1 00:00:03,270 --> 00:00:02,790 hello everyone my name is alexander 2 00:00:06,470 --> 00:00:03,280 thielen 3 00:00:08,390 --> 00:00:06,480 i'm an astrobiology npp postdoc at 4 00:00:10,150 --> 00:00:08,400 assets goddard space flight center 5 00:00:11,669 --> 00:00:10,160 and thank you for joining me today at 6 00:00:13,589 --> 00:00:11,679 april icon where i'll be talking about 7 00:00:15,190 --> 00:00:13,599 the exploration of titan's atmospheric 8 00:00:18,470 --> 00:00:15,200 chemistry and dynamical state 9 00:00:20,070 --> 00:00:18,480 with alma titan herbert is a substantial 10 00:00:21,590 --> 00:00:20,080 atmosphere which is primarily composed 11 00:00:23,029 --> 00:00:21,600 of molecular nitrogen 12 00:00:24,950 --> 00:00:23,039 there's also a small percentage of 13 00:00:26,550 --> 00:00:24,960 methane molecular hydrogen and all of 14 00:00:27,269 --> 00:00:26,560 these species are dissociated and 15 00:00:30,310 --> 00:00:27,279 recombined 16 00:00:31,429 --> 00:00:30,320 into a wealth of organic compounds today 17 00:00:33,190 --> 00:00:31,439 we'll be talking about mostly 18 00:00:34,470 --> 00:00:33,200 hydrocarbon and nitrile species but 19 00:00:36,709 --> 00:00:34,480 there are also some oxygen burying 20 00:00:38,869 --> 00:00:36,719 species such as carbon monoxide and a 21 00:00:40,630 --> 00:00:38,879 wealth of yet to be identified 22 00:00:41,910 --> 00:00:40,640 heavy ionospheric species in the upper 23 00:00:43,830 --> 00:00:41,920 atmosphere 24 00:00:45,110 --> 00:00:43,840 over on the right we have a temperature 25 00:00:48,549 --> 00:00:45,120 profile of 26 00:00:49,910 --> 00:00:48,559 the earth and these are remarkably 27 00:00:51,270 --> 00:00:49,920 similar in shape although titan's 28 00:00:54,069 --> 00:00:51,280 profile is much more extended 29 00:00:55,270 --> 00:00:54,079 and much colder the study of titan and 30 00:00:56,069 --> 00:00:55,280 the sub millimeter which we'll be 31 00:00:59,510 --> 00:00:56,079 discussing today 32 00:01:01,750 --> 00:00:59,520 between about a 1070 kilometers 33 00:01:03,750 --> 00:01:01,760 is comparable to previous observations 34 00:01:04,229 --> 00:01:03,760 by the cassini spacecraft and those from 35 00:01:07,429 --> 00:01:04,239 the ground 36 00:01:08,950 --> 00:01:07,439 in the uv and in the infrared the 37 00:01:10,390 --> 00:01:08,960 combination of all of these studies 38 00:01:11,030 --> 00:01:10,400 allows us to characterize titan's 39 00:01:13,270 --> 00:01:11,040 atmosphere 40 00:01:14,550 --> 00:01:13,280 chemically and dynamically and allows us 41 00:01:17,109 --> 00:01:14,560 to answer some questions 42 00:01:19,030 --> 00:01:17,119 such as how extensive is the atmospheric 43 00:01:20,710 --> 00:01:19,040 chemistry and the molecular inventory 44 00:01:22,390 --> 00:01:20,720 of titan and how are these trace 45 00:01:23,590 --> 00:01:22,400 constituents distributed spatially and 46 00:01:25,910 --> 00:01:23,600 temporally 47 00:01:27,990 --> 00:01:25,920 for interest to astrobiology we also 48 00:01:29,749 --> 00:01:28,000 wonder how are these species able to 49 00:01:31,749 --> 00:01:29,759 interact with the surface and possibly 50 00:01:33,350 --> 00:01:31,759 tighten the subsurface ocean 51 00:01:35,190 --> 00:01:33,360 to try to answer some of these questions 52 