1 00:00:00,790 --> 00:00:07,320 [Music] 2 00:00:11,459 --> 00:00:09,289 [Applause] 3 00:00:14,250 --> 00:00:11,469 morning everybody my name is Illya 4 00:00:15,990 --> 00:00:14,260 Wofford I am a postback at NASA Goddard 5 00:00:18,300 --> 00:00:16,000 Space Flight Center I'm really excited 6 00:00:19,800 --> 00:00:18,310 to be here so today I'm going to be 7 00:00:22,470 --> 00:00:19,810 talking to you about revisiting early 8 00:00:24,269 --> 00:00:22,480 Earth's methanogenic biosphere so if you 9 00:00:25,800 --> 00:00:24,279 were to think about early Earth you 10 00:00:27,689 --> 00:00:25,810 could think of it as like an exoplanet 11 00:00:31,710 --> 00:00:27,699 or a laboratory in which you can explore 12 00:00:35,790 --> 00:00:31,720 possible ranges of biospheres in which 13 00:00:37,110 --> 00:00:35,800 we can see what with the atmospheric 14 00:00:39,479 --> 00:00:37,120 composition of these terrestrial plants 15 00:00:40,709 --> 00:00:39,489 would look like and when we we also look 16 00:00:42,959 --> 00:00:40,719 about looking at when we think about 17 00:00:44,970 --> 00:00:42,969 early Earth is methane so you think 18 00:00:46,740 --> 00:00:44,980 about methane you think about 19 00:00:48,599 --> 00:00:46,750 methanogenesis which is one way we can 20 00:00:50,729 --> 00:00:48,609 create methane which in this case you 21 00:00:52,619 --> 00:00:50,739 have microbes that will take in these 22 00:00:54,209 --> 00:00:52,629 hydrogen molecules they will synthesize 23 00:00:56,069 --> 00:00:54,219 this methane in their bodies and 24 00:00:57,270 --> 00:00:56,079 eventually they will release it back 25 00:00:59,549 --> 00:00:57,280 into the oceans and they will eventually 26 00:01:01,200 --> 00:00:59,559 make its way into those atmospheres this 27 00:01:03,360 --> 00:01:01,210 is called biological methane production 28 00:01:05,130 --> 00:01:03,370 and we can use that biological methane 29 00:01:09,210 --> 00:01:05,140 production to create to look at 30 00:01:11,130 --> 00:01:09,220 biosignatures another way that we can 31 00:01:13,380 --> 00:01:11,140 see methane is that we can use 32 00:01:15,270 --> 00:01:13,390 serpentinization or abiotic methane 33 00:01:17,670 --> 00:01:15,280 productions which in this case motion 34 00:01:20,550 --> 00:01:17,680 across minerals such as such as olivine 35 00:01:22,380 --> 00:01:20,560 and pyroxene are will react with water 36 00:01:24,240 --> 00:01:22,390 and in that case you will create 37 00:01:26,010 --> 00:01:24,250 serpentine and as a byproduct of this 38 00:01:28,230 --> 00:01:26,020 reaction you will get hydrogen methane 39 00:01:39,480 --> 00:01:28,240 and heat that makes it a low temperature 40 00:01:41,399 --> 00:01:39,490 low pressure exothermic reaction so the 41 00:01:43,289 --> 00:01:41,409 motivation for our work is that we use 42 00:01:45,929 --> 00:01:43,299 dr. Chris Hansen Thailand's most recent 43 00:01:47,819 --> 00:01:45,939 project and what he did is he utilized 44 00:01:49,440 --> 00:01:47,829 the model to calculate methane fluxes 45 00:01:52,529 --> 00:01:49,450 based on oceanic parameters such as 46 00:01:54,660 --> 00:01:52,539 ocean crust arrest ocean crust ratios as 47 00:01:56,399 --> 00:01:54,670 well as seafloor spreading to name a few 48 00:01:58,289 --> 00:01:56,409 and was able to calculate a probability 49 00:01:59,999 --> 00:01:58,299 density of fluxes that could be 50 00:02:02,880 --> 00:02:00,009 explained by a by the methane production 51 00:02:04,410 --> 00:02:02,890 which is highlighted here so as you can 52 00:02:06,779 --> 00:02:04,420 see as you're moving the methane flex 53 00:02:08,070 --> 00:02:06,789 fluxes towards the 10 tera moles per 54 00:02:10,200 --> 00:02:08,080 year mark you can see that your 55 00:02:11,220 --> 00:02:10,210 probability is starting to go down but 56 00:02:12,600 --> 00:02:11,230 before that you can see that your 57 00:02:14,400 --> 00:02:12,610 