AST 251 Life on Other Worlds Dr. Michael Reid University of Toronto ast251@astro.utoronto.ca Credit: NASA/SETI/JPL How Do We Find Habitable Planets? AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 2 We have made an attempt to define “life” and establish its fundamental biochemistry. Now it’s time to investigate where in the cosmos life can survive. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 3 We refer to planets orbiting stars other than the Sun as extrasolar planets or exoplanets. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA Ames/JPL-Caltech/T. Pyle 4 You might imagine that we would find exoplanets by photographing them, the same way we do with other astronomical objects. This technique is known as direct imaging. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 5 Direct imaging is very difficult for the same reason it is difficult to photograph a firefly sitting on a car headlight. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: Flickr user mikelietz 6 messy stuff left over when we remove as much of the star’s light from the image as possible exoplanet AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto The Gemini Planet Imager on the Gemini South telescope in Chile imaged the star 51 Eridanus and found a new exoplanet (‘b’) in 2014 (McIntosh et al., Science, 2015) Credit: Gemini Observatory and J. Rameau (UdeM) and C. Marois NRC Herzberg 7 Planets orbiting the star HR 8799. This is typical of the level of detail we can see with direct imaging AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 8 The planets we can currently see using direct imaging are usually young, hot Jovian planets—not likely homes for life. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credits: Danielle Futselaar & Franck Marchis, SETI Institute 9 There are several other successful exoplanet detection methods, including: transits radial velocity/Doppler method astrometry pulsar timing transit timing variation microlensing AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 10 A transit occurs when one astronomical object passes in front of another from our point of view. star a transiting planet AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 11 A transit of the Moon across the Sun, as seen by the STEREO spacecraft AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/STEREO 12 We can’t actually see exoplanets transiting because we don’t have powerful enough telescopes to image the surfaces of distant stars. However, we can spot transits in a star’s light curve. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 13 star’s brightness The light curve of a star is a graph of the star’s brightness versus time time AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 14 star’s brightness ? time AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 15 Here, ingress and egress are too quick for you to see the slope (but you could see them if you could zoom the time axis). AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA 16 star’s brightness 1 Ingress and egress take time, so the light curve is sloped. 0.9999 time AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 17 Rstar star’s brightness Rplanet 1 Depth 0.99 time cross−sectional area of planet 𝐃𝐞𝐩𝐭𝐡 = cross−sectional area of star AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 18 Rstar star’s brightness Rplanet 1 Depth 0.99 time cross−sectional area of planet 𝐃𝐞𝐩𝐭𝐡 = cross−sectional area of star 𝛑𝐑𝟐𝐩𝐥𝐚𝐧𝐞𝐭 𝐃𝐞𝐩𝐭𝐡 = 𝛑𝐑𝟐𝐬𝐭𝐚𝐫 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 19 Rstar star’s brightness Rplanet 1 Depth 0.99 time cross−sectional area of planet 𝐃𝐞𝐩𝐭𝐡 = cross−sectional area of star 𝛑𝐑𝟐𝐩𝐥𝐚𝐧𝐞𝐭 𝐃𝐞𝐩𝐭𝐡 = 𝛑𝐑𝟐𝐬𝐭𝐚𝐫 𝐑 𝐩𝐥𝐚𝐧𝐞𝐭 = 𝐑 𝐬𝐭𝐚𝐫 𝐃𝐞𝐩𝐭𝐡 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 20 Measuring transit depths allows us to measure the sizes of each planet in an exoplanetary system, even though we can’t see the planets themselves. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/JPL-Caltech 21 Real transit light curves have some amount of “noise” in the data originating from elements of the telescope, detector, etc. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 22 In real situations, it’s often difficult to see the transit among all the “noise”. (Zhou et al., AJ, 2017) (Muirhead et al., ApJ, 2015) AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 23 If we only see one transit, we cannot be sure it is caused by an exoplanet. It could be caused by an asteroid in our own solar system, or a sunspot. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 24 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/SDO 25 To confirm that a transit is caused by a planet, we look for multiple transits repeating at regular intervals. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 26 The time it takes a planet to orbit its star is called the orbital period. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 27 If we know the orbital period of a planet, we can use Kepler’s Laws of planetary motion to calculate how far the planet is from the star— it’s orbital semi-major axis. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 28 The semi-major axis is crucial to determining habitability, as it tells us whether the planet is likely to be too hot, too cold, or just right for life. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: Carl Sagan Institute 29 German astronomer Johannes Kepler (1571-1630) worked out the three laws of planetary. Kepler’s laws are actually just consequences of Newton’s Law of Gravity, which hadn’t been discovered in Kepler’s time. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 30 Kepler’s First Law All planets orbit their parent stars in elliptical orbits with the star* at one focus. *This is technically not correct—the center of mass of the system is at one focus. However, in the general case that the star is much more massive than any of its planets, the difference is small. We will return to this point. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 31 focus semi-minor axis center semi-major axis, a c focus This ellipse has eccentricity = c/a = 0.6 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 32 center radius This ellipse has eccentricity = 0 (i.e. it’s a circle) AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 33 Orbits with different eccentricities (thicker line higher e) AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 34 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: YouTube user Ms. Edge 35 Kepler’s Second Law* As they orbit, planets sweep out equal areas in equal times. *This is the one that confuses everyone. It’s really a statement of the conservation of angular momentum. That language wasn’t accessible to Kepler. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 36 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 37 Snapshots of an orbiting planet spaced at equal times—the planet moves faster closer to the star. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 38 Kepler’s Third Law The square of a planet’s orbital period is proportional to the cube of its orbital semi-major axis. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 39 2a 𝟐 𝟒𝛑 𝐏𝟐 = 𝐚𝟑 𝐆(𝐌𝐩𝐥𝐚𝐧𝐞𝐭 + 𝐌𝐬𝐭𝐚𝐫 ) AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 40 If we assume the mass of the planet is much less than the mass of the star, we can use Kepler’s Third Law to work out the planet’s orbital semimajor axis from its orbital period: 𝟐 𝟒𝛑 𝐏𝟐 = 𝐚𝟑 𝐆(𝐌𝐩𝐥𝐚𝐧𝐞𝐭 + 𝐌𝐬𝐭𝐚𝐫 ) 𝟒𝛑𝟐 𝟑 𝐢𝐟 𝐌𝐬𝐭𝐚𝐫 ≫ 𝐌𝐩𝐥𝐚𝐧𝐞𝐭 ≅ 𝐚 𝐆𝐌𝐬𝐭𝐚𝐫 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 41 𝟐 𝟒𝛑 𝐏𝟐 = 𝐚𝟑 𝐆(𝐌𝐩𝐥𝐚𝐧𝐞𝐭 + 𝐌𝐬𝐭𝐚𝐫 ) 𝟐 𝟒𝛑 𝐏𝟐 ≅ 𝐚𝟑 𝐆𝐌𝐬𝐭𝐚𝐫 𝐆𝐌𝐬𝐭𝐚𝐫 𝟐 𝟑 𝐏 ≅ 𝐚 𝟒𝛑𝟐 𝐆𝐌𝐬𝐭𝐚𝐫 𝟐 𝒂≅ 𝐏 𝟐 𝟒𝛑 𝐛𝐞𝐜𝐚𝐮𝐬𝐞 𝐌𝐬𝐭𝐚𝐫 >> 𝐌𝐩𝐥𝐚𝐧𝐞𝐭 𝟏/𝟑 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 42 Let’s say P = 2.1 years and Mstar = 2.0 M☉. To find a, first convert everything to standard units (m, s, kg, etc.) AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 43 Let’s say P = 2.1 years and Mstar = 2.0 M☉. To find a, first convert everything to standard units (m, s, kg, etc.) Convert P to seconds: P = (2.1 y)(365.24 days/y)(86400 s/day) = 6.627 x 108 s AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 44 Let’s say P = 2.1 years and Mstar = 2.0 M☉. To find a, first convert everything to standard units (m, s, kg, etc.) Convert P to seconds: P = (2.1 y)(365.24 days/y)(86400 s/day) = 6.627 x 108 s Convert Mstar to kg: Mstar = 2MSun = (2)(1.989 x 1030 kg) = 3.978 x 1030 kg AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 45 Let’s say P = 2.1 years and Mstar = 2.0 M☉. To find a, first convert everything to standard units (m, s, kg, etc.) Convert P to seconds: P = (2.1 y)(365.24 days/y)(86400 s/day) = 6.627 x 108 s Convert Mstar to kg: Mstar = 2MSun = (2)(1.989 x 1030 kg) = 3.978 x 1030 kg (𝟔. 𝟔𝟕𝟒 × 𝟏𝟎−𝟏𝟏 𝐦𝟑 𝐤𝐠 −𝟏 𝐬−𝟐 )(𝟑. 𝟗𝟕𝟖 × 𝟏𝟎𝟑𝟎 𝐤𝐠) 𝐚≅ (𝟔. 𝟔𝟐𝟕 × 𝟏𝟎𝟖 𝐬)𝟐 𝟐 𝟒(𝟑. 𝟏𝟒𝟏𝟓𝟗) AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 𝟏/𝟑 46 Let’s say P = 2.1 years and Mstar = 2.0 M☉. To find a, first convert everything to standard units (m, s, kg, etc.) Convert P to seconds: P = (2.1 y)(365.24 days/y)(86400 s/day) = 6.627 x 108 s Convert Mstar to kg: Mstar = 2MSun = (2)(1.989 x 1030 kg) = 3.978 x 1030 kg (𝟔. 𝟔𝟕𝟒 × 𝟏𝟎−𝟏𝟏 𝐦𝟑 𝐤𝐠 −𝟏 𝐬−𝟐 )(𝟑. 𝟗𝟕𝟖 × 𝟏𝟎𝟑𝟎 𝐤𝐠) 𝐚≅ (𝟔. 𝟔𝟐𝟕 × 𝟏𝟎𝟖 𝐬)𝟐 𝟐 𝟒(𝟑. 𝟏𝟒𝟏𝟓𝟗) 𝟏/𝟑 𝐚 ≅ 𝟑. 𝟎𝟗 × 𝟏𝟎𝟏𝟏 𝐦 = 2.1 AU AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 47 1 AU = 1 Astronomical Unit 1 AU ≈ average distance between Earth and the Sun ≈ 150 million km AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: Wikimedia Commons user Huritisho 48 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 49 star’s brightness 1 time If the cadence of your observations is too low, the curve can be difficult to interpret. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 50 star’s brightness 1 time If the cadence of your observations is too low, the curve can be difficult to interpret. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 51 star’s brightness Could there be a pair of missing transits? 1 time If the cadence of your observations is too low, the curve can be difficult to interpret. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 52 Lower cadence can also cause you to miss ingress and/or egress, which are typically very fast. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 53 As in our solar system, most stars seem to have multiple planets. How many do you see here? AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 54 As in our solar system, most stars seem to have multiple planets. How many do you see here? AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 55 Hands-on activity Using plot.ly to plot and examine light curves AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 56 Planets themselves emit & reflect light, which means that there’s a secondary eclipse when the planet passes behind the star. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 57 star brightness no eclipse (we see all of the light from the star and the planet) primary transit (planet covers star) secondary eclipse (star covers planet) time AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 58 It’s even possible to use transit light curves to learn about the surface temperature of a planet, but only rarely. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 59 Just before the secondary eclipse, the warmer, brighter day side of the planet points toward Earth. The cold hot sides are turned equally toward Earth. To distant Earth Only the cool night side faces Earth during the primary transit. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 60 The varying amount of light from the planet makes the light curve vary in brightnes, even between transits. (Demory et al., Nature, 2016) To distant Earth AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 61 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/JPL-Caltech/University of Cambridge 62 hot spot on the side of the planet which faces the parent star AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 63 Biases of the Transit Method AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 64 transit visible from Earth transit NOT visible from Earth The transit method can only detect planets whose orbits are edge-on to our line of sight. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 65 Easier to detect Harder to detect Planets with larger radii are easier to detect. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 66 Jupiter size Earth size The transit method has difficulty finding Earth-sized and smaller planets with current telescopes because smaller planets produce shallower transits. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 67 Results of the Transit Method AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 68 To date, the transit method has been by far the most successful planet-finding method. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 69 Exoplanets by discovery year and method AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 70 Much of the success of this method was due to the Kepler space telescope. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 71 Credit: NASA/Ames Research Center/W. Stenzel/D. Rutter Kepler was operational from 2009-2018. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 72 Kepler has expanded the range of known types of planets beyond those known from our own solar system. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 73 “gas giants” terrestrial planets ice giants jovians Planets to scale; distances not to scale. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA 74 Terrestrial planets: mainly rock with thin atmospheres AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/JPL 75 Jovian planets: liquid hydrogen with thick gaseous atmospheres. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 76 Ice giants/Neptunian: slushy liquid interiors with thick gaseous atmospheres AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 77 Exoplanets come in types not present in our solar system: hot Jupiters super-Jupiters super-Earths mini-Neptunes lava worlds ocean worlds … AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 78 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/Kepler 79 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA Ames/W. Stenzel 80 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/Kepler 81 There seems to be a real lack of planets in the range around 1.75 Earth radii. What could be the cause? AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/Kepler 82 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA/Kepler 83 Using the method of transit spectroscopy, it is sometimes possible to measure the chemical composition of exoplanet’s atmosphere. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 84 Continuous spectrum Every atom and molecule absorbs a characteristic set of colours of light. If we measure transits in light of many different colours, we can spot deeper transits where particular chemicals are absorbing more light. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: astronoo.com 85 The transit depth will be shallower at a wavelength (colour) where no chemical is absorbing light from the star (so only the solid body of the planet blocks light). Credit: NASA's Goddard Space Flight Center, Additional animations courtesy ESA/Hubble The transit depth will be deeper at a wavelength (colour) where a particular chemical in the atmosphere is absorbing more light. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 86 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA's Goddard Space Flight Center, Additional animations courtesy ESA/Hubble 87 Transmission spectrum of the atmosphere of exoplanet WASP 19b. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: NASA's Goddard Space Flight Center, Additional animations courtesy ESA/Hubble 88 Credit: NASA/Ames Research Center/Wendy Stenzel and The University of Texas at Austin/Andrew Vanderburg AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 89 AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 90 Exomoons AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 91 As we have already seen, moons of giant planets may be the most numerous habitable environments in the cosmos. Can we detect moons of exoplanets—exomoons? AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 92 star’s brightness 1 0.9999 time AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 93 A planet with a moon will wobble as it orbits the star. The exact timing of consecutive transits will vary. (Kipping, 2014, arXiv:1405.1455) AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 94 In October 2018, the first evidence of an exomoon emerged. (Teachey & Kipping, Science, 2018) AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto Credit: Dan Durda 95 Questions? Meet me outside the classroom or visit me during office hours. AST 251: Life on Other Worlds | Dr. M. Reid | University of Toronto 96