1 00:00:12,250 --> 00:00:06,150 you 2 00:00:20,190 --> 00:00:14,160 [Music] 3 00:00:23,740 --> 00:00:20,200 hey I'm Jade this is my first talk and 4 00:00:26,410 --> 00:00:23,750 today I'd like to talk to you about the 5 00:00:29,109 --> 00:00:26,420 possibility of snowball bifurcations on 6 00:00:34,180 --> 00:00:29,119 tightly locked exoplanet so orbiting and 7 00:00:36,100 --> 00:00:34,190 stars okay so as everyone in the room 8 00:00:38,290 --> 00:00:36,110 here knows by now we found many ago 9 00:00:40,330 --> 00:00:38,300 planets and much of the fields focus is 10 00:00:42,340 --> 00:00:40,340 on trying to figure out which one's of 11 00:00:43,780 --> 00:00:42,350 those could be habitable now to know 12 00:00:45,760 --> 00:00:43,790 that we need to know which ones can 13 00:00:55,600 --> 00:00:45,770 support surface liquid water because 14 00:00:57,850 --> 00:00:55,610 habitability is a surface property okay 15 00:01:00,790 --> 00:00:57,860 now a major factor that can affect a 16 00:01:02,970 --> 00:01:00,800 planet's habitability is the ice albedo 17 00:01:06,400 --> 00:01:02,980 feedback so here on the left is very 18 00:01:08,560 --> 00:01:06,410 simple cartoon illustrates the effect so 19 00:01:10,990 --> 00:01:08,570 we know that the ocean absorbs much more 20 00:01:13,300 --> 00:01:11,000 solar radiation than ice which is very 21 00:01:16,210 --> 00:01:13,310 reflective so if we were to increase the 22 00:01:17,800 --> 00:01:16,220 insulation on the planet we would have a 23 00:01:20,410 --> 00:01:17,810 melting of sea ice which will decrease 24 00:01:22,240 --> 00:01:20,420 the albedo and induce more melting but 25 00:01:24,969 --> 00:01:22,250 if we were to lower the inspiration we 26 00:01:26,859 --> 00:01:24,979 would have some sea ice on forming which 27 00:01:28,630 --> 00:01:26,869 will increase the albedo and induce more 28 00:01:30,820 --> 00:01:28,640 freezing so because of this 29 00:01:33,340 --> 00:01:30,830 non-linearity a planet like the earth 30 00:01:36,399 --> 00:01:33,350 can have two stable States for a range 31 00:01:38,950 --> 00:01:36,409 of installations so we can look here at 32 00:01:41,920 --> 00:01:38,960 the plot on the right here the vertical 33 00:01:43,990 --> 00:01:41,930 axis is the sign of the ice latitude so 34 00:01:46,990 --> 00:01:44,000 the ice latitude is the latitudinal 35 00:01:50,050 --> 00:01:47,000 extent of ice on the planet and the 36 00:01:52,090 --> 00:01:50,060 horizontal axis is the insulation the 37 00:01:54,370 --> 00:01:52,100 solid lines represent stable States and 38 00:01:56,080 --> 00:01:54,380 the dashed line unstable sticks so if we 39 00:01:58,149 --> 00:01:56,090 start at the top right with a planet 40 00:01:59,530 --> 00:01:58,159 like the earth like modern earth in its 41 00:02:04,600 --> 00:01:59,540 warm state and we decrease the 42 00:02:06,670 --> 00:02:04,610 insulation eventually it will jump into 43 00:02:08,770 --> 00:02:06,680 a snowball state right there now to get 44 00:02:10,630 --> 00:02:08,780 out of this noble state we would need to 45 00:02:13,090 --> 00:02:10,640 increase the insulation but much more 46 00:02:14,920 --> 00:02:13,100 than the glaciation insulation so a 47 00:02:17,080 --> 00:02:14,930 planet might have a hard time to escape 48 00:02:19,690 --> 00:02:17,090 that snuggle state and this could have 49 00:02:21,490 --> 00:02:19,700 bad