probability density for a budding 58 00:02:16,050 --> 00:02:14,410 methane is pretty high so you could 59 00:02:18,119 --> 00:02:16,060 think of this as your abiotic methane 60 00:02:19,770 --> 00:02:18,129 range and then of course when you get to 61 00:02:21,210 --> 00:02:19,780 10 tera moles per year to approximately 62 00:02:23,040 --> 00:02:21,220 15 tera moles per year you can 63 00:02:24,990 --> 00:02:23,050 see that you're you there's still a 64 00:02:27,840 --> 00:02:25,000 slight chance it's very small less than 65 00:02:29,880 --> 00:02:27,850 0.1% of it to actually be justified by a 66 00:02:31,320 --> 00:02:29,890 body methane production so this you 67 00:02:33,180 --> 00:02:31,330 could think of as your gray area or your 68 00:02:35,940 --> 00:02:33,190 plausible methane biology biological 69 00:02:37,920 --> 00:02:35,950 methane production range and then of 70 00:02:39,480 --> 00:02:37,930 course after the 15 tera moles per year 71 00:02:42,060 --> 00:02:39,490 mark this is what you would consider 72 00:02:43,620 --> 00:02:42,070 your definitive biological methane 73 00:02:49,260 --> 00:02:43,630 production range in which where you 74 00:02:52,050 --> 00:02:49,270 would most likely see life so as we move 75 00:02:53,699 --> 00:02:52,060 focus me as I move forward into flagship 76 00:02:55,800 --> 00:02:53,709 missions such as Lavar we're going to 77 00:02:57,390 --> 00:02:55,810 rely on them to actually give us give us 78 00:03:00,750 --> 00:02:57,400 information how to identify spectral 79 00:03:01,920 --> 00:03:00,760 features of exoplanets particularly if 80 00:03:04,350 --> 00:03:01,930 we could actually see these spectral 81 00:03:07,860 --> 00:03:04,360 differences in biotic atmospheres versus 82 00:03:09,449 --> 00:03:07,870 anybody methane being produced so in our 83 00:03:10,830 --> 00:03:09,459 project what we did is use this model 84 00:03:12,990 --> 00:03:10,840 called Atomos which is a 1d 85 00:03:16,020 --> 00:03:13,000 photochemical climate model it consists 86 00:03:17,790 --> 00:03:16,030 of two two components you have the 87 00:03:19,710 --> 00:03:17,800 photochemical component which simulates 88 00:03:22,350 --> 00:03:19,720 atmospheric reactions in our case we're 89 00:03:24,060 --> 00:03:22,360 using arc and earth and then we take 90 00:03:25,500 --> 00:03:24,070 those reaction in atmospheric reactions 91 00:03:26,910 --> 00:03:25,510 and they're sent to a climate to the 92 00:03:28,620 --> 00:03:26,920 climate component which basically 93 00:03:30,270 --> 00:03:28,630 generates a temperature profile based on 94 00:03:31,920 --> 00:03:30,280 those photochemical reactions and this 95 00:03:33,509 --> 00:03:31,930 is an actual run that's being shown in 96 00:03:37,110 --> 00:03:33,519 real time even though the resolution is 97 00:03:38,970 --> 00:03:37,120 not very good another thing that we use 98 00:03:40,350 --> 00:03:38,980 is PSG or the planetary spectrum 99 00:03:42,690 --> 00:03:40,360 generator which basically takes those 100 00:03:44,699 --> 00:03:42,700 methane fluxes and we put them into this 101 00:03:45,690 --> 00:03:44,709 PSG over the spectrum generator in order 102 00:03:48,270 --> 00:03:45,700 to give us a spectra of what these 103 00:03:50,460 --> 00:03:48,280 fluxes would look like and then lastly 104 00:03:52,320 --> 00:03:50,470 we use lavars cronograph noise model 105 00:03:54,180 --> 00:03:52,330 which in this case what we did is that 106 00:03:55,680 --> 00:03:54,190 it was able to take those methane fluxes 107 00:03:59,220 --> 00:03:55,690 and essentially show us what the 108 00:04:00,660 --> 00:03:59,230 observers perspective would look like so 109 00:04:02,759 --> 00:04:00,670 in working order what we've done is 110 00:04:04,680 --> 00:04:02,769 we've given it a flux we gave it to at 111 00:04:06,630 --> 00:04:04,690 most at most then printed a mixing ratio 112 00:04:08,670 --> 00:04:06,640 we then plotted our