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A dark gray and red sphere representing the Earth lies against a black background to the right of an orange circular object representing the Sun
Artist's concept of the carbonized Earth 7.9 billion years from now, after the Sun has entered the red giant stage.

While predictions of the future can never be absolutely certain,[1] present understanding in various scientific fields allows for the prediction of far-future events, if only in the broadest outline. These fields include astrophysics, which has revealed how planets and stars form, interact, and die; particle physics, which has revealed how matter behaves at the smallest scales; evolutionary biology, which predicts how life will evolve over time; and plate tectonics, which shows how continents shift over millennia.

All projections of the future of the Earth, the Solar System, and the universe must account for the second law of thermodynamics, which states that entropy, or a loss of the energy available to do work, must rise over time.[2] Stars will eventually exhaust their supply of hydrogen fuel and burn out. Close encounters gravitationally fling planets from their star systems, and star systems from galaxies.[3]

Eventually, matter itself is expected to come under the influence of radioactive decay, as even the most stable materials break apart into subatomic particles.[4] Current data suggest that the universe has a flat geometry (or very close to flat), and thus, will not collapse in on itself after a finite time,[5] and the infinite future allows for the occurrence of a number of massively improbable events, such as the formation of Boltzmann brains.[6]

The timelines displayed here cover events from the beginning of the 11th millennium[note 1] to the furthest reaches of future time. A number of alternative future events are listed to account for questions still unresolved, such as whether humans will become extinct, whether protons decay, and whether the earth survives when the sun expands to the red giant.

ꯆꯪꯒꯗꯕꯁꯤꯡ[edit | edit source]

Astronomy and astrophysics Astronomy and astrophysics
Geology and planetary science Geology and planetary science
Biology Biology
Particle physics Particle physics
Mathematics Mathematics
Technology and culture Technology and culture

ꯃꯂꯦꯝꯁꯤꯗ ꯑꯣꯏꯔꯛꯀꯗꯕ, ꯅꯨꯃꯤꯠꯀꯤ ꯑꯃꯁꯨꯡ ꯇꯥꯏꯄꯡꯄꯥꯜꯄꯥ[edit | edit source]

Template:See also

Key.svg Years from now Event
Geology and planetary science 10,000 If a failure of the Wilkes Subglacial Basin "ice plug" in the next few centuries were to endanger the East Antarctic Ice Sheet, it will take up to this long to melt completely. Sea levels would rise 3 to 4 meters.[7] (One of the potential long-term effects of global warming, this is separate from the shorter term threat of the West Antarctic Ice Sheet.)
Astronomy and astrophysics 10,000[note 2] The red supergiant star Antares will likely have exploded in a supernova. The explosion is expected to be easily visible in daylight.[8]
Geology and planetary science 15,000 According to the Sahara pump theory, the precession of Earth's poles will move the North African Monsoon far enough north to convert the Sahara back into a tropical climate, as it was during 5,000–10,000 years ago.[9][10]
Geology and planetary science 25,000 The northern Martian polar ice cap could recede as Mars reaches a warming peak of the northern hemisphere during the c. 50,000-year perihelion precession aspect of its Milankovitch cycle.[11][12]
Astronomy and astrophysics 36,000 The small red dwarf Ross 248 will pass within 3.024 light-years of Earth, becoming the closest star to the Sun.[13] It will recede after about 8,000 years, making first Alpha Centauri again and then Gliese 445 the nearest stars[13] (see timeline).
Geology and planetary science 50,000 According to Berger and Loutre, the current interglacial period ends[14] sending the Earth back into a glacial period of the current ice age, regardless of the effects of anthropogenic global warming.

Niagara Falls will have eroded away the remaining 32 km to Lake Erie, and ceased to exist.[15]

The many glacial lakes of the Canadian Shield will have been erased by post-glacial rebound and erosion.[16]

Astronomy and astrophysics 50,000 The length of the day used for astronomical timekeeping reaches about 86,401 SI seconds, due to lunar tides decelerating the Earth's rotation. Under the present-day timekeeping system, either a leap second would need to be added to the clock every single day, or else by then, in order to compensate, the length of the day would have had to have been officially lengthened by one SI second.[17]
Astronomy and astrophysics 100,000 The proper motion of stars across the celestial sphere, which is the result of their movement through the Milky Way, renders many of the constellations unrecognisable.[18]
Astronomy and astrophysics 100,000[note 2] The hypergiant star VY Canis Majoris will likely have exploded in a hypernova.[19]
Geology and planetary science 100,000[note 2] Earth will likely have undergone a supervolcanic eruption large enough to erupt Template:Convert of magma. For comparison, Lake Erie is Template:Convert.[20]
Biology 100,000 Native North American earthworms, such as Megascolecidae, will have naturally spread north through the United States Upper Midwest to the Canada–US border, recovering from the Laurentide Ice Sheet glaciation (38°N to 49°N), assuming a migration rate of 10 metres per year.[21] (However, non-native invasive earthworms of North America have already been introduced by humans on a much shorter timescale, causing a shock to the regional ecosystem.)
Geology and planetary science 100,000+ As one of the long-term effects of global warming, 10% of anthropogenic carbon dioxide will still remain in a stabilized atmosphere.[22]
Geology and planetary science 250,000 Lōʻihi, the youngest volcano in the Hawaiian–Emperor seamount chain, will rise above the surface of the ocean and become a new volcanic island.[23]
Astronomy and astrophysics c. 300,000[note 2] At some point in the next "several" hundred thousand years, the Wolf–Rayet star WR 104 is expected to explode in a supernova. It has been suggested that it may produce a gamma-ray burst that could pose a threat to life on Earth should its poles be aligned 12° or lower towards Earth. The star's axis of rotation has yet to be determined with certainty.[24]
Astronomy and astrophysics 500,000[note 2] Earth will likely have been hit by an asteroid of roughly 1 km in diameter, assuming it cannot be averted.[25]
Geology and planetary science 500,000 The rugged terrain of Badlands National Park in South Dakota will have eroded away completely.[26]
Geology and planetary science 950,000 Meteor Crater, a large impact crater in Arizona considered the "freshest" of its kind, will have eroded away.[27]
Geology and planetary science 1 million[note 2] Earth will likely have undergone a supervolcanic eruption large enough to erupt Template:Convert of magma, an event comparable to the Toba supereruption 75,000 years ago.[20]
Astronomy and astrophysics 1 million[note 2] Highest estimated time until the red supergiant star Betelgeuse explodes in a supernova. The explosion is expected to be easily visible in daylight.[28][29] It may explode in as little as 100,000 years, depending on the evolutionary model.
Astronomy and astrophysics 1 million[note 2] Desdemona and Cressida, moons of Uranus, will likely have collided.[30]
Astronomy and astrophysics 1.4 million The star Gliese 710 will pass as close as 9,000 AU (0.14 light-years to the Sun) before moving away. This will gravitationally perturb members of the Oort cloud, a halo of icy bodies orbiting at the edge of the Solar System, thereafter raising the likelihood of a cometary impact in the inner Solar System.[31]
Biology 2 million Estimated time for the recovery of coral reef ecosystems from human-caused ocean acidification; a similar time was taken for the recovery of marine ecosystems after the acidification event that occurred about 65 million years ago.[32]
Geology and planetary science 2 million+ The Grand Canyon will erode further, deepening slightly, but principally widening into a broad valley surrounding the Colorado River.[33]
Astronomy and astrophysics 2.7 million Average orbital half-life of current centaurs, that are unstable because of gravitational interaction of the several outer planets.[34] See predictions for notable centaurs.
Geology and planetary science 10 million The widening East African Rift valley is flooded by the Red Sea, causing a new ocean basin to divide the continent of Africa[35] and the African Plate into the newly formed Nubian Plate and the Somali Plate.
Biology 10 million Estimated time for full recovery of biodiversity after a potential Holocene extinction, if it were on the scale of the five previous major extinction events.[36]

Even without a mass extinction, by this time most current species will have disappeared through the background extinction rate, with many clades gradually evolving into new forms.[37]