implications for habitability but at 50 00:02:24,340 --> 00:02:21,500 the same time although I'm not an expert 51 00:02:26,780 --> 00:02:24,350 on this for Earth 52 00:02:28,610 --> 00:02:26,790 like going through a snowball stage has 53 00:02:31,010 --> 00:02:28,620 been associated with the rise in oxygen 54 00:02:34,960 --> 00:02:31,020 and in complex life so it could be a 55 00:02:38,870 --> 00:02:34,970 good thing but still up for debate so 56 00:02:40,970 --> 00:02:38,880 okay now on this beautiful figure again 57 00:02:42,950 --> 00:02:40,980 by funny we see that the boundaries of 58 00:02:45,770 --> 00:02:42,960 the habitable zone strongly depend on 59 00:02:47,810 --> 00:02:45,780 the stellar type so for an M dwarf here 60 00:02:49,910 --> 00:02:47,820 which is much smaller and dimmer than a 61 00:02:54,530 --> 00:02:49,920 G sorry the habitable zone is much more 62 00:02:56,210 --> 00:02:54,540 close in so in fact it's so close in 63 00:02:58,520 --> 00:02:56,220 that a planet that's orbiting in the 64 00:03:00,710 --> 00:02:58,530 habitable zone of those M stars are 65 00:03:04,220 --> 00:03:00,720 close enough to likely become tightly 66 00:03:06,470 --> 00:03:04,230 locked as we see here so this means that 67 00:03:08,660 --> 00:03:06,480 one side of the planet will always be 68 00:03:11,360 --> 00:03:08,670 facing the star and the other side will 69 00:03:13,640 --> 00:03:11,370 always be facing away so because those 70 00:03:15,949 --> 00:03:13,650 planets orbit their stars in such a 71 00:03:18,260 --> 00:03:15,959 different manner than rapidly rotating 72 00:03:19,790 --> 00:03:18,270 planets like the earth we want to know 73 00:03:21,740 --> 00:03:19,800 whether they could still go through a 74 00:03:26,720 --> 00:03:21,750 snowboard bifurcation like we know the 75 00:03:29,240 --> 00:03:26,730 earth can now there's already been some 76 00:03:32,390 --> 00:03:29,250 work done on the subject first let's 77 00:03:35,690 --> 00:03:32,400 look here at those two plots by Joshi in 78 00:03:38,030 --> 00:03:35,700 2012 the top panel shows that the peak 79 00:03:39,860 --> 00:03:38,040 of the third spectrum of an M star is 80 00:03:41,990 --> 00:03:39,870 that a higher wavelength than that of a 81 00:03:44,600 --> 00:03:42,000 G star and because of this the Eifel 82 00:03:46,759 --> 00:03:44,610 video of a planet orbiting those M stars 83 00:03:48,979 --> 00:03:46,769 will be much lower so the non-linearity 84 00:03:51,080 --> 00:03:48,989 of the Eifel video effect will be 85 00:03:53,000 --> 00:03:51,090 reduced and we can imagine that a planet 86 00:03:55,370 --> 00:03:53,010 orbiting an M sir might have a more 87 00:03:58,640 --> 00:03:55,380 difficult time going through a snowball 88 00:04:01,970 --> 00:03:58,650 bifurcation because of that and also 89 00:04:04,850 --> 00:04:01,980 more recently here shields in 2014 90 00:04:08,210 --> 00:04:04,860 showed that for an M star compared to a 91 00:04:11,390 --> 00:04:08,220 G star the range of information at which 92 00:04:12,890 --> 00:04:11,400 there is by stability is much smaller so 93 00:04:14,990 --> 00:04:12,900 again the planet might have a more 94 00:04:17,479 --> 00:04:15,000 difficult time going through its network 95 00:04:20,090 --> 00:04:17,489 bifurcation now both of those works were 96 00:04:22,460 --> 00:04:20,100 about comparing the different solar 97 00:04:25,610 --> 