flux versus mixing 113 00:04:11,250 --> 00:04:08,680 ratio and then we were able to give it 114 00:04:13,410 --> 00:04:11,260 to PSG which gave us the spectra which 115 00:04:14,580 --> 00:04:13,420 is here and then from those fluxes we 116 00:04:16,170 --> 00:04:14,590 able we were able to give it to the 117 00:04:17,670 --> 00:04:16,180 coronagraph to give us direct imaging of 118 00:04:23,250 --> 00:04:17,680 what the actual observer would actually 119 00:04:24,840 --> 00:04:23,260 see based on those fluxes so the bigger 120 00:04:26,610 --> 00:04:24,850 question is how will be spectral 121 00:04:28,890 --> 00:04:26,620 peeresses change if we were looking at 122 00:04:33,240 --> 00:04:28,900 about an abiotic methane flux versus a 123 00:04:34,740 --> 00:04:33,250 biological methane flux all right so if 124 00:04:35,549 --> 00:04:34,750 you were to look at this plot what we 125 00:04:38,789 --> 00:04:35,559 did is that we 126 00:04:41,219 --> 00:04:38,799 at these fluxes in a 1% 2% and 5% co2 127 00:04:43,319 --> 00:04:41,229 atmospheres because that's we know that 128 00:04:45,389 --> 00:04:43,329 co2 or carbon dioxide affects how meant 129 00:04:46,949 --> 00:04:45,399 they builds up in the atmosphere and as 130 00:04:48,809 --> 00:04:46,959 you can see looking at the pink line 131 00:04:50,759 --> 00:04:48,819 which is your 1% co2 atmosphere you can 132 00:04:51,959 --> 00:04:50,769 see that your methane mixing ratio is 133 00:04:53,579 --> 00:04:51,969 getting higher meaning that you have 134 00:04:55,649 --> 00:04:53,589 more methane accumulating in those 135 00:04:57,719 --> 00:04:55,659 atmospheres and thus making the methane 136 00:05:00,119 --> 00:04:57,729 very detectable whereas if you look at 137 00:05:01,919 --> 00:05:00,129 your 2% and 5% witches are your blue and 138 00:05:03,809 --> 00:05:01,929 your yellow your green line excuse me 139 00:05:05,369 --> 00:05:03,819 you can see that you have less methane 140 00:05:07,109 --> 00:05:05,379 accumulating meaning that it's orders of 141 00:05:08,939 --> 00:05:07,119 magnitudes lower than your one percent 142 00:05:10,889 --> 00:05:08,949 atmosphere me that you will need higher 143 00:05:12,169 --> 00:05:10,899 fluxes in those atmospheres in order for 144 00:05:14,729 --> 00:05:12,179 the methane to be detectable 145 00:05:16,649 --> 00:05:14,739 so in our parameters what we did is that 146 00:05:18,389 --> 00:05:16,659 we know that your zero to approximately 147 00:05:20,609 --> 00:05:18,399 10 tera moles based on Josh's paper 148 00:05:21,929 --> 00:05:20,619 initially but approximately 0 to 10 tera 149 00:05:25,289 --> 00:05:21,939 moles you can safely say those are your 150 00:05:26,579 --> 00:05:25,299 abiotic fluxes whereas we also simulate 151 00:05:28,349 --> 00:05:26,589 the earth life fluxes which is 152 00:05:29,759 --> 00:05:28,359 approximately 10 tera moles per year to 153 00:05:31,409 --> 00:05:29,769 approximately 40 tera moles which would 154 00:05:33,659 --> 00:05:31,419 be like your earth light body fluxes and 155 00:05:36,029 --> 00:05:33,669 then of course we also simulated even 156 00:05:37,769 --> 00:05:36,039 greater flux biological fluxes because 157 00:05:39,779 --> 00:05:37,779 we just frankly don't know what these 158 00:05:41,459 --> 00:05:39,789 methane budgets could be for some of 159 00:05:46,709 --> 00:05:41,469 those exoplanets and hopefully they'll 160 00:05:48,239 --> 00:05:46,719 have really cool microbes like this so 161 00:05:49,949 --> 00:05:48,249 when we take a look at the sorry excuse 162 00:05:52,709 --> 00:05:49,959 me so when we take a look at the one 163 00:05:54,839 --> 00:05:52,719 percent co2 spectra your blue line is a 164 00:05:56,879 --> 00:05:54,849 low methane flux your yellow line is a 165 00:05:58,859 --> 00:05:56,889 medium methane flux as well as your 166 00:06:00,749 --> 00:05:58,869 Green Line is the high methane flux and 167 00:06:02,009 --> 