Astronomy and astrophysics 10 to 1,000 million[note 2] Cupid and Belinda, moons of Uranus, will likely have collided.[30]
Geology and planetary science 25 million According to Christopher R. Scotese, the movement of the San Andreas Fault will cause the Gulf of California to flood into the Central Valley. This will form a new inland sea on the West Coast of North America.[38]
Astronomy and astrophysics 50 million Maximum estimated time before the moon Phobos collides with Mars.[39]
Geology and planetary science 50 million According to Christopher R. Scotese, the movement of the San Andreas Fault will cause the current locations of Los Angeles and San Francisco to merge.[38] The Californian coast will begin to be subducted into the Aleutian Trench.[40]

Africa's collision with Eurasia closes the Mediterranean Basin and creates a mountain range similar to the Himalayas.[41]

The Appalachian Mountains peaks will largely erode away,[42] weathering at 5.7 Bubnoff units, although topography will actually rise as regional valleys deepen at twice this rate.[43]

Geology and planetary science 50–60 million The Canadian Rockies will erode away to a plain, assuming a rate of 60 Bubnoff units.[44] (The Southern Rockies in the United States are eroding at a somewhat slower rate.[45])
Geology and planetary science 50–400 million Estimated time for Earth to naturally replenish its fossil fuel reserves.[46]
Geology and planetary science 80 million The Big Island will have become the last of the current Hawaiian Islands to sink beneath the surface of the ocean, while a more recently formed chain of "new Hawaiian Islands" will then have emerged in their place.[47]
Astronomy and astrophysics 100 million[note 2] Earth will likely have been hit by an asteroid comparable in size to the one that triggered the K–Pg extinction 66 million years ago, assuming it cannot be averted.[48]
Geology and planetary science 100 million According to the Pangaea Proxima Model created by Christopher R. Scotese, a new subduction zone will open in the Atlantic Ocean and the Americas will begin to converge back toward Africa.[38]
Geology and planetary science 100 million Upper estimate for lifespan of the rings of Saturn in their current state.[49]
Astronomy and astrophysics 180 million Due to the gradual slowing down of Earth's rotation, a day on Earth will be one hour longer than it is today.[50]
Mathematics 230 million Prediction of the orbits of the planets is impossible over greater time spans than this, due to the limitations of Lyapunov time.[51]
Astronomy and astrophysics 240 million From its present position, the Solar System completes one full orbit of the Galactic center.[52]
Geology and planetary science 250 million Due to the northward movement of the West Coast of North America, the coast of California will collide with Alaska.[38]
Geology and planetary science 250 million All the continents on Earth may fuse into a supercontinent. Three potential arrangements of this configuration have been dubbed Amasia, Novopangaea, and Pangaea Ultima.[38][53]
Geology and planetary science 300–600 million Estimated time for Venus's mantle temperature to reach its maximum. Then, over a period of about 100 million years, major subduction occurs and the crust is recycled.[54]
Geology and planetary science 400–500 million[note 2] The supercontinent (Pangaea Ultima, Novopangaea, or Amasia) will likely have rifted apart.[53]
Astronomy and astrophysics 500 million[note 2] Estimated time until a gamma-ray burst, or massive, hyperenergetic supernova, occurs within 6,500 light-years of Earth; close enough for its rays to affect Earth's ozone layer and potentially trigger a mass extinction, assuming the hypothesis is correct that a previous such explosion triggered the Ordovician–Silurian extinction event. However, the supernova would have to be precisely oriented relative to Earth to have any negative effect.[55]
Astronomy and astrophysics 600 million Tidal acceleration moves the Moon far enough from Earth that total solar eclipses are no longer possible.[56]
Geology and planetary science 600 million The Sun's increasing luminosity begins to disrupt the carbonate–silicate cycle; higher luminosity increases weathering of surface rocks, which traps carbon dioxide in the ground as carbonate. As water evaporates from the Earth's surface, rocks harden, causing plate tectonics to slow and eventually stop. Without volcanoes to recycle carbon into the Earth's atmosphere, carbon dioxide levels begin to fall.[57] By this time, carbon dioxide levels will fall to the point at which C3 photosynthesis is no longer possible. All plants that utilize C3 photosynthesis (~99 percent of present-day species) will die.[58]
Biology 600-700 million[note 2] As temperatures continue to rise, plants could survive longer by evolving new ways that require less photosynthetic processes, like becoming carnivorous, adapting to desiccation, or associating with fungi. These adaptations are likely to occur just before the moist greenhouse effect.[59]
Biology 700–800 million[note 2] The death of most plant life will result in less oxygen in the atmosphere, allowing for more DNA damaging Ultraviolet Radiation to reach the surface. The rising temperatures will increase chemical reactions in the atmosphere, further lowering oxygen levels. As a result, vast migrations of species could occur. Flying animals would be better off because of their ability to travel large distances looking for cooler temperatures.Template:Sfn Many animals may be driven to the poles or possibly underground. These creatures would become active during the polar night and hibernate during the polar day due to the intense heat and radiation. Much of the land would become a barren desert and plants + animals would primarily be found in the oceans.Template:Sfn
Biology 800 million Carbon dioxide levels fall to the point at which C4 photosynthesis is no longer possible.[58] Without plant life to recycle oxygen in the atmosphere, free oxygen and the ozone layer will disappear from the atmosphere allowing for intense levels of deadly UV light to reach the surface. However, in their book The Life and Death of Planet Earth, authors Peter D. Ward and Donald Brownlee stated that some animal life may be able to survive in the oceans. Eventually, however, all multicellular life will die out.[60] The only life left on the Earth after this will be single celled bacteria.
Geology and planetary science 1 billion[note 3] 27% of the ocean's mass will have been subducted into the mantle. If this were to continue uninterrupted, it would reach an equilibrium where 65% of the surface water would remain at the surface.[61]
Geology and planetary science 1.1 billion The Sun's luminosity has risen by 10%, causing Earth's surface temperatures to reach an average of c. Template:Cvt. The atmosphere will become a "moist greenhouse", resulting in a runaway evaporation of the oceans. [57][62] Pockets of water may still be present at the poles, allowing abodes for simple life.[63][64]
Biology 1.3 billion Eukaryotic life dies out on Earth due to carbon dioxide starvation. Only prokaryotes remain.[60]
Astronomy and astrophysics 1.5–1.6 billion The Sun's rising luminosity causes its circumstellar habitable zone to move outwards; as carbon dioxide rises in Mars's atmosphere, its surface temperature rises to levels akin to Earth during the ice age.[60][65]
Biology 1.6 billion Lower estimate till all prokaryotic life will go extinct.[60]
Geology and planetary science 2.3 billion The Earth's outer core freezes, if the inner core continues to grow at its current rate of 1 mm per year.[66][67] Without its liquid outer core, the Earth's magnetic field shuts down,[68] and charged particles emanating from the Sun gradually deplete the atmosphere.[69]
Geology and planetary science 2.8 billion Earth's surface temperature, even at the poles, reaches an average of c. Template:Convert. At this point, all life, now reduced to unicellular colonies in isolated, scattered microenvironments such as high-altitude lakes or subsurface caves, will go extinct.[57][70]
Astronomy and astrophysics c. 3 billion[note 2] There is a roughly 1 in 100,000 chance that the Earth might be ejected into interstellar space by a stellar encounter before this point, and a 1 in 3 million chance that it will then be captured by another star. Were this to happen, life, assuming it survived the interstellar journey, could potentially continue for far longer.Template:Sfn
Astronomy and astrophysics 3 billion Median point at which the Moon's rising distance from the Earth lessens its stabilising effect on the Earth's axial tilt. As a consequence, Earth's true polar wander becomes chaotic and extreme, leading to dramatic shifts in the planet's climate due to the changing axial tilt.[71]
Astronomy and astrophysics 3.3 billion 1% chance that Jupiter's gravity may make Mercury's orbit so eccentric as to collide with Venus, sending the inner Solar System into chaos. Possible scenarios include Mercury colliding with the Sun, being ejected from the Solar System, or colliding with Earth.[72]
Geology and planetary science 3.5–4.5 billion All water currently present in oceans (if not lost earlier) evaporates. The greenhouse effect caused by the massive water atmosphere combined with the luminosity of the Sun reaching roughly 35–40% more than its present-day value, will result in Earth's surface heating up with the temperature rising to Template:Convert in extreme case, which is hot enough to melt some surface rock.[73][74]Template:Sfn[75] This period in Earth's future is often compared to Venus today, but the temperature is actually around two times the temperature on Venus today, and at this temperature the surface will be partially molten,[76] while Venus probably has a mostly solid surface at present. Venus will also probably drastically heat up at this time as well, most likely being much hotter than Earth will be as it is closer to the Sun.
Astronomy and astrophysics 3.6 billion Neptune's moon Triton falls through the planet's Roche limit, potentially disintegrating into a planetary ring system similar to Saturn's.[77]
Astronomy and astrophysics 4 billion Median point by which the Andromeda Galaxy will have collided with the Milky Way, which will thereafter merge to form a galaxy dubbed "Milkomeda".[78] The planets of the Solar System are expected to be relatively unaffected by this collision.[79][80][81]
Astronomy and astrophysics 5.4 billion With the hydrogen supply exhausted at its core, the Sun leaves the main sequence and begins to evolve into a red giant.[82]
Astronomy and astrophysics 7.5 billion Earth and Mars may become tidally locked with the expanding subgiant Sun.[65]
Astronomy and astrophysics 7.59 billion The Earth and Moon are very likely destroyed by falling into the Sun, just before the Sun reaches the tip of its red giant phase and its maximum radius of 256 times the present-day value.[82][note 4] Before the final collision, the Moon possibly spirals below Earth's Roche limit, breaking into a ring of debris, most of which falls to the Earth's surface.[83] During this time, most of the Earth's atmosphere will be lost to space and it's surface will consist of a lava ocean with floating continents of metals and metal oxides as well as icebergs of refractory materials, with an average temperature of over Template:Convert.[84]