00:04:22,470 spectra of an M star energy star and 98 00:04:27,680 --> 00:04:25,620 seeing how going like orbiting an M star 99 00:04:29,960 --> 00:04:27,690 might make it more difficult for the 100 00:04:31,909 --> 00:04:29,970 planet to go through the bifurcation but 101 00:04:34,159 --> 00:04:31,919 what we want to know is whether or not 102 00:04:36,260 --> 00:04:34,169 the fact itself that the planet 103 00:04:38,749 --> 00:04:36,270 My Luck whether it's orbiting an M star 104 00:04:40,489 --> 00:04:38,759 or a G star or whatever could make it 105 00:04:44,480 --> 00:04:40,499 more difficult to go through the 106 00:04:46,939 --> 00:04:44,490 bifurcation okay so we use a global 107 00:04:50,420 --> 00:04:46,949 climate model called blessing so it's a 108 00:04:52,010 --> 00:04:50,430 3d GCM of medium complexity we set it up 109 00:04:54,350 --> 00:04:52,020 in a modern earth continual 110 00:04:58,399 --> 00:04:54,360 configuration computed clouds and kept 111 00:05:00,980 --> 00:04:58,409 this here to fix a 360 ppm and here's 112 00:05:02,420 --> 00:05:00,990 what we see first for the earth so I'm 113 00:05:04,339 --> 00:05:02,430 here the top panels the surface 114 00:05:06,649 --> 00:05:04,349 temperature the bottom the sea ice cover 115 00:05:10,279 --> 00:05:06,659 and again the horizontal axis is always 116 00:05:12,529 --> 00:05:10,289 insulation the red stars here correspond 117 00:05:15,110 --> 00:05:12,539 to a warm start so where the planet is 118 00:05:17,089 --> 00:05:15,120 completely ice-free and the blue stars 119 00:05:19,279 --> 00:05:17,099 correspond to a cold start or it's 120 00:05:22,730 --> 00:05:19,289 completely ice covered on both of those 121 00:05:25,219 --> 00:05:22,740 initially and we see that we retrieve 122 00:05:27,860 --> 00:05:25,229 the expected snowboard bifurcation here 123 00:05:29,719 --> 00:05:27,870 and we have by stability so great the 124 00:05:32,570 --> 00:05:29,729 GPM reproduces the very well-known 125 00:05:35,179 --> 00:05:32,580 result for the earth but now using it in 126 00:05:37,670 --> 00:05:35,189 a tightly locked configuration we see 127 00:05:40,459 --> 00:05:37,680 something quite different right here on 128 00:05:42,740 --> 00:05:40,469 the left so whether we start cold or 129 00:05:44,209 --> 00:05:42,750 warm the surface temperature increases 130 00:05:46,339 --> 00:05:44,219 or decreases linearly with the 131 00:05:49,159 --> 00:05:46,349 insulation we don't see a snowboard 132 00:05:51,860 --> 00:05:49,169 bifurcation now you might be wondering 133 00:05:53,659 --> 00:05:51,870 about the small gap right here in 134 00:05:56,329 --> 00:05:53,669 surface temperature for those 135 00:05:58,399 --> 00:05:56,339 intermediate ranges of installations but 136 00:06:00,769 --> 00:05:58,409 this is not real hysteresis it's 137 00:06:02,959 --> 00:06:00,779 actually just a model artifact due to 138 00:06:05,389 --> 00:06:02,969 the simple CI scheme of the GPM we're 139 00:06:06,950 --> 00:06:05,399 using I don't want to get more into it 140 00:06:09,139 --> 00:06:06,960 now but if you'd like to know you can 141 00:06:10,969 --> 00:06:09,149 always ask me later but what's really 142 00:06:12,649 --> 00:06:10,979 important is just setting up the planet 143 00:06:15,170 --> 00:06:12,659 in the GCM in a tightly locked 144 00:06:17,420 --> 00:06:15,180 configuration gets rid of the snowboard 