on the ground and the ground itself (where it may pond) 20 00:01:43,470 --> 00:01:47,450 and from there it evaporates back to the atmosphere. 21 00:01:47,450 --> 00:01:53,110 The typical time scale of this process is between an hour and a day. 22 00:01:53,110 --> 00:02:00,110 If the ponding is large enough, water may flow overland and find its way to the stream. 23 00:02:00,430 --> 00:02:06,920 We call that infiltration excess overland flow, or Hortonian overland flow, after the 24 00:02:06,920 --> 00:02:10,039 great American hydrologist Horton 25 00:02:10,039 --> 00:02:15,280 This overland flow is very fast, with a time scale of hours. 26 00:02:15,280 --> 00:02:21,580 The remainder infiltrates into the soil, from where it can transpire or percolate into the 27 00:02:21,580 --> 00:02:24,200 groundwater. 28 00:02:25,300 --> 00:02:33,420 During a rainfall event, the soil can become so saturated that pockets of saturation occur 29 00:02:33,420 --> 00:02:37,940 under the ground at relatively shallow depth. 30 00:02:37,940 --> 00:02:43,130 If the terrain is sloped, then this sub-surface pocket may connect and generate subsurface 31 00:02:43,130 --> 00:02:47,760 runoff through a network of preferential channels. 32 00:02:47,760 --> 00:02:53,700 These channels have been created by the water itself, making use of root channels, animal 33 00:02:53,700 --> 00:02:56,590 burrows and fissures. 34 00:02:56,590 --> 00:03:05,060 In mountainous and hilly area, this is a dominant mechanism, which we call storage excess subsurface 35 00:03:05,060 --> 00:03:09,860 flow or shortly ‘interflow’ 36 00:03:09,860 --> 00:03:16,410 The water that percolates to the groundwater subsequently feeds the very slow groundwater 37 00:03:16,410 --> 00:03:20,989 flow, that sustains the base flow of the river. 38 00:03:20,989 --> 00:03:27,800 Finally, groundwater can be exchanged with neighbouring areas or may rise to the unsaturated 39 00:03:27,800 --> 00:03:32,069 soil by capillary rise. 40 00:03:32,069 --> 00:03:39,040 The many storages and thresholds in this system are the reason why the rainfall-runoff processes 41 00:03:39,040 --> 00:03:42,430 is highly non-linear, 42 00:03:42,430 --> 00:03:48,290 although the individual processes can often very well be described by linear processes, 43 00:03:48,290 --> 00:03:53,370 just like we saw with the groundwater seepage. 44 00:03:53,370 --> 00:04:00,370 So the fast surface runoff is the precipitation minus the interception and the infiltration 45 00:04:01,099 --> 00:04:06,959 The fast sub-surface runoff is the infiltration minus the transpiration, the soil evaporation 46 00:04:06,959 --> 00:04:09,450 and the percolation 47 00:04:09,450 --> 00:04:16,450 And the base flow equals the percolation minus the capillary rise 48 00:04:16,549 --> 00:04:21,310 It is hard to distinguish these different runoff components once the water has entered 49 00:04:21,310 --> 00:04:22,779 the river. 50 00:04:22,779 --> 00:04:29,779 But the water can reveal its origin when we look at its colour and composition. 51 00:04:30,319 --> 00:04:36,150 If it is very turbid, and flowing fast, then it stems from surface runoff. 52 00:04:36,150 --> 00:04:43,129 If it flows fast and is mostly clear, then it stems from rapid subsurface flow. 53 00:04:43,129 --> 00:04:50,129 If the water is clear and the flow is quiet, then it consists of seepage flow from GW 54 00:04:51,439 --> 00:04:56,749 From the chemical elements in the water, the isotope composition and the turbidity we can 55 00:04:56,749 --> 00:04:59,999 deduct the origin of the water, 56 00:04:59,999 --> 00:05:05,289 but also the time it spent in the catchment before it came to runoff 57 00:05:05,289 --> 00:05:09,509 But that goes beyond this introductory course. 58 00:05:09,900 --> 00:05:14,940 Depending on the climate and the physical properties of the landscapes in the catchment, 59 00:05:14,949 --> 00:05:18,159 rivers have different runoff signatures 60 00:05:18,159 --> 00:05:22,879 Here we see clearly different signatures from two neighbouring catchments 61 00:05:23,580 --> 00:05:29,400 On average, the Rhine has about ten times more discharge than the Meuse 62 00:05:30,039 --> 00:05:36,729 Not only is the runoff of the Rhine larger, it is also less variable over the year 63 00:05:36,729 --> 00:05:39,939 What makes these patterns so different? 