00:01:37,030 --> 00:01:35,200 we use the atacama large millimeters 53 00:01:38,870 --> 00:01:37,040 submillimeter array or alma which is 54 00:01:41,429 --> 00:01:38,880 located high in the chilean desert 55 00:01:43,670 --> 00:01:41,439 close to 5000 meters in altitude almost 56 00:01:46,069 --> 00:01:43,680 comprised of 66 antenna dishes 57 00:01:47,030 --> 00:01:46,079 in multiple different arrays and these 58 00:01:49,749 --> 00:01:47,040 are movable 59 00:01:51,830 --> 00:01:49,759 which allows for baselines between 150 60 00:01:54,389 --> 00:01:51,840 meters and 16 kilometers 61 00:01:55,190 --> 00:01:54,399 this enables fairly high spatial 62 00:01:58,069 --> 00:01:55,200 resolution 63 00:01:59,749 --> 00:01:58,079 at these long wavelengths and you can 64 00:02:02,469 --> 00:01:59,759 see that titan is a fairly 65 00:02:03,429 --> 00:02:02,479 bright and compact continuum source at 66 00:02:05,749 --> 00:02:03,439 these frequencies 67 00:02:07,109 --> 00:02:05,759 and as such alma used titan for a number 68 00:02:09,669 --> 00:02:07,119 of different flux calibration 69 00:02:11,190 --> 00:02:09,679 observations since its inception in 2011 70 00:02:12,470 --> 00:02:11,200 all the way until 2017 71 00:02:14,550 --> 00:02:12,480 so there's a wealth of titan 72 00:02:17,830 --> 00:02:14,560 observations that are available on the 73 00:02:20,150 --> 00:02:17,840 alma science archive for us to use 74 00:02:21,350 --> 00:02:20,160 when looking through the alma flux 75 00:02:23,030 --> 00:02:21,360 calibration archive 76 00:02:25,510 --> 00:02:23,040 of titan observations we quickly found 77 00:02:26,229 --> 00:02:25,520 that alma has a variety of capabilities 78 00:02:27,830 --> 00:02:26,239 that are 79 00:02:29,589 --> 00:02:27,840 suitable for planetary atmosphere 80 00:02:32,229 --> 00:02:29,599 studies in addition to those of 81 00:02:34,630 --> 00:02:32,239 astrophysical and extra galactic sources 82 00:02:36,790 --> 00:02:34,640 this includes the coverage of numerous 83 00:02:37,990 --> 00:02:36,800 molecular species which may appear in 84 00:02:40,390 --> 00:02:38,000 planetary atmospheres 85 00:02:41,270 --> 00:02:40,400 for chemistry and isotopic ratio studies 86 00:02:43,509 --> 00:02:41,280 the high 87 00:02:44,790 --> 00:02:43,519 spectral resolution of alma heterodyne 88 00:02:46,630 --> 00:02:44,800 spectra allow for 89 00:02:48,470 --> 00:02:46,640 wind speed measurements through doppler 90 00:02:50,390 --> 00:02:48,480 shift and also to resolve 91 00:02:51,990 --> 00:02:50,400 atmospheric emission lines which allow 92 00:02:55,430 --> 00:02:52,000 you to measure the temperature 93 00:02:57,350 --> 00:02:55,440 the abundance of gas with altitude 94 00:02:58,869 --> 00:02:57,360 the spatial resolution as mentioned 95 00:03:01,350 --> 00:02:58,879 before allows us to map 96 00:03:03,350 --> 00:03:01,360 these things instantaneously to look at 97 00:03:05,350 --> 00:03:03,360 abundance or brightness temperature maps 98 00:03:06,710 --> 00:03:05,360 and the sensitivity of the array as a 99 00:03:08,309 --> 00:03:06,720 whole allows for 100 00:03:09,910 --> 00:03:08,319 new molecular detections in the 101 00:03:12,070 --> 00:03:09,920 atmosphere of titan and other solar 102 00:03:14,710 --> 00:03:12,080 system targets 103 00:03:16,149 --> 00:03:14,720 here's a representative spectrum of 104 00:03:18,149 --> 00:03:16,159 titan which is actually obtained from 105 00:03:19,430 --> 00:03:18,159 flux calibration observations so roughly 106 00:03:22,070 --> 00:03:19,440 two and a half minutes 107 00:03:23,190 --> 00:03:22,080 on source during 2014 but even in this 108 00:03:25,190 --> 00:03:23,200 short integration 109 00:03:27,110 --> 00:03:25,200 we can see the richness of these 110 00:03:29,110 --> 00:03:27,120 submillimeter spectra 111 00:03:30,630 --> 00:03:29,120 over on the left we have a band of 112 00:03:31,990 --> 00:03:30,640 acetonitrile we have these two 113 00:03:34,309 --> 00:03:32,000 relatively strong lines 114 00:03:35,270 --> 00:03:34,319 of hydrogen cyanide isotopes the carbon 115 00:03:38,070 --> 00:03:35,280 and nitrogen 116 00:03:38,630 --> 00:03:38,080 isotopes and then we even have some low 117 00:03:40,390 --> 00:03:38,640 signal 118 00:03:41,670 --> 00:03:40,400 acrylonitrile or ethyl cyanide 119 00:03:43,270 --> 00:03:41,680 transitions here 120 00:03:44,710 --> 00:03:43,280 so analyzing these spectra in a number 121 00:03:46,309 --> 00:03:44,720 of different ways will 122 00:03:48,630 --> 00:03:46,319 allow us to complete some of the 123 00:03:51,350 --> 00:03:48,640 projects that i'll describe 124 00:03:51,830 --> 00:03:51,360 here after and even just integrating 125 00:03:54,869 --> 00:03:51,840 over 126 00:03:55,750 --> 00:03:54,879 these spectral lines you can obtain 127 00:03:57,830 --> 00:03:55,760 these nice 128 00:03:59,110 --> 00:03:57,840 emission maps which will show you a 129 00:04:01,350 --> 00:03:59,120 snapshot view 130 00:04:02,309 --> 00:04:01,360 of the distribution of a given molecular 131 00:04:04,309 --> 00:04:02,319 species 132 00:04:05,350 --> 00:04:04,319 at a certain time when the observation 133 00:04:07,910 --> 00:04:05,360 was taken so 134 00:04:09,670 --> 00:04:07,920 on the top row we have hc3n or 135 00:04:12,229 --> 00:04:09,680 cyanoacetylene which we can see 136 00:04:14,470 --> 00:04:12,239 very rapidly transitions from the north 137 00:04:17,270 --> 00:04:14,480 pole to the south pole during 138 00:04:18,229 --> 00:04:17,280 2012 to 2015 and this is because of the 139 00:04:20,310 --> 00:04:18,239 relatively 140 00:04:21,670 --> 00:04:20,320 short photochemical lifetime of this 141 00:04:24,390 --> 00:04:21,680 species whereas 142 00:04:25,510 --> 00:04:24,400 in contrast the bottom row we can see 143 00:04:27,110 --> 00:04:25,520 ch3cn 144 00:04:29,990 --> 00:04:27,120 or pseudonitrile which we showed 145 00:04:32,870 --> 00:04:30,000 previously which stays at the north pole 146 00:04:34,230 --> 00:04:32,880 much longer than saturn acetylene 147 00:04:35,270 --> 00:04:34,240 because of its long photochemical 148 00:04:38,150 --> 00:04:35,280 lifetime which 149 00:04:40,390 --> 00:04:38,160 makes it a good tracer of the dynamics 150 00:04:42,310 --> 00:04:40,400 of titan's atmosphere 151 00:04:44,310 --> 00:04:42,320 there's a few ways that we can assess 152 00:04:46,390 --> 00:04:44,320 titan's dynamical state using 153 00:04:48,150 --> 00:04:46,400 alma observations the first is through 154 00:04:51,030 --> 00:04:48,160 the retrieval of temperature 155 00:04:51,830 --> 00:04:51,040 from carbon monoxide from roughly the 