145 00:06:19,040 --> 00:06:17,430 by vacation and this is with a GSR 146 00:06:21,469 --> 00:06:19,050 spectrum all right so we can imagine 147 00:06:23,269 --> 00:06:21,479 that if we had used an answer spectrum 148 00:06:26,689 --> 00:06:23,279 it would be even less likely to go 149 00:06:28,909 --> 00:06:26,699 through a bifurcation okay now how can 150 00:06:31,279 --> 00:06:28,919 we understand this well we can use a 151 00:06:34,219 --> 00:06:31,289 simple energy balance model right here 152 00:06:36,290 --> 00:06:34,229 where the absorb solar radiation is 153 00:06:39,019 --> 00:06:36,300 equal to the outgoing long-wave plus the 154 00:06:40,969 --> 00:06:39,029 heat transport both on parametrize so 155 00:06:43,339 --> 00:06:40,979 first for the earth here's an example 156 00:06:46,159 --> 00:06:43,349 state for the planet and what's 157 00:06:47,570 --> 00:06:46,169 important to note right here is so this 158 00:06:49,580 --> 00:06:47,580 is the equator in the middle 159 00:06:51,560 --> 00:06:49,590 it's that the installation shape is 160 00:06:53,720 --> 00:06:51,570 flatter on the equator right we don't 161 00:06:56,630 --> 00:06:53,730 see a super sharp increase in insulation 162 00:06:59,270 --> 00:06:56,640 from the pole to the equator now solving 163 00:07:01,610 --> 00:06:59,280 this IBM for the ice latitude so again 164 00:07:04,130 --> 00:07:01,620 the isolated is the latitudinal extent 165 00:07:06,020 --> 00:07:04,140 of the ice on the planet we retrieve the 166 00:07:08,150 --> 00:07:06,030 bifurcation diagram that I showed and 167 00:07:09,920 --> 00:07:08,160 explained at the beginning so where the 168 00:07:15,290 --> 00:07:09,930 planet can jump into a snowball stage 169 00:07:17,300 --> 00:07:15,300 here okay now setting up the EVM in a 170 00:07:18,910 --> 00:07:17,310 tightly locked configuration what's 171 00:07:21,320 --> 00:07:18,920 important is that the insulation 172 00:07:23,930 --> 00:07:21,330 increases really sharply from the 173 00:07:25,850 --> 00:07:23,940 Terminator which is here to the sub-zero 174 00:07:28,700 --> 00:07:25,860 point which is here right compared to 175 00:07:31,130 --> 00:07:28,710 the earth which was much more flat now 176 00:07:33,770 --> 00:07:31,140 solving the EBM again for the ice 177 00:07:35,960 --> 00:07:33,780 latitude the bifurcation diagram here 178 00:07:37,820 --> 00:07:35,970 shows no bifurcation so it looks like 179 00:07:41,000 --> 00:07:37,830 the EBM is able to explain what's 180 00:07:43,460 --> 00:07:41,010 happening in our GCM now I just note 181 00:07:45,530 --> 00:07:43,470 that we are able to retrieve the 182 00:07:47,930 --> 00:07:45,540 bifurcation in this slightly large 183 00:07:49,580 --> 00:07:47,940 configuration in our ABM if we just 184 00:07:52,130 --> 00:07:49,590 greatly increase the heat transport 185 00:07:57,110 --> 00:07:52,140 let's just keep this in mind for the 186 00:07:58,940 --> 00:07:57,120 next slide ok so this slide explain 187 00:08:00,740 --> 00:07:58,950 what's happening in DBM but before 188 00:08:02,630 --> 00:08:00,750 looking at it ultimately what you need 189 00:08:04,610 --> 00:08:02,640 to know is that whether or not the 190 00:08:07,820 --> 00:08:04,620 planet goes through on the bifurcation 191 00:08:10,430 --> 00:08:07,830 depends on the insulation shape so let's 192 00:08:12,080 --> 00:08:10,440 first look at on the right