64 00:05:39,939 --> 00:05:42,039 Is it climate? 65 00:05:42,039 --> 00:05:47,719 “It’s the landscape, the climate is not so different” 66 00:05:47,719 --> 00:05:53,089 The mountainous part of the Rhine, with its snow cover and glaciers makes that the runoff 67 00:05:53,089 --> 00:05:58,650 during the dry summer months is still substantial, whereas the runoff of the Meuse in de dry 68 00:05:58,650 --> 00:06:02,180 summer months is very low. 69 00:06:02,180 --> 00:06:05,479 But climate can be very important. 70 00:06:05,479 --> 00:06:12,479 Whether a river is ephemeral, intermittent or perennial depends primarily on the climate 71 00:06:14,499 --> 00:06:20,270 Traditionally we measure discharge by a current meter at a certain position in the cross-section 72 00:06:20,270 --> 00:06:20,759 of a river 73 00:06:20,759 --> 00:06:27,759 We find the total discharge by integration of all these points over the cross-section 74 00:06:28,080 --> 00:06:31,710 This is a lot of work, although it is fun 75 00:06:31,710 --> 00:06:34,610 As you can see 76 00:06:34,610 --> 00:06:41,510 But although its is great fun doing it in this way, it is also a bit old fashioned. 77 00:06:41,860 --> 00:06:47,780 Nowadays we use Doppler instruments in the stream that are able to map the entire velocity field 78 00:06:47,789 --> 00:06:53,529 or we make use of movies from iPhones to infer the discharge from the flow pattern observed 79 00:06:53,529 --> 00:06:55,409 from the top 80 00:06:55,409 --> 00:07:00,999 But this is something for an advanced course 81 00:07:00,999 --> 00:07:08,759 We use discharge measurements to compose rating curves, linking the water level to the discharge 82 00:07:09,460 --> 00:07:15,789 The relation between depth h and discharge Q is a power function which plots a straight 83 00:07:15,789 --> 00:07:22,610 line on double log paper provided we have the zero of the reading right: the so-called 84 00:07:22,610 --> 00:07:29,610 h0, or the gauge reading when the discharge is zero 85 00:07:29,689 --> 00:07:36,119 These rating curves are expressions of the Manning formula for ‘uniform’ flow. 86 00:07:36,119 --> 00:07:40,939 The power function of the rating curve completely matches the Manning formula below. 87 00:07:41,320 --> 00:07:47,440 The Manning formula consists of two parts: the first part is a constant for the given 88 00:07:47,610 --> 00:07:52,830 section and the second part depends on the water level h 89 00:07:52,830 --> 00:07:59,429 The width, the depth and the hydraulic radius R all depend on the depth, whereas the roughness 90 00:07:59,429 --> 00:08:04,549 coefficient n and the slope S does not 91 00:08:05,060 --> 00:08:13,040 Interestingly, the water level dependent part purely depends on the geometry of the cross-section 92 00:08:13,050 --> 00:08:17,599 Stevens developed a very smart way of combining the two. 93 00:08:17,599 --> 00:08:24,599 The first part (the curve), one can derive from a topographical survey of the cross-section. 94 00:08:25,219 --> 00:08:32,219 This curve can be extrapolated as far as necessary, as high as the water level may go. 95 00:08:33,060 --> 00:08:38,060 The other part, the line, required a couple of discharge measurements, 96 00:08:38,060 --> 00:08:43,990 but because it is a straight line, it requires only a limited number of points 97 00:08:43,990 --> 00:08:50,990 And subsequently we can use that line to combine with the curve 98 00:08:52,020 --> 00:08:57,490 Have a look at the example to see how it works. 99 00:08:57,490 --> 00:09:04,860 Rating curves can have peculiarities, On double log paper, they should plot on a straight line, 100 00:09:04,860 --> 00:09:09,090 (if you select the right H0) 101 00:09:09,090 --> 00:09:16,090 but they can show kinks (inflections) in the curves, which can bend up as well as down. 102 00:09:17,560 --> 00:09:22,300 Here you see a hand-drawn rating curve made in the 1980’s 103 00:09:22,300 --> 00:09:25,460 of the Limpopo river in Mozambique. 