00:06:00,759 what you're seeing here is that your 168 00:06:03,359 --> 00:06:02,019 Green Line shows that you have very 169 00:06:05,429 --> 00:06:03,369 strong absorption features across 170 00:06:07,439 --> 00:06:05,439 various wavelengths showing you that 171 00:06:09,269 --> 00:06:07,449 your methane is absorbing a lot I mean 172 00:06:11,399 --> 00:06:09,279 that is detectable whereas if you're 173 00:06:13,199 --> 00:06:11,409 looking at your 1% which is your low or 174 00:06:15,599 --> 00:06:13,209 your low methane flux and your yellow 175 00:06:16,739 --> 00:06:15,609 which is the medium methane flux you 176 00:06:18,179 --> 00:06:16,749 still have strong absorption at 177 00:06:19,439 --> 00:06:18,189 different wavelengths but it's not as 178 00:06:22,319 --> 00:06:19,449 strong as you would see in very high 179 00:06:23,789 --> 00:06:22,329 methane environment methane fluxes but 180 00:06:26,129 --> 00:06:23,799 then when you look at your to person as 181 00:06:28,499 --> 00:06:26,139 your co2 is increasing you see that you 182 00:06:31,109 --> 00:06:28,509 still when you look at your high methane 183 00:06:32,159 --> 00:06:31,119 flux you can see that you have the green 184 00:06:34,589 --> 00:06:32,169 you can see that your stuff strong 185 00:06:36,599 --> 00:06:34,599 absorption at different wavelengths but 186 00:06:38,279 --> 00:06:36,609 not as strong as you would in the 1% 187 00:06:39,899 --> 00:06:38,289 whereas if you were looking at the blue 188 00:06:42,109 --> 00:06:39,909 and the yellow which is your low in your 189 00:06:43,829 --> 00:06:42,119 medium you can see that your flex or 190 00:06:45,989 --> 00:06:43,839 spectral lines are becoming almost 191 00:06:47,999 --> 00:06:45,999 indiscernible and again that same 192 00:06:48,960 --> 00:06:48,009 behavior is seen in the 5% co2 193 00:06:49,980 --> 00:06:48,970 atmosphere 194 00:06:51,480 --> 00:06:49,990 where you're still seeing strong 195 00:06:53,670 --> 00:06:51,490 absorption of the green which is the 196 00:06:55,560 --> 00:06:53,680 very high methane flux but when you look 197 00:06:57,570 --> 00:06:55,570 at your low and medium which is the blue 198 00:06:58,980 --> 00:06:57,580 and the yellow once again you can see 199 00:07:03,030 --> 00:06:58,990 that the lines are still becoming very 200 00:07:04,590 --> 00:07:03,040 indiscernible and then here what we've 201 00:07:06,270 --> 00:07:04,600 done this is where our last step which 202 00:07:07,950 --> 00:07:06,280 was where we use lavars cronograph to 203 00:07:09,810 --> 00:07:07,960 basically give us direct imagery or the 204 00:07:11,910 --> 00:07:09,820 actual process in which the observer 205 00:07:13,710 --> 00:07:11,920 would actually see these fluxes and as 206 00:07:15,720 --> 00:07:13,720 you can see that you're still seeing the 207 00:07:17,790 --> 00:07:15,730 same spectral features across various 208 00:07:19,590 --> 00:07:17,800 wavelengths but you can also take in 209 00:07:23,700 --> 00:07:19,600 combination of signal-to-noise ratio as 210 00:07:25,200 --> 00:07:23,710 well as instrument parameters so in 211 00:07:27,270 --> 00:07:25,210 conclusion what you've seen here is that 212 00:07:28,680 --> 00:07:27,280 you have high co2 and high methane which 213 00:07:30,180 --> 00:07:28,690 means that you have detectable methane 214 00:07:31,530 --> 00:07:30,190 which means that you actually have the 215 00:07:32,940 --> 00:07:31,540 signs of life which is what we want 216 00:07:35,880 --> 00:07:32,950 methane production rates that are 217 00:07:37,560 --> 00:07:35,890 comfortable to biology and then lastly 218 00:07:39,660 --> 00:07:37,570 when you have increasing atmospheric co2 219 00:07:41,280 --> 00:07:39,670 you know that you decrease the amount of 220 00:07:42,720 --> 00:07:41,290 methane is that skimming your Emma 221 00:07:45,270 --> 00:07:42,730 sphere and dust that makes your methane 222 00:07:47,040 --> 