156 00:04:53,909 --> 00:04:51,840 tropopause 157 00:04:55,270 --> 00:04:53,919 around 60 kilometers to the lower 158 00:04:58,070 --> 00:04:55,280 mesosphere above 159 00:04:59,670 --> 00:04:58,080 500 kilometers and this is because co is 160 00:05:01,430 --> 00:04:59,680 well mixed in the atmosphere titan at 161 00:05:04,230 --> 00:05:01,440 roughly 50 parts per million 162 00:05:05,110 --> 00:05:04,240 so here is a composition of different 163 00:05:07,430 --> 00:05:05,120 radio transfer 164 00:05:08,870 --> 00:05:07,440 retrieval results of titan's temperature 165 00:05:10,150 --> 00:05:08,880 at different latitudes which i've made 166 00:05:13,909 --> 00:05:10,160 into a temperature map 167 00:05:14,950 --> 00:05:13,919 during 2017 in titan's northern summer 168 00:05:16,870 --> 00:05:14,960 solstice 169 00:05:19,270 --> 00:05:16,880 so we can see a large warming that 170 00:05:21,909 --> 00:05:19,280 occurs at the 171 00:05:22,790 --> 00:05:21,919 subsolar latitudes around 26 north but 172 00:05:24,469 --> 00:05:22,800 there's also 173 00:05:25,990 --> 00:05:24,479 warming that's occurring in the 174 00:05:28,710 --> 00:05:26,000 stratopause 175 00:05:29,909 --> 00:05:28,720 at the north polar region and the mid 176 00:05:32,390 --> 00:05:29,919 southern latitudes 177 00:05:34,230 --> 00:05:32,400 and this is indicative of titan's global 178 00:05:37,110 --> 00:05:34,240 pole the pole circulation cell 179 00:05:38,070 --> 00:05:37,120 which is currently lofting air from the 180 00:05:41,189 --> 00:05:38,080 northern or 181 00:05:44,070 --> 00:05:41,199 summer pole down into the southern 182 00:05:45,510 --> 00:05:44,080 winter pole we can measure titan's 183 00:05:47,510 --> 00:05:45,520 atmospheric temperature further up in 184 00:05:48,310 --> 00:05:47,520 the atmosphere using emission lines of 185 00:05:50,469 --> 00:05:48,320 hcn 186 00:05:51,990 --> 00:05:50,479 as you can see over here on the left 187 00:05:55,749 --> 00:05:52,000 these really broad features 188 00:05:58,790 --> 00:05:55,759 allow us to sound temperatures into the 189 00:05:59,590 --> 00:05:58,800 800 and 900 kilometer range and in 190 00:06:02,469 --> 00:05:59,600 particular 191 00:06:04,390 --> 00:06:02,479 this absorption core in the hdm spectra 192 00:06:05,749 --> 00:06:04,400 allows us to infer the mesopause 193 00:06:05,990 --> 00:06:05,759 temperature of titan which hasn't really 194 00:06:08,629 --> 00:06:06,000 been 195 00:06:09,350 --> 00:06:08,639 studied in depth with latitude or with 196 00:06:11,350 --> 00:06:09,360 time 197 00:06:12,790 --> 00:06:11,360 before these analyses so this is a 198 00:06:13,749 --> 00:06:12,800 preliminary result but we're seeing 199 00:06:16,070 --> 00:06:13,759 already from 200 00:06:16,790 --> 00:06:16,080 observations that the mesopause likely 201 00:06:18,870 --> 00:06:16,800 varies 202 00:06:20,790 --> 00:06:18,880 significantly in both its altitude and 203 00:06:23,909 --> 00:06:20,800 its temperature measurement 204 00:06:25,830 --> 00:06:23,919 so this is you know largely due to wave 205 00:06:27,350 --> 00:06:25,840 motion and changes in the atmospheric 206 00:06:29,029 --> 00:06:27,360 composition which can have effects on 207 00:06:30,870 --> 00:06:29,039 the radiative energy budget 208 00:06:33,350 --> 00:06:30,880 