During this era, Saturn's moon Titan may reach surface temperatures necessary to support life.[85]

Astronomy and astrophysics 7.9 billion The Sun reaches the tip of the red-giant branch of the Hertzsprung–Russell diagram, achieving its maximum radius of 256 times the present-day value.[86] In the process, Mercury, Venus, very likely Earth, and possibly Mars are destroyed.[82]
Astronomy and astrophysics 8 billion The Sun becomes a carbon-oxygen white dwarf with about 54.05% its present mass.[82][87][88][89] At this point, if somehow the Earth survives, temperatures on the surface of the planet, as well as other remaining planets in the Solar System, will begin dropping rapidly, due to the white dwarf Sun emitting much less energy than it does today.
Astronomy and astrophysics 22 billion The end of the Universe in the Big Rip scenario, assuming a model of dark energy with [[Equation of state (cosmology)|Template:Var = −1.5]].[90] If the density of dark energy is less than -1, then the Universe's expansion would continue to accelerate and the Observable Universe would continue to get smaller. Around 200 million years before the rip, galaxy clusters like the Local Group or the Sculptor Group would be destroyed. 60 million years before the rip, all galaxies will begin to lose stars around their edges and will completely disintegrate in another 40 million years. Three months before the end, all star systems will become gravitationally unbound, and planets will fly off into the rapidly expanding universe. 30 minutes before the end, planets, stars, asteroids and even extreme objects like neutron stars and black holes will evaporate into atoms. 10−19 seconds before the end, atoms would break apart and right at the moment of the rip even space time itself would disintegrate. The universe would enter into a "rip singularity" when all distances become infinitely large. Where as a "crunch singularity" all matter is infinitely concentrated, in a "rip singularity" all matter is infinitely spread out.[91] However, Observations of galaxy cluster speeds by the Chandra X-ray Observatory suggest that the true value of Template:Var is c. −0.991, meaning the Big Rip will not occur.[92]
Astronomy and astrophysics 50 billion If the Earth and Moon are not engulfed by the Sun, by this time they will become tidelocked, with each showing only one face to the other.[93][94] Thereafter, the tidal action of the white dwarf Sun will extract angular momentum from the system, causing the lunar orbit to decay and the Earth's spin to accelerate.[95]
Astronomy and astrophysics 65 billion The Moon may end up colliding with the Earth due to the decay of its orbit, assuming the Earth and Moon are not engulfed by the red giant Sun.[96]
Astronomy and astrophysics 100-150 billion The Universe's expansion causes all galaxies beyond the former Milky Way's Local Group to disappear beyond the cosmic light horizon, removing them from the observable universe.[97]
Astronomy and astrophysics 150 billion The cosmic microwave background cools from its current temperature of c. 2.7 K to 0.3 K, rendering it essentially undetectable with current technology.[98]
Astronomy and astrophysics 450 billion Median point by which the c. 47 galaxies[99] of the Local Group will coalesce into a single large galaxy.[4]
Astronomy and astrophysics 800 billion Expected time when the net light emission from the combined "Milkomeda" galaxy begins to decline as the red dwarf stars pass through their blue dwarf stage of peak luminosity.[100]
Astronomy and astrophysics 1012 (1 trillion) Low estimate for the time until star formation ends in galaxies as galaxies are depleted of the gas clouds they need to form stars.[4]

The universe's expansion, assuming a constant dark energy density, multiplies the wavelength of the cosmic microwave background by 1029, exceeding the scale of the cosmic light horizon and rendering its evidence of the Big Bang undetectable. However, it may still be possible to determine the expansion of the universe through the study of hypervelocity stars.[97]

Astronomy and astrophysics 1012 (1 trillion)[note 2] Estimated time the end of the Universe via the Big Crunch, assuming a "closed" model. Depending on how long the expansion phase is, the events in the contraction phase will happen in the reverse order.[101] Galaxy superclusters would first merge, followed by galaxy clusters and then later galaxies. About 100,000 years before the Big Crunch, stars have become so close together that they will begin to collide with each other. Also, the cosmic microwave background temperature will rise to about Template:Convert, which means that stars will no longer be able to expel their internal heat, slowly cooking themselves until they explode. Minutes before the Big Crunch, the temperature will be so great that atomic nuclei will disband and the partials will be sucked up by already coalescing black holes. Finally, all the black holes in the universe will merge into one singular black hole containing all the matter in the universe, which it would then devour the universe, including itself.[101] After this, it is possible that a new Big Bang would follow and create a new universe. The observed actions of dark energy do not support this scenario; however, the properties of dark energy are still not known, it is possible that dark energy could reverse sometime in the future.[102]
Astronomy and astrophysics 4×1012 (4 trillion) Estimated time until the red dwarf star Proxima Centauri, the closest star to the Sun at a distance of 4.25 light-years, leaves the main sequence and becomes a white dwarf.[103]
Astronomy and astrophysics 1.2×1013 (12 trillion) Estimated time until the red dwarf VB 10, as of 2016 the least massive main sequence star with an estimated mass of 0.075 Template:Solar mass, runs out of hydrogen in its core and becomes a white dwarf.[104][105]
Astronomy and astrophysics 3×1013 (30 trillion) Estimated time for stars (including the Sun) to undergo a close encounter with another star in local stellar neighborhoods. Whenever two stars (or stellar remnants) pass close to each other, their planets' orbits can be disrupted, potentially ejecting them from the system entirely. On average, the closer a planet's orbit to its parent star the longer it takes to be ejected in this manner, because it is gravitationally more tightly bound to the star.[106]
Astronomy and astrophysics 1014 (100 trillion) High estimate for the time until normal star formation ends in galaxies.[4] This marks the transition from the Stelliferous Era to the Degenerate Era; with no free hydrogen to form new stars, all remaining stars slowly exhaust their fuel and die.[3]
Astronomy and astrophysics 1.1–1.2×1014 (110–120 trillion) Time by which all stars in the universe will have exhausted their fuel (the longest-lived stars, low-mass red dwarfs, have lifespans of roughly 10–20 trillion years).[4] After this point, the stellar-mass objects remaining are stellar remnants (white dwarfs, neutron stars, black holes) and brown dwarfs.