here for the 193 00:08:14,990 --> 00:08:12,090 case where the planet does go through 194 00:08:16,730 --> 00:08:15,000 the bifurcation so we have the ice line 195 00:08:19,850 --> 00:08:16,740 somewhere between the pole and equator 196 00:08:22,100 --> 00:08:19,860 and we perturb it slightly towards the 197 00:08:24,140 --> 00:08:22,110 equator now there the insulation and the 198 00:08:26,210 --> 00:08:24,150 hay transport will be greater but 199 00:08:28,700 --> 00:08:26,220 because as we saw for the earth the 200 00:08:30,860 --> 00:08:28,710 insulation ship is not so sharp or on 201 00:08:32,570 --> 00:08:30,870 the equator at that point the hay 202 00:08:34,820 --> 00:08:32,580 transport will actually have increased 203 00:08:37,340 --> 00:08:34,830 more than the insulation increased and 204 00:08:39,650 --> 00:08:37,350 because of this di slang we continue all 205 00:08:42,950 --> 00:08:39,660 the way to the equator for the planet is 206 00:08:44,570 --> 00:08:42,960 in a snowball state now on the left for 207 00:08:46,970 --> 00:08:44,580 the stable case for example for a 208 00:08:48,440 --> 00:08:46,980 tightly locked planet again we have a 209 00:08:50,240 --> 00:08:48,450 nice line somewhere between the 210 00:08:53,150 --> 00:08:50,250 Terminator and the substellar point and 211 00:08:55,460 --> 00:08:53,160 we again perturb it slightly so towards 212 00:08:57,980 --> 00:08:55,470 the sub-zero point this time but because 213 00:09:00,110 --> 00:08:57,990 as we saw for HIV locked a net the rise 214 00:09:02,450 --> 00:09:00,120 in insulation is so sharp from the term 215 00:09:04,010 --> 00:09:02,460 later to the substernal point this time 216 00:09:06,530 --> 00:09:04,020 the installation will have increased 217 00:09:08,480 --> 00:09:06,540 more than the heat transport and because 218 00:09:11,060 --> 00:09:08,490 of this the ice line will return to its 219 00:09:13,870 --> 00:09:11,070 original position so the planet doesn't 220 00:09:16,519 --> 00:09:13,880 go through a snowball bifurcation so 221 00:09:18,800 --> 00:09:16,529 this is my conclusion that tightly 222 00:09:20,780 --> 00:09:18,810 locked exoplanets are unlikely to go 223 00:09:23,030 --> 00:09:20,790 through a snowball bifurcation because 224 00:09:25,130 --> 00:09:23,040 of the sharp increase in insulation from 225 00:09:27,860 --> 00:09:25,140 the Terminator to the sub-zero point and 226 00:09:29,120 --> 00:09:27,870 we have a paper in prep on this that 227 00:09:41,510 --> 00:09:29,130 will be submitted soon if you're 228 00:09:43,160 --> 00:09:41,520 interested thank you hi my name is 229 00:09:44,870 --> 00:09:43,170 Richard Archer from University Colorado 230 00:09:48,380 --> 00:09:44,880 Boulder I thought it was really great 231 00:09:50,420 --> 00:09:48,390 presentation so congratulations I have a 232 00:09:53,090 --> 00:09:50,430 question regarding volcanism so in terms 233 00:09:55,519 --> 00:09:53,100 of snowball earth it was there are 234 00:09:57,079 --> 00:09:55,529 people that suggested that the release 235 00:09:59,930 --> 00:09:57,089 of some all births condition was driven 236 00:10:01,610 --> 00:09:59,940 by volcanic co2 so after it's still all 237 00:10:03,350 --> 00:10:01,620 earth you actually have very large 238 00:10:06,620 --> 00:10:03,360 greenhouse effect and I just wonder what 239 00:10:09,500 --> 00:10:06,630 you think that might apply