00:07:45,280 less detectable and then of course that 223 00:07:48,840 --> 00:07:47,050 when we start to think about project men 224 00:07:50,700 --> 00:07:48,850 about missions such as lovara we know 225 00:07:52,560 --> 00:07:50,710 that we can detect that methane across 226 00:07:55,980 --> 00:07:52,570 various wavelengths and there when you 227 00:07:57,330 --> 00:07:55,990 have very high methane so as our future 228 00:07:58,800 --> 00:07:57,340 directions been moving forward what we 229 00:08:00,840 --> 00:07:58,810 hope to do is that we're going to change 230 00:08:03,510 --> 00:08:00,850 the parent star so in this case we are 231 00:08:05,820 --> 00:08:03,520 dealing with our qiansun we have tipless 232 00:08:07,890 --> 00:08:05,830 in our model that allow us to model 233 00:08:09,810 --> 00:08:07,900 indoor such as ad leo and Proxima 234 00:08:11,190 --> 00:08:09,820 Centauri and we know that those type 235 00:08:12,540 --> 00:08:11,200 when you change those start stellar 236 00:08:14,330 --> 00:08:12,550 types we know that they can change the 237 00:08:16,740 --> 00:08:14,340 spectral features that you're seeing 238 00:08:17,760 --> 00:08:16,750 another thing that we can also do is 239 00:08:19,260 --> 00:08:17,770 that we're looking at changing the 240 00:08:21,360 --> 00:08:19,270 planetary distance from the parent star 241 00:08:23,640 --> 00:08:21,370 which in that case what we do is that 242 00:08:25,560 --> 00:08:23,650 we're currently at 1 au which is where 243 00:08:27,510 --> 00:08:25,570 Earth is currently and that when you 244 00:08:30,480 --> 00:08:27,520 also change those pros distance between 245 00:08:32,190 --> 00:08:30,490 the star between the star you know that 246 00:08:34,980 --> 00:08:32,200 you can also see different spectral 247 00:08:36,750 --> 00:08:34,990 features as well and then lastly another 248 00:08:38,760 --> 00:08:36,760 long term goals that we could actually 249 00:08:40,230 --> 00:08:38,770 use an Earth System model known as genie 250 00:08:41,969 --> 00:08:40,240 it's actually Spore the boundary 251 00:08:46,800 --> 00:08:41,979 conditions for what it called for a body 252 00:08:54,060 --> 00:08:46,810 methane production and then I'm ready 253 00:09:15,220 --> 00:09:11,260 Thank You Alina questions I think it's 254 00:09:18,210 --> 00:09:15,230 all ok 255 00:09:21,610 --> 00:09:18,220 David Kaplan University of Washington so 256 00:09:23,889 --> 00:09:21,620 on the the paper that Josh croissants 257 00:09:26,889 --> 00:09:23,899 and Taunton did I'm he said I was his 258 00:09:30,760 --> 00:09:26,899 advisor we also talked about carbon 259 00:09:32,470 --> 00:09:30,770 monoxide and the idea was that on a 260 00:09:35,860 --> 00:09:32,480 biological planet it should get eaten 261 00:09:37,269 --> 00:09:35,870 and so if it's less than about 100 ppm I 262 00:09:40,360 --> 00:09:37,279 mean it depends on the spectrum of the 263 00:09:42,370 --> 00:09:40,370 star as Eddy sweetie Moniz looked at but 264 00:09:44,010 --> 00:09:42,380 is that something else that maybe you 265 00:09:46,510 --> 00:09:44,020 could you could also consider that 266 00:09:49,000 --> 00:09:46,520 because if it's if it's very high at Sur 267 00:09:51,250 --> 00:09:49,010 sort of anti bio signature and if it's 268 00:09:53,800 --> 00:09:51,260 very low that's consistent with biology 269 00:09:55,990 --> 00:09:53,810 so there's an additional diagnostic that 270 00:09:58,780 --> 00:09:56,000 you can use besides the high methane 271 00:10:00,340 --> 00:09:58,790 levels and so it's just a comment really 272 00:10:02,410 --> 00:10:00,350 that that would also be an interesting 273 00:10:03,760 --> 00:10:02,420 thing to look at and thanks very much 274 00:10:11,440 --> 00:10:03,770 for your talk by the way which is very 275 00:10:13,630 --> 00:10:11,450 clear very nice yeah thank you thank you 276 00:10:15,660 --> 00:10:13,640 for your time and I appreciate have an