Collisions between brown dwarfs will create new red dwarfs on a marginal level: on average, about 100 stars will be shining in what was once the Milky Way. Collisions between stellar remnants will create occasional supernovae.[4]

Astronomy and astrophysics 1015 (1 quadrillion) Estimated time until stellar close encounters detach all planets in star systems (including the Solar System) from their orbits.[4]

By this point, the Sun will have cooled to five degrees above absolute zero.[107]

Astronomy and astrophysics 1019 to 1020
(10–100 quintillion)
Estimated time until 90%–99% of brown dwarfs and stellar remnants (including the Sun) are ejected from galaxies. When two objects pass close enough to each other, they exchange orbital energy, with lower-mass objects tending to gain energy. Through repeated encounters, the lower-mass objects can gain enough energy in this manner to be ejected from their galaxy. This process eventually causes the Milky Way to eject the majority of its brown dwarfs and stellar remnants.[4][108]
Astronomy and astrophysics 1020 (100 quintillion) Estimated time until the Earth collides with the black dwarf Sun due to the decay of its orbit via emission of gravitational radiation,[109] if the Earth is not ejected from its orbit by a stellar encounter or engulfed by the Sun during its red giant phase.[109]
Astronomy and astrophysics 1030 (1 nonillion) Estimated time until those stars not ejected from galaxies (1%–10%) fall into their galaxies' central supermassive black holes. By this point, with binary stars having fallen into each other, and planets into their stars, via emission of gravitational radiation, only solitary objects (stellar remnants, brown dwarfs, ejected planets, black holes) will remain in the universe.[4]
Particle physics 2×1036 The estimated time for all nucleons in the observable universe to decay, if the hypothesized proton half-life takes its smallest possible value (8.2×1033 years).[110][111][note 5]
Particle physics 3×1043 Estimated time for all nucleons in the observable universe to decay, if the hypothesized proton half-life takes the largest possible value, 1041 years,[4] assuming that the Big Bang was inflationary and that the same process that made baryons predominate over anti-baryons in the early Universe makes protons decay.[111][note 5] By this time, if protons do decay, the Black Hole Era, in which black holes are the only remaining celestial objects, begins.[3][4]
Particle physics 1065 Assuming that protons do not decay, estimated time for rigid objects, from free-floating rocks in space to planets, to rearrange their atoms and molecules via quantum tunneling. On this timescale, any discrete body of matter "behaves like a liquid" and becomes a smooth sphere due to diffusion and gravity.[109]
Particle physics 5.8×1068 Estimated time until a stellar mass black hole with a mass of 3 solar masses decays into subatomic particles by the Hawking process.[112]
Particle physics 6.036×1099 Estimated time until the supermassive black hole of TON 618, as of 2018 the most massive known with the mass of 66 billion solar masses, dissipates by the emission of Hawking radiation,[112] assuming zero angular momentum (non-rotating black hole).
Particle physics 1.7×10106 Estimated time until a supermassive black hole with a mass of 20 trillion solar masses decays by the Hawking process.[112] This marks the end of the Black Hole Era. Beyond this time, if protons do decay, the Universe enters the Dark Era, in which all physical objects have decayed to subatomic particles, gradually winding down to their final energy state in the heat death of the universe.[3][4]
Particle physics 10139 2018 estimate of Standard Model lifetime before collapse of a false vacuum; 95% confidence interval is 1058 to 10241 years due in part to uncertainty about the top quark mass.[113]
Particle physics 10200 Estimated high time for all nucleons in the observable universe to decay, if they do not via the above process, through any one of many different mechanisms allowed in modern particle physics (higher-order baryon non-conservation processes, virtual black holes, sphalerons, etc.) on time scales of 1046 to 10200 years.[3]
Particle physics 101500 Assuming protons do not decay, the estimated time until all baryonic matter has either fused together to form iron-56 or decayed from a higher mass element into iron-56 (see iron star).[109]
Particle physics [note 6][note 7] Low estimate for the time until all objects exceeding the Planck massTemplate:Failed verification collapse via quantum tunnelling into black holes, assuming no proton decay or virtual black holes.[109] On this vast timescale, even ultra-stable iron stars are destroyed by quantum tunnelling events. First iron stars of sufficient mass will collapse via tunnelling into neutron stars. Subsequently, neutron stars and any remaining iron stars collapse via tunnelling into black holes. The subsequent evaporation of each resulting black hole into sub-atomic particles (a process lasting roughly 10100 years) is on these timescales instantaneous.
Particle physics [note 2][note 7] Estimated time for a Boltzmann brain to appear in the vacuum via a spontaneous entropy decrease.[6]
Particle physics [note 7] High estimate for the time until all matter collapses into neutron stars or black holes, assuming no proton decay or virtual black holes,[109] which then (on these timescales) instantaneously evaporate into sub-atomic particles.
Particle physics [note 7] High estimate for the time for the universe to reach its final energy state, even in the presence of a false vacuum.[6]Template:Failed verification
Particle physics [note 2][note 7] Around this vast timeframe, quantum tunnelling in any isolated patch of the vacuum could generate, via inflation, new Big Bangs giving birth to new universes.[114]

Because the total number of ways in which all the subatomic particles in the observable universe can be combined is ,[115][116] a number which, when multiplied by , disappears into the rounding error, this is also the time required for a quantum-tunnelled and quantum fluctuation-generated Big Bang to produce a new universe identical to our own, assuming that every new universe contained at least the same number of subatomic particles and obeyed laws of physics within the range predicted by string theory.[117]

ꯃꯤꯑꯣꯏꯕꯗ ꯑꯣꯏꯔꯛꯀꯗꯕ[edit | edit source]

Key.svg Years from now Event
technology and culture 10,000 Most probable estimated lifespan of technological civilization, according to Frank Drake's original formulation of the Drake equation.[118]
Biology 10,000 If globalization trends lead to panmixia, human genetic variation will no longer be regionalized, as the effective population size will equal the actual population size.[119] This does not mean homogeneity, as minority traits will still be preserved, e.g. the blonde gene will not disappear, but it will be rather evenly distributed worldwide.
Mathematics 10,000 Humanity has a 95% probability of being extinct by this date, according to Brandon Carter's formulation of the controversial Doomsday argument, which argues that half of the humans who will ever have lived have probably already been born.[120]
technology and culture 20,000 According to the glottochronology linguistic model of Morris Swadesh, future languages should retain just 1 out of 100 "core vocabulary" words on their Swadesh list compared to that of their current progenitors.[121]
Geology and planetary science 100,000+ Time required to terraform Mars with an oxygen-rich breathable atmosphere, using only plants with solar efficiency comparable to the biosphere currently found on Earth.[122]
Technology and culture 1 million Estimated shortest time by which humanity could colonize our Milky Way galaxy and become capable of harnessing all the energy of the galaxy, assuming a velocity of 10% the speed of light.[123]
Biology 2 million Vertebrate species separated for this long will generally undergo allopatric speciation.[124] Evolutionary biologist James W. Valentine predicted that if humanity has been dispersed among genetically isolated space colonies over this time, the galaxy will host an evolutionary radiation of multiple human species with a "diversity of form and adaptation that would astound us".[125] This would be a natural process of isolated populations, unrelated to potential deliberate genetic enhancement technologies.
Mathematics 7.8 million Humanity has a 95% probability of being extinct by this date, according to J. Richard Gott's formulation of the controversial Doomsday argument, which argues that we have probably already lived through half the duration of human history.[126]
technology and culture 100 million Maximal estimated lifespan of technological civilization, according to Frank Drake's original formulation of the Drake equation.[127]
Astronomy and astrophysics 1 billion Estimated time for an astroengineering project to alter the Earth's orbit, compensating for the Sun's rising brightness and outward migration of the habitable zone, accomplished by repeated asteroid gravity assists.[128][129]

ꯅꯣꯡꯊꯧ ꯊꯤꯖꯤꯟꯕ ꯑꯃꯁꯨꯡ ꯅꯣꯡꯊꯧꯒꯤ ꯍꯤꯖꯥꯎ[edit | edit source]

To date five spacecraft (Voyager 1, Voyager 2, Pioneer 10, Pioneer 11 and New Horizons) are on trajectories which will take them out of the Solar System and into interstellar space. Barring an extremely unlikely collision with some object, the craft should persist indefinitely.[130]