104 00:09:25,460 --> 00:09:34,860 The dots with the years were observations during big floods, when the whole of the flood 105 00:09:34,870 --> 00:09:38,200 plain of the river was covered with water. 106 00:09:38,200 --> 00:09:43,440 The inflection point is at the water level where the river starts to fill the floodplain 107 00:09:43,560 --> 00:09:49,380 and where the flood plain offers an additional and much wider channel 108 00:09:49,380 --> 00:09:55,690 This is Bangladesh, the delta of the Ganges, Bramaputhra and Meghna. 109 00:09:55,690 --> 00:09:59,520 Look at the upper Eastern corner, called Sylhet 110 00:09:59,520 --> 00:10:04,510 This is where world record rain is falling 111 00:10:04,510 --> 00:10:10,970 During the monsoon the Sylhet area is deeply flooded, up to more than 4 m deep. 112 00:10:10,970 --> 00:10:16,180 You might think this is because of the heavy rainfall in the area, but it is because of 113 00:10:16,180 --> 00:10:22,640 the backwater from the Meghna, where it joins the Ganges and the Bramaputhra 114 00:10:22,640 --> 00:10:26,210 Here you see this backwater effect. 115 00:10:26,210 --> 00:10:33,210 During the pre-monsoon, in May, the floods in the Surma, which drains Sylhet, can discharge 116 00:10:33,260 --> 00:10:37,090 uninhibited to the Gulf of Bengal, 117 00:10:37,090 --> 00:10:42,360 But during the peak of the monsoon, the discharge of the Ganges and Bramaputhra is so high, 118 00:10:42,360 --> 00:10:45,740 that it causes a great backwater. 119 00:10:45,740 --> 00:10:50,260 This causes rating curves to tilt up 120 00:10:50,700 --> 00:10:56,440 We see that these backwater curves are labelled as design floods with a probability of 121 00:10:56,450 --> 00:11:00,270 once in a 100 and once in 20 years. 122 00:11:00,270 --> 00:11:04,900 How do we determine flood levels with these probabilities? 123 00:11:04,900 --> 00:11:11,340 In the chapter on precipitation, we prepared duration curves to rank the rainfall events 124 00:11:11,340 --> 00:11:13,850 according to their magnitude, 125 00:11:13,850 --> 00:11:17,740 In that way we obtained frequency curves. 126 00:11:17,740 --> 00:11:24,740 For extreme floods, we shall make use of Gumbel's theory for annual extremes. 127 00:11:25,440 --> 00:11:32,310 Here you see how a hydrograph can be turned into a duration curve, showing the % of time 128 00:11:32,310 --> 00:11:39,310 that a certain discharge is exceeded, or in this case ‘not-exceeded’. 129 00:11:39,460 --> 00:11:42,550 We call this the probability of non-exceedence 130 00:11:42,550 --> 00:11:45,830 The interesting part of this curve is the upper part, 131 00:11:45,830 --> 00:11:52,830 and moreover, we would like to extrapolate the curve to rare probabilities such as once 132 00:11:53,080 --> 00:12:00,080 in a 100 years: a probability of non-exceedence of 99%. 133 00:12:00,380 --> 00:12:04,710 Gumbel developed a statistical distribution for such extremes. 134 00:12:05,050 --> 00:12:11,260 His statistics are useful for determining design discharges or extreme flood levels 135 00:12:11,260 --> 00:12:15,410 such as these 136 00:12:15,410 --> 00:12:20,740 The basic assumption underlying Gumbel’s theory is that the underlying phenomenon 137 00:12:20,740 --> 00:12:27,740 (in this case river flow, or alternatively water levels or precipitation) are normally 138 00:12:27,780 --> 00:12:29,650 distributed 139 00:12:29,650 --> 00:12:33,410 But this is unfortunately seldom true 140 00:12:34,160 --> 00:12:43,020 additionally the data series needs to be homogeneous (caused by a single population of events) 141 00:12:43,880 --> 00:12:50,070 It should also be stationary (no climatic change or man-induced changes) 142 00:12:50,070 --> 00:12:55,760 and long enough (a reasonable part of the return period) 143 00:12:55,760 --> 00:12:59,750 But also these things are seldom true 144 00:12:59,750 --> 00:13:02,820 Is Gumbel’s theory then still useful? 145 00:13:02,820 --> 00:13:08,080 Well, yes, but you have to use it with good common sense 146 00:13:08,700 --> 00:13:10,600 These are the equations. 