to to your 240 00:10:10,880 --> 00:10:09,510 model so that's to get out of the snow 241 00:10:13,690 --> 00:10:10,890 board once you're already in it 242 00:10:17,390 --> 00:10:13,700 volcanoes could out gas a lot of co2 243 00:10:19,010 --> 00:10:17,400 right I mean we just saw that tightly 244 00:10:21,019 --> 00:10:19,020 locked planet don't go through the solar 245 00:10:22,370 --> 00:10:21,029 bifurcation but yes they can be in a 246 00:10:25,160 --> 00:10:22,380 snowboard state if you decrease the 247 00:10:26,810 --> 00:10:25,170 insulation enough however to get out of 248 00:10:28,880 --> 00:10:26,820 this noble state it would be much easier 249 00:10:30,650 --> 00:10:28,890 than for the earth because it's not a 250 00:10:38,820 --> 00:10:30,660 bifurcation so you would just need to 251 00:10:48,300 --> 00:10:46,380 oh so you mean for example if we had 252 00:10:55,650 --> 00:10:48,310 tried using the GCM with a much higher 253 00:10:57,900 --> 00:10:55,660 co2 level sure okay yeah I was just 254 00:10:59,130 --> 00:10:57,910 wondering the the result eeeh tightly 255 00:11:02,490 --> 00:10:59,140 locked exoplanets are unlikely to go 256 00:11:04,769 --> 00:11:02,500 through its Noble is that conditional on 257 00:11:07,440 --> 00:11:04,779 assuming that there is not any heat 258 00:11:08,670 --> 00:11:07,450 transport from the insulated side to the 259 00:11:13,319 --> 00:11:08,680 shadow side of a tidally locked planet 260 00:11:15,360 --> 00:11:13,329 ah no no there is heat transport so you 261 00:11:16,710 --> 00:11:15,370 have a basic model of default this is 262 00:11:18,210 --> 00:11:16,720 how much heat transport you have and 263 00:11:20,850 --> 00:11:18,220 then you still get tight and you just 264 00:11:22,440 --> 00:11:20,860 and you still get a what - you do not go 265 00:11:25,050 --> 00:11:22,450 through the bifurcation but if you 266 00:11:27,150 --> 00:11:25,060 increase that above what you expect then 267 00:11:30,420 --> 00:11:27,160 you do go through them the heat 268 00:11:33,269 --> 00:11:30,430 transport yes yes yeah you are actually 269 00:11:36,389 --> 00:11:33,279 yeah actually it's interesting that in 270 00:11:38,519 --> 00:11:36,399 the GCM I didn't present it in the talk 271 00:11:40,170 --> 00:11:38,529 but we found that the heat transport on 272 00:11:42,449 --> 00:11:40,180 the tightly locked planet is much 273 00:11:44,430 --> 00:11:42,459 greater than for the earth and it's 274 00:11:47,250 --> 00:11:44,440 great enough that on the IBM we should 275 00:11:49,980 --> 00:11:47,260 be able to get the bifurcation back but 276 00:11:52,500 --> 00:11:49,990 the difference in albedo it's smaller 277 00:11:54,540 --> 00:11:52,510 than for the earth because of so many 278 00:11:56,340 --> 00:11:54,550 clouds at the Sub Zero point and they 279 00:11:58,170 --> 00:11:56,350 still get the tidally locked planet to 280 00:11:59,730 --> 00:11:58,180 not go through the bifurcation so as 281 00:12:02,130 --> 00:11:59,740 heat transport is really important it's 282 00:12:03,810 --> 00:12:02,140 definitely happening and it's enough to 283 00:12:07,430 --> 00:12:03,820 normally go through a bifurcation if 284 00:12:11,850 --> 00:12:07,440 that albedo range wasn't smaller please 285 00:12:13,740 --> 00:12:11,860 any more questions if not we can give 286 00:12:14,250 --> 00:12:13,750 Jada round of applause thank you very