of titan's atmosphere we've previously 209 00:06:36,309 --> 00:06:33,360 seen that this portion of the atmosphere 210 00:06:39,590 --> 00:06:36,319 is really variable with time from 211 00:06:43,270 --> 00:06:41,430 alma's high spectral resolution 212 00:06:45,510 --> 00:06:43,280 capabilities allow us to 213 00:06:46,790 --> 00:06:45,520 observe doppler shifts in emission lines 214 00:06:50,469 --> 00:06:46,800 of rotational spectra 215 00:06:52,469 --> 00:06:50,479 which we can directly map to wind 216 00:06:54,710 --> 00:06:52,479 speed magnitudes in the atmosphere of 217 00:06:57,189 --> 00:06:54,720 titan depending on what chemical species 218 00:06:59,510 --> 00:06:57,199 you're observing you can look between 219 00:07:00,790 --> 00:06:59,520 300 and 1000 kilometers in the 220 00:07:01,350 --> 00:07:00,800 atmosphere depending on where the 221 00:07:04,390 --> 00:07:01,360 species 222 00:07:06,790 --> 00:07:04,400 line core is sensitive to emission so 223 00:07:07,870 --> 00:07:06,800 in martin coroner's paper from last year 224 00:07:12,230 --> 00:07:07,880 we were looking at 225 00:07:15,189 --> 00:07:12,240 ch3cn hc3n and hnc 226 00:07:15,830 --> 00:07:15,199 wind maps from 2017 and comparing those 227 00:07:18,870 --> 00:07:15,840 to 228 00:07:21,749 --> 00:07:18,880 the published ones in 2016 from luciano 229 00:07:23,350 --> 00:07:21,759 where they found a thermospheric jet in 230 00:07:24,230 --> 00:07:23,360 titan's upper atmosphere around the 231 00:07:26,469 --> 00:07:24,240 equator 232 00:07:28,070 --> 00:07:26,479 our wind speed measurements showed a 233 00:07:31,830 --> 00:07:28,080 dramatic decrease 234 00:07:34,070 --> 00:07:31,840 over this nine-month period of about 47 235 00:07:35,749 --> 00:07:34,080 which is due to a dynamical instability 236 00:07:36,950 --> 00:07:35,759 or variable wave activity 237 00:07:39,990 --> 00:07:36,960 between the middle and the upper 238 00:07:41,589 --> 00:07:40,000 atmosphere of titan which is really cool 239 00:07:43,029 --> 00:07:41,599 now moving on to some chemistry and 240 00:07:44,950 --> 00:07:43,039 composition studies which 241 00:07:46,550 --> 00:07:44,960 are possible from these alma 242 00:07:48,150 --> 00:07:46,560 observations we can take the 243 00:07:49,830 --> 00:07:48,160 temperatures that we retrieved earlier 244 00:07:51,670 --> 00:07:49,840 from co and acn 245 00:07:53,430 --> 00:07:51,680 and use them to do radio transfer 246 00:07:56,230 --> 00:07:53,440 analysis in multiple occasions on 247 00:07:58,309 --> 00:07:56,240 titan's disk to make these abundance 248 00:07:59,110 --> 00:07:58,319 maps with latitude and altitude or 249 00:08:01,589 --> 00:07:59,120 pressure 250 00:08:02,629 --> 00:08:01,599 so on the left we have a map of 251 00:08:04,950 --> 00:08:02,639 cytoacetylene 252 00:08:05,830 --> 00:08:04,960 with altitude and on the right we have a 253 00:08:08,550 --> 00:08:05,840 pseudo nitrile 254 00:08:09,110 --> 00:08:08,560 and again similar to the maps that i 255 00:08:11,830 --> 00:08:09,120 showed 256 00:08:12,869 --> 00:08:11,840 a few slides ago both of these molecules 257 00:08:15,430 --> 00:08:12,879 have an abundance 258 00:08:17,430 --> 00:08:15,440 enhancement towards the pole and in 259 00:08:19,189 --> 00:08:17,440 particular the enhancement of