147 00:13:10,610 --> 00:13:15,260 I am sure they look difficult and complicated to you, 148 00:13:15,260 --> 00:13:17,260 but in fact they are not. 149 00:13:17,740 --> 00:13:22,840 They are much easier than the normal distribution, which is very similar 150 00:13:22,840 --> 00:13:29,840 Gumbel’s equation for q (the probability of non-exceedence) is simpler than Gauss’ 151 00:13:29,840 --> 00:13:33,530 equation, which we see here. 152 00:13:33,530 --> 00:13:39,550 Unlike the normal distribution, Gumbels's equation can be calculated easily with a pocket 153 00:13:39,550 --> 00:13:42,750 calculator or an iPhone 154 00:13:43,020 --> 00:13:47,320 Moreover, the reduced variate looks similar 155 00:13:47,920 --> 00:13:54,540 To carry out a Gumbel analysis, you have to select the extremes of a series. 156 00:13:54,640 --> 00:13:58,360 Normally we look at annual extremes. 157 00:13:59,230 --> 00:14:06,230 Say you have N years of data, then you take the N highest values of these years 158 00:14:06,250 --> 00:14:10,690 You then rank these extremes in order of magnitude 159 00:14:10,690 --> 00:14:16,660 To determine their frequency, you use the plotting position 160 00:14:16,660 --> 00:14:22,930 To prevent that the lowest value in the series gets a probability of 1, you add one to the 161 00:14:22,930 --> 00:14:26,300 number of years in the denominator 162 00:14:26,300 --> 00:14:32,310 As a result, the highest value in 9 years, has a probability of exceedence of once in 163 00:14:32,310 --> 00:14:34,610 10 years 164 00:14:35,300 --> 00:14:41,100 Here is a Table with highest peaks over a period of 7 years. 165 00:14:41,770 --> 00:14:44,960 A short series, merely as an example. 166 00:14:44,960 --> 00:14:50,310 We select the 7 highest values and rank them 167 00:14:50,310 --> 00:14:56,150 The highest value then has the probability of exceedence of once in 8 years. 168 00:14:56,150 --> 00:15:03,150 Gumbel paper is prepared in a way that the horizontal axis for the reduced variate y 169 00:15:03,320 --> 00:15:05,380 is linear. 170 00:15:05,380 --> 00:15:12,120 The Gumbel equation then plots as a straight line against the vertical ordinate. 171 00:15:12,120 --> 00:15:17,970 The probability of non-exceedence belonging to these y values are calculated with the 172 00:15:17,970 --> 00:15:24,779 Gumbel formula resulting in the typical probability pattern of the graph. 173 00:15:24,779 --> 00:15:30,599 The vertical ordinate is the x, which has a linear relationship with y 174 00:15:32,400 --> 00:15:37,440 I’ll show you an example of a Gumbel line for Thailand 175 00:15:37,440 --> 00:15:44,440 where as you can see severe floods can take place such as in 2011, when all the bank were 176 00:15:44,540 --> 00:15:47,310 overtopped 177 00:15:47,310 --> 00:15:51,680 I'll show you the Gumbel graph of Phraya Banlu 178 00:15:51,680 --> 00:15:58,680 It clearly shows that the highest values bend of when the banks overtop 179 00:15:59,360 --> 00:16:03,080 Just like we saw happening with the rating curve 180 00:16:03,080 --> 00:16:10,080 Of course the kink disappears when you build a dike on both sides of the river 181 00:16:10,960 --> 00:16:17,960 But what is the probability that a flood with a return period of T actually occurs within 182 00:16:18,470 --> 00:16:23,839 a period of n years? It's this ! 183 00:16:23,839 --> 00:16:28,110 Try it yourself in the exercise 184 00:16:28,110 --> 00:16:33,920 In applying Gumbel’s theory, you should always remain critical 185 00:16:33,920 --> 00:16:37,150 Series are seldom normally distributed 186 00:16:37,150 --> 00:16:42,800 You cannot extrapolate the theory much beyond the length of the series and you must always 187 00:16:42,800 --> 00:16:47,000 be aware that series are not homogeneous. 188 00:16:47,000 --> 00:16:52,420 Moreover, people are always tampering with the hydrological system 189 00:16:52,420 --> 00:16:59,420 and as a result, its characteristics change over time 190 00:16:59,960 --> 00:17:06,960 This was maybe not an easy part of the course, but if you study it closely, and if you practice, 191 00:17:08,039 --> 00:17:11,980 then it is simpler than it seems. 192 00:17:11,980 --> 00:17:16,860 In the next module we'll discuss the runoff generation mechanisms.