Key.svg Years from now Event
Astronomy and astrophysics 10,000 Pioneer 10 passes within 3.8 light-years of Barnard's Star.[131]
Astronomy and astrophysics 25,000 The Arecibo message, a collection of radio data transmitted on 16 November 1974, reaches the distance of its destination, the globular cluster Messier 13.[132] This is the only interstellar radio message sent to such a distant region of the galaxy. There will be a 24-light-year shift in the cluster's position in the galaxy during the time it takes the message to reach it, but as the cluster is 168 light-years in diameter, the message will still reach its destination.[133] Any reply will take at least another 25,000 years from the time of its transmission.
Astronomy and astrophysics 32,000 Pioneer 10 passes within 3 light-years of Ross 248.[134][135]
Astronomy and astrophysics 40,000 Voyager 1 passes within 1.6 light-years of AC+79 3888, a star in the constellation Camelopardalis also known as Gliese 445.[136]
Astronomy and astrophysics 50,000 The KEO space time capsule, if it is launched, will reenter Earth's atmosphere.[137]
Astronomy and astrophysics 296,000 Voyager 2 passes within 4.3 light-years of Sirius, the brightest star in the night sky.[136]
Astronomy and astrophysics 800,000–8 million Low estimate of Pioneer 10 plaque lifespan, before the etching is destroyed by poorly-understood interstellar erosion processes.[138]
Astronomy and astrophysics 2 million Pioneer 10 passes near the bright star Aldebaran.[139]
Astronomy and astrophysics 4 million Pioneer 11 passes near one of the stars in the constellation Aquila.[139]
Astronomy and astrophysics 8 million The LAGEOS satellites' orbits will decay, and they will re-enter Earth's atmosphere, carrying with them a message to any far future descendants of humanity, and a map of the continents as they are expected to appear then.[140]
Astronomy and astrophysics 1 billion Estimated lifespan of the two Voyager Golden Records, before the information stored on them is rendered unrecoverable.[141]

ꯁꯤꯟ-ꯁꯥꯕꯒꯤ ꯊꯧꯔꯥꯡꯁꯤꯡ[edit | edit source]

Key.svg Years from now Event
technology and culture 10,000 Planned lifespan of the Long Now Foundation's several ongoing projects, including a 10,000-year clock known as the Clock of the Long Now, the Rosetta Project, and the Long Bet Project.[142]

Estimated lifespan of the HD-Rosetta analog disc, an ion beam-etched writing medium on nickel plate, a technology developed at Los Alamos National Laboratory and later commercialized. (The Rosetta Project uses this technology, named after the Rosetta Stone).

Biology 10,000 Projected lifespan of Norway's Svalbard Global Seed Vault.[143]
technology and culture 100,000+ Estimated lifespan of Memory of Mankind (MOM) self storage-style repository in Hallstatt salt mine in Austria, which stores information on inscribed tablets of stoneware.[144]
technology and culture 1 million Planned lifespan of the Human Document Project being developed at the University of Twente in the Netherlands.[145]
technology and culture 1 billion Estimated lifespan of "Nanoshuttle memory device" using an iron nanoparticle moved as a molecular switch through a carbon nanotube, a technology developed at the University of California at Berkeley.[146]
technology and culture more than 13 billion Estimated lifespan of "Superman memory crystal" data storage using femtosecond laser-etched nanostructures in glass, a technology developed at the University of Southampton.[147][148]

ꯃꯤꯑꯣꯏꯕꯅ ꯁꯦꯝꯒꯠꯄꯁꯤꯡ[edit | edit source]

Key.svg Years from now Event
Geology and planetary science 50,000 Estimated atmospheric lifetime of tetrafluoromethane, the most durable greenhouse gas.[149]
Geology and planetary science 1 million Current glass objects in the environment will be decomposed.[150]

Various public monuments composed of hard granite will have eroded one meter, in a moderate climate, assuming a rate of 1 Bubnoff unit (1 mm / 1,000 years, or ~1 inch / 10,000 years).[151]

Without maintenance, the Great Pyramid of Giza will erode into unrecognizability.[152]

On the Moon, Neil Armstrong's "one small step" footprint at Tranquility Base will erode by this time, along with those left by all twelve Apollo moonwalkers, due to the accumulated effects of space weathering.[153][154] (Normal erosion processes active on Earth are not present due to the Moon's almost complete lack of atmosphere.)

Geology and planetary science 7.2 million Without maintenance, Mount Rushmore will erode into unrecognizability.[155]
Geology and planetary science 100 million Future archaeologists should be able to identify an "Urban Stratum" of fossilized great coastal cities, mostly through the remains of underground infrastructure such as building foundations and utility tunnels.[156]

ꯁꯟꯊꯣꯡꯂꯣꯟ(ꯂꯥꯡꯄꯨꯡꯂꯣꯟ)ꯀꯤ ꯊꯩꯑꯣꯡꯁꯤꯡ[edit | edit source]

Extremely rare astronomical events beginning in the 11th millennium AD (year 10,001) will be:

Date / Years from now Event
Astronomy and astrophysics 20 August, AD 10,663 A simultaneous total solar eclipse and transit of Mercury.[157]
Astronomy and astrophysics 25 August, AD 11,268 A simultaneous total solar eclipse and transit of Mercury.[157]
Astronomy and astrophysics 28 February, AD 11,575 A simultaneous annular solar eclipse and transit of Mercury.[157]
Astronomy and astrophysics 17 September, AD 13,425 A near-simultaneous transit of Venus and Mercury.[157]
Astronomy and astrophysics AD 13,727 The Earth's axial precession will have made Vega the northern pole star.[158][159][160][161]
Astronomy and astrophysics 13,000 years By this point, halfway through the precessional cycle, Earth's axial tilt will be reversed, causing summer and winter to occur on opposite sides of Earth's orbit. This means that the seasons in the Northern Hemisphere, which experiences more pronounced seasonal variation due to a higher percentage of land, will be even more extreme, as it will be facing towards the Sun at Earth's perihelion and away from the Sun at aphelion.[159]
Astronomy and astrophysics 5 April, AD 15,232 A simultaneous total solar eclipse and transit of Venus.[157]
Astronomy and astrophysics 20 April, AD 15,790 A simultaneous annular solar eclipse and transit of Mercury.[157]
Astronomy and astrophysics 14,000–17,000 years The Earth's axial precession will make Canopus the South Star, but it will only be within 10° of the south celestial pole.[162]
Astronomy and astrophysics AD 20,346 Thuban will be the northern pole star.[163]
Astronomy and astrophysics AD 27,800 Polaris will again be the northern pole star.[164]
Astronomy and astrophysics 27,000 years The eccentricity of Earth's orbit will reach a minimum, 0.00236 (it is now 0.01671).[165][166]
Astronomy and astrophysics October, AD 38,172 A transit of Uranus from Neptune, the rarest of all planetary transits.[167]
Astronomy and astrophysics 26 July, AD 69,163 A simultaneous transit of Venus and Mercury.[157]
Astronomy and astrophysics AD 70,000 Comet Hyakutake returns to the inner Solar System, after traveling in its orbit out to its aphelion 3,410 A.U. from the Sun and back.[168]
Astronomy and astrophysics 27 and 28 March, AD 224,508 Respectively, Venus and then Mercury will transit the Sun.[157]
Astronomy and astrophysics AD 571,741 A simultaneous transit of Venus and the Earth as seen from Mars[157]
Astronomy and astrophysics 6 million Comet C/1999 F1 (Catalina), one of the longest-period comets known, returns to the inner Solar System, after traveling in its orbit out to its aphelion 66,600 A.U. (1.05 light-years) from the Sun and back.[169]

ꯆꯩꯆꯠꯂꯣꯟ(ꯊꯄꯥꯂꯣꯟ)ꯀꯤ predictions[edit | edit source]

Key.svg Years from now Event
Astronomy and astrophysics 10,000
The Gregorian calendar will be roughly 10 days out of sync with the seasons.[170]
Astronomy and astrophysics Expression error: Unrecognized punctuation character "꯲". 10 June, AD 12,892 In the Hebrew calendar, due to a gradual drift with regard to the solar year, Passover will fall on the northern summer solstice (it is meant to fall around the spring equinox).[171]
Astronomy and astrophysics Expression error: Unrecognized punctuation character "꯲". AD 20,874 The lunar Islamic calendar and the solar Gregorian calendar will share the same year number. After this, the shorter Islamic calendar will slowly overtake the Gregorian.[172]
Astronomy and astrophysics 25,000
The Tabular Islamic calendar will be roughly 10 days out of sync with the Moon's phase.[173]
Astronomy and astrophysics Expression error: Unrecognized punctuation character "꯲". 1 March, AD 48,901[note 8] The Julian day number (a measure used by astronomers) at Greenwich mean midnight (start of day) is 19 581 842.5 for both dates. The Julian calendar (365.25 days) and Gregorian calendar (365.2425 days) will be one year apart.[174]

Nuclear power[edit | edit source]