the south 260 00:08:21,990 --> 00:08:19,199 pole compared to the equator 261 00:08:23,350 --> 00:08:22,000 for these species varies by an order of 262 00:08:26,550 --> 00:08:23,360 magnitude which is 263 00:08:28,550 --> 00:08:26,560 really interesting and the global 264 00:08:29,909 --> 00:08:28,560 circulation of titan's pole the pole 265 00:08:32,149 --> 00:08:29,919 cell is also evident 266 00:08:33,190 --> 00:08:32,159 here in the enhancement above the south 267 00:08:36,149 --> 00:08:33,200 pole and 268 00:08:38,310 --> 00:08:36,159 the relative dearth of each of these 269 00:08:41,990 --> 00:08:38,320 molecular species towards the equator or 270 00:08:46,630 --> 00:08:45,030 and maybe more exciting is the detection 271 00:08:48,310 --> 00:08:46,640 of a new molecular species 272 00:08:49,990 --> 00:08:48,320 in titan's atmosphere which has a lot of 273 00:08:53,190 --> 00:08:50,000 applications for both 274 00:08:54,630 --> 00:08:53,200 its overall chemistry feedback into its 275 00:08:56,710 --> 00:08:54,640 atmospheric dynamics and for 276 00:08:59,350 --> 00:08:56,720 perspectives on astrobiology 277 00:09:00,910 --> 00:08:59,360 previous detections from our group early 278 00:09:03,829 --> 00:09:00,920 on included 279 00:09:06,470 --> 00:09:03,839 c2h5cn or just ethyl cyanide on the top 280 00:09:07,990 --> 00:09:06,480 and c2h3cn which is vinyl side on the 281 00:09:11,030 --> 00:09:08,000 bottom which had a lot of interest 282 00:09:13,190 --> 00:09:11,040 from the astrobiology community and 283 00:09:14,630 --> 00:09:13,200 last year we made two new molecular 284 00:09:17,310 --> 00:09:14,640 detections in the atmosphere of titan 285 00:09:18,870 --> 00:09:17,320 using dedicated alma observations from 286 00:09:20,710 --> 00:09:18,880 2016-2019 287 00:09:22,790 --> 00:09:20,720 on the top i'm showing the detection of 288 00:09:26,070 --> 00:09:22,800 methyl cyanoacetylene in this 289 00:09:29,350 --> 00:09:26,080 purple spectrum inset from our 2019 data 290 00:09:32,630 --> 00:09:29,360 and this molecule ch3c3n is 291 00:09:34,870 --> 00:09:32,640 the largest nitrogen bearing species 292 00:09:36,070 --> 00:09:34,880 that we've found thus far also has a 293 00:09:39,389 --> 00:09:36,080 really long name 294 00:09:41,509 --> 00:09:39,399 and in contrast to this molecule is 295 00:09:43,350 --> 00:09:41,519 cyclopropanilidine which also has a long 296 00:09:46,150 --> 00:09:43,360 name and is the smallest 297 00:09:47,990 --> 00:09:46,160 cyclic molecule that we found thus far 298 00:09:49,829 --> 00:09:48,000 in any solar system object 299 00:09:51,990 --> 00:09:49,839 both of these molecules have column 300 00:09:53,829 --> 00:09:52,000 density measurements which are 301 00:09:56,310 --> 00:09:53,839 far below everything else that we've 302 00:09:59,190 --> 00:09:56,320 found thus far in titan's atmosphere 303 00:10:00,870 --> 00:09:59,200 so alma really is one of the best tools 304 00:10:04,150 --> 00:10:00,880 that we have in the moment to push 305 00:10:05,990 --> 00:10:04,160 the molecular inventory and the you know 306 00:10:08,870 --> 00:10:06,000 photochemical products of titan's 307 00:10:10,790 --> 00:10:08,880 atmosphere even further 308 00:10:12,310 --> 00:10:10,800 finally alma allows us to observe many 309 00:10:13,829 --> 00:10:12,320 different isotopic species in the 310 00:10:17,030 --> 00:10:13,839 atmosphere of titan on the top 311 00:10:19,110 --> 00:10:17,040 row we have ch3d as well as isotopes of 312 00:10:22,710 --> 00:10:19,120 hcn and on the bottom right we have 313 00:10:25,110 --> 00:10:22,720 co and ch3 cn isotopes 314 00:10:26,389 --> 00:10:25,120 shown and their respective values are 315 00:10:28,949 --> 00:10:26,399 printed below 316 00:10:31,030 --> 00:10:28,959 the investigation of isotope ratios 317 00:10:32,949 --> 00:10:31,040 gives us insights into the formation and 318 00:10:36,069 --> 00:10:32,959 evolution of the atmosphere of titan 319 00:10:38,150 --> 00:10:36,079 and nitrogen and carbon ratios give us 320 00:10:40,710 --> 00:10:38,160 some insights into the selective 321 00:10:42,069 --> 00:10:40,720 isotopic fractionation that happens in 322 00:10:44,069 --> 00:10:42,079 the upper atmosphere 323 00:10:46,150 --> 00:10:44,079 the dh ratio of titan is interesting 324 00:10:48,310 --> 00:10:46,160 because it's an order of magnitude 325 00:10:49,269 --> 00:10:48,320 higher than that of saturn or jupiter is 326 00:10:51,829 --> 00:10:49,279 much more in line 327 00:10:53,350 --> 00:10:51,839 with the oceans on earth similarly the 328 00:10:57,030 --> 00:10:53,360 oxygen ratios on titan are pretty 329 00:10:59,910 --> 00:10:58,949 so in summary this was a collection of 330 00:11:00,710 --> 00:10:59,920 different projects that we've been 331 00:11:03,509 --> 00:11:00,720 working on 332 00:11:04,230 --> 00:11:03,519 and nasa are using alma to observe titan 333 00:11:06,150 --> 00:11:04,240 and also 334 00:11:08,150 --> 00:11:06,160 now to observe other planetary 335 00:11:08,790 --> 00:11:08,160 atmospheres but alma is a really great 336 00:11:10,550 --> 00:11:08,800 tool 337 00:11:12,310 --> 00:11:10,560 to look at the spatial and temporal 338 00:11:12,949 --> 00:11:12,320 variations in the temperature the 339 00:11:15,350 --> 00:11:12,959 abundance 340 00:11:17,509 --> 00:11:15,360 and the wind speeds of different plants 341 00:11:19,509 --> 00:11:17,519 and its high sensitivity allows for 342 00:11:21,829 --> 00:11:19,519 the detection of new complex molecular 343 00:11:23,829 --> 00:11:21,839 species and also isotopes 344 00:11:24,949 --> 00:11:23,839 these things together allow us to 345 00:11:27,269 --> 00:11:24,959 examine the 346 00:11:28,470 --> 00:11:27,279 chemical complexity and the evolution of 347 00:11:30,310 --> 00:11:28,480 planetary atmospheres 348 00:11:31,670 --> 00:11:30,320 and for titan in particular allows us to 349 00:11:32,630 --> 00:11:31,680 continue the legacy of the cassini 350 00:11:35,110 --> 00:11:32,640 huygens mission 351 00:11:36,230 --> 00:11:35,120 after its end in 2017 and observe 352 00:11:37,910 --> 00:11:36,240 seasonal changes 353 00:11:40,069 --> 00:11:37,920 in titan after its northern summer 354 00:11:41,990 --> 00:11:40,079 solstice these measurements will help us 355 00:11:45,030 --> 00:11:42,000 to constrain photochemical and dynamical 356 00:11:47,350 --> 00:11:45,040 models of titan's atmosphere and 357 00:11:49,190 --> 00:11:47,360 we'll hopefully get more observations 358 00:11:50,150 --> 00:11:49,200 that are dedicated observations of titan 359 00:11:51,430 --> 00:11:50,160 in the future