Key.svg Years from now Event
Particle physics 10,000 The Waste Isolation Pilot Plant, for nuclear weapons waste, is planned to be protected until this time, with a "Permanent Marker" system designed to warn off visitors through both multiple languages (the six UN languages and Navajo) and through pictograms.[175] (The Human Interference Task Force has provided the theoretical basis for United States plans for future nuclear semiotics.)
Particle physics 20,000 The Chernobyl Exclusion Zone, the Template:Convert area of Ukraine and Belarus left deserted by the 1986 Chernobyl disaster, becomes safe for human life.[176]
Geology and planetary science 30,000 Estimated supply lifespan of fission-based breeder reactor reserves, using known sources, assuming 2009 world energy consumption.[177]
Geology and planetary science 60,000 Estimated supply lifespan of fission-based light-water reactor reserves if it is possible to extract all the uranium from seawater, assuming 2009 world energy consumption.[177]
Particle physics 211,000 Half-life of technetium-99, the most important long-lived fission product in uranium-derived nuclear waste.
Particle physics 250,000 The estimated minimum time at which the spent plutonium stored at New Mexico's Waste Isolation Pilot Plant will cease to be lethal to humans.[178]
Particle physics 15.7 million Half-life of iodine-129, the most durable long-lived fission product in uranium-derived nuclear waste.
Geology and planetary science 60 million Estimated supply lifespan of fusion power reserves if it is possible to extract all the lithium from seawater, assuming 1995 world energy consumption.[179]
Geology and planetary science 5 billion Estimated supply lifespan of fission-based breeder reactor reserves if it is possible to extract all the uranium from seawater, assuming 1983 world energy consumption.[180]
Geology and planetary science 150 billion Estimated supply lifespan of fusion power reserves if it is possible to extract all the deuterium from seawater, assuming 1995 world energy consumption.[179]

Graphical timelines[edit | edit source]

For graphical, logarithmic timelines of these events see:

ꯁꯤꯖꯨ ꯌꯦꯡꯉꯨ[edit | edit source]

Template:Wp/mni/div col end

Notes[edit | edit source]

  1. The precise cutoff point is 0:00 on 1 January AD 10,001
  2. 2.00 2.01 2.02 2.03 2.04 2.05 2.06 2.07 2.08 2.09 2.10 2.11 2.12 2.13 2.14 2.15 2.16 2.17 This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.
  3. Units are short scale
  4. This has been a tricky question for quite a while; see the 2001 paper by Rybicki, K. R. and Denis, C. However, according to the latest calculations, this happens with a very high degree of certainty.
  5. 5.0 5.1 Around 264 half-lives. Tyson et al. employ the computation with a different value for half-life.
  6. is 1 followed by 1026 (100 septillion) zeroes
  7. 7.0 7.1 7.2 7.3 7.4 Although listed in years for convenience, the numbers beyond this point are so vast that their digits would remain unchanged regardless of which conventional units they were listed in, be they nanoseconds or star lifespans.
  8. Manually calculated from the fact that the calendars were 10 days apart in 1582 and grew further apart by 3 days every 400 years. 1 March AD 48900 (Julian) and 1 March AD 48901 (Gregorian) are both Tuesday.

ꯂꯧꯔꯛꯐꯝꯁꯤꯡ[edit | edit source]

  1. Template:Cite book
  2. Nave, C.R.. Second Law of Thermodynamics. Georgia State University. Retrieved on 3 December 2011
  3. 3.0 3.1 3.2 3.3 3.4 (1999) The Five Ages of the Universe. New York: The Free Press. ISBN 978-0684854229. 
  4. 4.00 4.01 4.02 4.03 4.04 4.05 4.06 4.07 4.08 4.09 4.10 4.11 Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337.
  5. Komatsu, E.; Smith, K. M.; Dunkley, J.; et al. (2011). "Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Cosmological Interpretation". The Astrophysical Journal Supplement Series. 192 (2): 18. arXiv:1001.4731. Bibcode:2011ApJS..192...19W. doi:10.1088/0067-0049/192/2/18.
  6. 6.0 6.1 6.2 Linde, Andrei. (2007). "Sinks in the Landscape, Boltzmann Brains and the Cosmological Constant Problem". Journal of Cosmology and Astroparticle Physics. 2007 (1): 022. arXiv:hep-th/0611043. Bibcode:2007JCAP...01..022L. CiteSeerX doi:10.1088/1475-7516/2007/01/022.
  7. Template:Cite journal
  8. Template:Cite journal
  9. Template:Cite web
  10. Template:Cite web
  11. Template:Cite journal
  12. Template:Cite book
  13. 13.0 13.1 Matthews, R. A. J. (Spring 1994). "The Close Approach of Stars in the Solar Neighborhood". Quarterly Journal of the Royal Astronomical Society. 35 (1): 1. Bibcode:1994QJRAS..35....1M.
  14. Berger, A & Loutre, MF (2002). "Climate: an exceptionally long interglacial ahead?". Science. 297 (5585): 1287–1288. doi:10.1126/science.1076120. PMID 12193773.
  15. Niagara Falls Geology Facts & Figures. Niagara Parks. Archived from the original on 19 July 2011 ꯫ Retrieved on 29 April 2011
  16. Template:Cite bookTemplate:ISBN missing
  17. Finkleman, David; Allen, Steve; Seago, John; Seaman, Rob; Seidelmann, P. Kenneth (June 2011). "The Future of Time: UTC and the Leap Second". American Scientist, July–August , V N4 P312. 2011 (99). arXiv:1106.3141.
  18. Tapping, Ken (2005). The Unfixed Stars. National Research Council Canada. Archived from the original on 8 July 2011 ꯫ Retrieved on 29 December 2010
  19. Monnier, J. D.; Tuthill, P.; Lopez, GB; et al. (1999). "The Last Gasps of VY Canis Majoris: Aperture Synthesis and Adaptive Optics Imagery". The Astrophysical Journal. 512 (1): 351–361. arXiv:astro-ph/9810024. Bibcode:1999ApJ...512..351M. doi:10.1086/306761.
  20. 20.0 20.1 Super-eruptions: Global effects and future threats. The Geological Society. Retrieved on 25 May 2012
  21. Template:Cite bookTemplate:ISBN missing
  22. Template:Cite book
  23. Frequently Asked Questions. Hawai'i Volcanoes National Park (2011). Retrieved on 22 October 2011
  24. Template:Cite journal
  25. Bostrom, Nick (March 2002). "Existential Risks: Analyzing Human Extinction Scenarios and Related Hazards". Journal of Evolution and Technology. 9 (1). Retrieved 10 September 2012.
  26. Template:Cite web
  27. Template:Cite bookTemplate:ISBN missing
  28. Sharpest Views of Betelgeuse Reveal How Supergiant Stars Lose Mass. European Southern Observatory (29 July 2009). Retrieved on 6 September 2010
  29. Sessions, Larry (29 July 2009). Betelgeuse will explode someday. EarthSky Communications, Inc. Retrieved on 16 November 2010
  30. 30.0 30.1 Template:Cite web
  31. Filip Berski and Piotr A. Dybczyński (25 October 2016). "Gliese 710 will pass the Sun even closer". Astronomy and Astrophysics. 595 (L10): L10. Bibcode:2016A&A...595L..10B. doi:10.1051/0004-6361/201629835.
  32. Template:Cite bookTemplate:ISBN missing
  33. Template:Cite web
  34. Template:Cite journal
  35. Haddok, Eitan (29 September 2008). Birth of an Ocean: The Evolution of Ethiopia's Afar Depression. Scientific American. Retrieved on 27 December 2010
  36. Template:Cite journal
  37. Template:Cite bookTemplate:ISBN missing
  38. 38.0 38.1 38.2 38.3 38.4 Scotese, Christopher R.. Pangea Ultima will form 250 million years in the Future. Retrieved on 13 March 2006
  39. Bills, Bruce G.; Gregory A. Neumann; David E. Smith; Maria T. Zuber (2005). "Improved estimate of tidal dissipation within Mars from MOLA observations of the shadow of Phobos" (PDF). Journal of Geophysical Research. 110 (E07004): E07004. Bibcode:2005JGRE..110.7004B. doi:10.1029/2004je002376.
  40. Garrison, Tom (2009). Essentials of Oceanography, 5, Brooks/Cole, 62. Template:ISBN missing
  41. Continents in Collision: Pangea Ultima. NASA (2000). Retrieved on 29 December 2010
  42. Template:Cite encyclopedia
  43. Template:Cite journal
  44. Template:Cite bookTemplate:ISBN missing
  45. Template:Cite journal
  46. Template:Cite bookTemplate:ISBN missing
  47. Template:Cite news
  48. Nelson, Stephen A.. Meteorites, Impacts, and Mass Extinction. Tulane University. Retrieved on 13 January 2011
  49. Template:Cite bookTemplate:ISBN missing
  50. Template:Cite web
  51. Hayes, Wayne B. (2007). "Is the Outer Solar System Chaotic?". Nature Physics. 3 (10): 689–691. arXiv:astro-ph/0702179. Bibcode:2007NatPh...3..689H. CiteSeerX doi:10.1038/nphys728.
  52. Leong, Stacy (2002). Period of the Sun's Orbit Around the Galaxy (Cosmic Year). Retrieved on 2 April 2007
  53. 53.0 53.1 "Pangaea, the comeback"꯫ New Scientist꯫ 20 October 2007 ꯫ ꯆꯠꯅꯕ ꯆꯩꯆꯠ - 2 January 2014 ꯫ ꯫ ꯂꯤꯗꯨꯅ ꯊꯝꯂꯦ ꯑꯁꯦꯡꯕ ꯃꯐꯝꯗ 13 April 2008 ꯫ 
  54. Template:Cite journal
  55. Minard, Anne (2009). Gamma-Ray Burst Caused Mass Extinction?. National Geographic News. Retrieved on 2012-08-27
  56. Questions Frequently Asked by the Public About Eclipses. NASA. Archived from the original on 12 March 2010 ꯫ Retrieved on 7 March 2010
  57. 57.0 57.1 57.2 Template:Cite journal
  58. 58.0 58.1 Heath, Martin J.; Doyle, Laurance R. (2009). "Circumstellar Habitable Zones to Ecodynamic Domains: A Preliminary Review and Suggested Future Directions". arXiv:0912.2482 [astro-ph.EP].
  59. Cite error: Invalid <ref> tag; no text was provided for refs named mj2013
  60. 60.0 60.1 60.2 60.3 Franck, S.; Bounama, C.; Von Bloh, W. (November 2005). "Causes and timing of future biosphere extinction" (PDF). Biogeosciences Discussions. 2 (6): 1665–1679. Bibcode:2005BGD.....2.1665F. doi:10.5194/bgd-2-1665-2005. Retrieved 19 October 2011.
  61. Bounama, Christine; Franck, S.; Von Bloh, W. (2001). "The fate of Earth's ocean" (PDF). Hydrology and Earth System Sciences. 5 (4): 569–575. Bibcode:2001HESS....5..569B. doi:10.5194/hess-5-569-2001. Retrieved 3 July 2009.
  62. Schröder, K.-P.; Connon Smith, Robert (1 May 2008). "Distant future of the Sun and Earth revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x.
  63. (2010) "Planetary habitability on astronomical time scales", Heliophysics: Evolving Solar Activity and the Climates of Space and Earth. Cambridge University Press. ISBN 978-0521112949. 
  64. Li King-Fai; Pahlevan, Kaveh; Kirschvink, Joseph L.; Yung, Luk L. (2009). "Atmospheric pressure as a natural climate regulator for a terrestrial planet with a biosphere". Proceedings of the National Academy of Sciences of the United States of America. 106 (24): 9576–9579. Bibcode:2009PNAS..106.9576L. doi:10.1073/pnas.0809436106. PMC 2701016. PMID 19487662.
  65. 65.0 65.1 Kargel, Jeffrey Stuart (2004). Mars: A Warmer, Wetter Planet. Springer, 509. ISBN 978-1852335687. Retrieved on 29 October 2007. 
  66. Waszek, Lauren; Irving, Jessica; Deuss, Arwen (20 February 2011). "Reconciling the Hemispherical Structure of Earth's Inner Core With its Super-Rotation". Nature Geoscience. 4 (4): 264–267. Bibcode:2011NatGe...4..264W. doi:10.1038/ngeo1083.
  67. McDonough, W. F. (2004). Compositional Model for the Earth's Core 2, 547–568. doi:10.1016/B0-08-043751-6/02015-6. ISBN 978-0080437514. 
  68. Luhmann, J. G.; Johnson, R. E.; Zhang, M. H. G. (1992). "Evolutionary impact of sputtering of the Martian atmosphere by O+ pickup ions". Geophysical Research Letters. 19 (21): 2151–2154. Bibcode:1992GeoRL..19.2151L. doi:10.1029/92GL02485.
  69. Template:Cite journal
  70. Adams, Fred C. (2008). "Long-term astrophysicial processes", Global Catastrophic Risks. Oxford University Press, 33–47. Template:ISBN missing
  71. Neron de Surgey, O.; Laskar, J. (1996). "On the Long Term Evolution of the Spin of the Earth". Astronomy and Astrophysics. 318: 975. Bibcode:1997A&A...318..975N.
  72. "Study: Earth May Collide With Another Planet"꯫ Fox News꯫ 11 June 2009 ꯫ ꯆꯠꯅꯕ ꯆꯩꯆꯠ - 8 September 2011 ꯫  
  73. Template:Citation
  74. Template:Citation
  75. Template:Citation
  76. Hecht, Jeff꯫ "Science: Fiery Future for Planet Earth"꯫ New Scientist꯫ 2 April 1994꯫ ꯂꯃꯥꯏ - 14 ꯫ ꯆꯠꯅꯕ ꯆꯩꯆꯠ - 29 October 2007 ꯫  
  77. Chyba, C. F.; Jankowski, D. G.; Nicholson, P. D. (1989). "Tidal Evolution in the Neptune-Triton System". Astronomy and Astrophysics. 219: 23. Bibcode:1989A&A...219L..23C.
  78. Cox, J. T.; Loeb, Abraham (2007). "The Collision Between The Milky Way And Andromeda". Monthly Notices of the Royal Astronomical Society. 386 (1): 461–474. arXiv:0705.1170. Bibcode:2008MNRAS.386..461C. doi:10.1111/j.1365-2966.2008.13048.x.
  79. Template:Cite web
  80. Template:Cite news
  81. Braine, J.; Lisenfeld, U.; Duc, P. A.; et al. (2004). "Colliding molecular clouds in head-on galaxy collisions". Astronomy and Astrophysics. 418 (2): 419–428. arXiv:astro-ph/0402148. Bibcode:2004A&A...418..419B. doi:10.1051/0004-6361:20035732.
  82. 82.0 82.1 82.2 82.3 Schroder, K. P.; Connon Smith, Robert (2008). "Distant Future of the Sun and Earth Revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x.
  83. Powell, David (January 22, 2007), "Earth's Moon Destined to Disintegrate", Space.com, Tech Media Network, retrieved 2010-06-01.
  84. Cite error: Invalid <ref> tag; no text was provided for refs named Kargel2003
  85. Lorenz, Ralph D.; Lunine, Jonathan I.; McKay, Christopher P. (1997). "Titan under a red giant sun: A new kind of "habitable" moon" (PDF). Geophysical Research Letters. 24 (22): 2905–2908. Bibcode:1997GeoRL..24.2905L. doi:10.1029/97GL52843. PMID 11542268. Retrieved 21 March 2008.
  86. Rybicki, K. R.; Denis, C. (2001). "On the Final Destiny of the Earth and the Solar System". Icarus. 151 (1): 130–137. Bibcode:2001Icar..151..130R. doi:10.1006/icar.2001.6591.
  87. Balick, Bruce. Planetary Nebulae and the Future of the Solar System. University of Washington. Retrieved on 23 June 2006
  88. Kalirai, Jasonjot S.; et al. (March 2008). "The Initial-Final Mass Relation: Direct Constraints at the Low-Mass End". The Astrophysical Journal. 676 (1): 594–609. arXiv:0706.3894. Bibcode:2008ApJ...676..594K. doi:10.1086/527028.
  89. Based upon the weighted least-squares best fit on p. 16 of Kalirai et al. with the initial mass equal to a solar mass.
  90. Universe May End in a Big Rip (1 May 2003). Retrieved on 22 July 2011
  91. Template:Cite journal
  92. Vikhlinin, A.; Kravtsov, A.V.; Burenin, R.A.; et al. (2009). "Chandra Cluster Cosmology Project III: Cosmological Parameter Constraints". The Astrophysical Journal. 692 (2): 1060–1074. arXiv:0812.2720. Bibcode:2009ApJ...692.1060V. doi:10.1088/0004-637X/692/2/1060.
  93. Template:Cite book
  94. Template:Cite book
  95. Template:Cite book
  96. Template:Cite web
  97. 97.0 97.1 Loeb, Abraham (2011). "Cosmology with Hypervelocity Stars". Harvard University. 2011 (4): 023. arXiv:1102.0007. Bibcode:2011JCAP...04..023L. doi:10.1088/1475-7516/2011/04/023.
  98. Chown, Marcus (1996). Afterglow of Creation. University Science Books, 210. Template:ISBN missing
  99. The Local Group of Galaxies. Students for the Exploration and Development of Space. Retrieved on 2 October 2009
  100. Adams, F. C.; Graves, G. J. M.; Laughlin, G. (December 2004). García-Segura, G.; Tenorio-Tagle, G.; Franco, J.; Yorke, H. W., eds. "Gravitational Collapse: From Massive Stars to Planets. / First Astrophysics meeting of the Observatorio Astronomico Nacional. / A meeting to celebrate Peter Bodenheimer for his outstanding contributions to Astrophysics: Red Dwarfs and the End of the Main Sequence". Revista Mexicana de Astronomía y Astrofísica (Serie de Conferencias). 22: 46–49. Bibcode:2004RMxAC..22...46A. See Fig. 3.
  101. 101.0 101.1 Template:Cite book
  102. Template:Citation
  103. Template:Cite journal
  104. Template:Cite journal
  105. Template:Cite journal
  106. Tayler, Roger John (1993). Galaxies, Structure and Evolution, 2, Cambridge University Press, 92. ISBN 978-0521367103. 
  107. (19 May 1988) The Anthropic Cosmological Principle, foreword by John A. Wheeler, Oxford: Oxford University Press. LC 87-28148. ISBN 978-0192821478. Retrieved on 31 December 2009. 
  108. (1999) The Five Ages of the Universe. New York: The Free Press, 85–87. ISBN 978-0684854229. 
  109. 109.0 109.1 109.2 109.3 109.4 109.5 Dyson, Freeman J. (1979). "Time Without End: Physics and Biology in an Open Universe". Reviews of Modern Physics. 51 (3): 447–460. Bibcode:1979RvMP...51..447D. doi:10.1103/RevModPhys.51.447. Retrieved 5 July 2008.
  110. Nishino, Super-K Collaboration, et al. (2009). "Search for Proton Decay via Template:Subatomic particleTemplate:Subatomic particleTemplate:Subatomic particle and Template:Subatomic particleTemplate:Subatomic particleTemplate:Subatomic particle in a Large Water Cherenkov Detector". Physical Review Letters. 102 (14): 141801. arXiv:0903.0676. Bibcode:2009PhRvL.102n1801N. doi:10.1103/PhysRevLett.102.141801. PMID 19392425.
  111. 111.0 111.1 (2000) One Universe: At Home in the Cosmos. Joseph Henry Press. ISBN 978-0309064880. 
  112. 112.0 112.1 112.2 Page, Don N. (1976). "Particle Emission Rates from a Black Hole: Massless Particles from an Uncharged, Nonrotating Hole". Physical Review D. 13 (2): 198–206. Bibcode:1976PhRvD..13..198P. doi:10.1103/PhysRevD.13.198. See in particular equation (27).
  113. Template:Cite journal
  114. Carroll, Sean M.; Chen, Jennifer (27 Oct 2004). "Spontaneous Inflation and the Origin of the Arrow of Time". arXiv:hep-th/0410270.
  115. Template:Cite journal
  116. Template:Cite journal
  117. M. Douglas, "The statistics of string / M theory vacua", JHEP 0305, 46 (2003). Template:Arxiv; S. Ashok and M. Douglas, "Counting flux vacua", JHEP 0401, 060 (2004).
  118. Template:Cite bookTemplate:ISBN missing
  119. Template:Cite bookTemplate:ISBN missing
  120. Carter, Brandon; McCrea, W. H. (1983). "The anthropic principle and its implications for biological evolution". Philosophical Transactions of the Royal Society of London. A310 (1512): 347–363. Bibcode:1983RSPTA.310..347C. doi:10.1098/rsta.1983.0096.
  121. Template:Cite bookTemplate:ISBN missing
  122. Template:Cite journal
  123. Kaku, Michio (2010). The Physics of Interstellar Travel: To one day, reach the stars. mkaku.org. Retrieved on 29 August 2010
  124. Template:Cite journal
  125. Template:Cite bookTemplate:ISBN missing
  126. Template:Cite journal
  127. Template:Cite bookTemplate:ISBN missing
  128. Template:Cite journal
  129. Template:Cite journal
  130. "Hurtling Through the Void"꯫ Time꯫ 20 June 1983 ꯫ ꯆꯠꯅꯕ ꯆꯩꯆꯠ - 5 September 2011 ꯫  
  131. Template:Cite book
  132. Cornell News: "It's the 25th Anniversary of Earth's First (and only) Attempt to Phone E.T.". Cornell University (12 November 1999). Archived from the original on 2 August 2008 ꯫ Retrieved on 29 March 2008
  133. Template:Cite web
  134. Pioneer 10 Spacecraft Nears 25TH Anniversary, End of Mission. nasa.gov. Retrieved on 2013-12-22
  135. Space Flight 2003 – United States Space Activities. nasa.gov. Retrieved on 2013-12-22
  136. 136.0 136.1 Voyager: The Interstellar Mission. NASA. Retrieved on 5 September 2011
  137. KEO FAQ. keo.org. Retrieved on 14 October 2011
  138. Template:Cite web
  139. 139.0 139.1 The Pioneer Missions. NASA. Retrieved on 5 September 2011
  140. LAGEOS 1, 2. NASA. Retrieved on 21 July 2012
  141. Template:Cite AV media
  142. The Long Now Foundation. The Long Now Foundation (2011). Retrieved on 21 September 2011
  143. Template:Cite news
  144. Template:Cite web
  145. Template:Cite web
  146. Template:Cite journal
  147. Template:Cite journal
  148. Template:Cite journal
  149. Template:Cite web
  150. Template:Cite web
  151. Template:Cite bookTemplate:ISBN missing
  152. Template:Citation
  153. Template:Cite web
  154. Template:Cite bookTemplate:ISBN missing
  155. Template:Citation
  156. Template:Citation, Review in Stanford Archaeolog
  157. 157.0 157.1 157.2 157.3 157.4 157.5 157.6 157.7 157.8 Template:Cite journal
  158. Why is Polaris the North Star?. NASA. Archived from the original on 25 July 2011 ꯫ Retrieved on 10 April 2011
  159. 159.0 159.1 Plait, Phil (2002). Bad Astronomy: Misconceptions and Misuses Revealed, from Astrology to the Moon Landing "Hoax". John Wiley and Sons, 55–56. Template:ISBN missing
  160. Template:Cite bookTemplate:ISBN missing
  161. Template:Citation
  162. Template:Cite web
  163. Template:Cite bookTemplate:ISBN missing
  164. Template:Cite bookTemplate:ISBN missing
  165. Laskar, J.; et al. (1993). "Orbital, Precessional, and Insolation Quantities for the Earth From ?20 Myr to +10 Myr". Astronomy and Astrophysics. 270: 522–533. Bibcode:1993A&A...270..522L.
  166. Laskar. Astronomical Solutions for Earth Paleoclimates. Institut de mécanique céleste et de calcul des éphémérides. Retrieved on 20 July 2012
  167. Template:Cite web
  168. Template:Cite journal
  169. Template:Cite web
  170. Borkowski, K.M. (1991). "The Tropical Calendar and Solar Year". J. Royal Astronomical Soc. Of Canada. 85 (3): 121–130. Bibcode:1991JRASC..85..121B.
  171. Template:Cite web
  172. Strous, Louis (2010). Astronomy Answers: Modern Calendars. University of Utrecht. Retrieved on 14 September 2011
  173. Template:Cite bookTemplate:ISBN missing
  174. Julian Date Converter. US Naval Observatory. Retrieved on 20 July 2012
  175. Template:Cite web
  176. Template:Cite book
  177. 177.0 177.1 Template:Cite news
  178. Template:Cite web
  179. 179.0 179.1 Template:Cite journal
  180. Cohen, Bernard L. (January 1983). "Breeder Reactors: A Renewable Energy Source" (PDF). American Journal of Physics. 51 (1): 75. Bibcode:2005BGD.....2.1665F. doi:10.1119/1.13440.

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