Tag: Geophysics

  • How volcanoes shaped our planet — and why we need to be ready for the next big eruption

    How volcanoes shaped our planet — and why we need to be ready for the next big eruption

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    Adventures in Volcanoland: What Volcanoes Tell Us About the World and Ourselves Tamsin Mather Abacus (2024)

    Unlike Alice in Alice in Wonderland, volcanologists cannot fall down a deep rabbit hole to discover what goes on in the bowels of the Earth. Instead, they scour the surface and examine the chemistry of emitted gases, lava and rocks ejected during eruptions. Only by combining many clues can researchers learn where and how molten rock (magma) forms, how it ascends from the mantle below Earth’s crust and what triggers volcanic eruptions.

    In Adventures in Volcanoland, volcanologist Tamsin Mather takes readers on a journey to some of the world’s most notorious and active volcanoes — from Mount Vesuvius in Italy to Masaya in Nicaragua. Her eloquent and enchanting book, which is rich in analogies and anecdotes, weaves together geological, historical and personal stories to explain how volcanoes work, how they have shaped our planet and how they have been understood through history.

    Volcanoes’ captivating power clearly entrances Mather, as it does me. And volcanoes make volcanologists work hard to uncover their secrets. Mather explains how researchers, equipped with the geochemical equivalent of a stethoscope, listen to the beating pulses of volcanoes. Scientists can also capture volcanoes’ ‘breath’ — toxic gases that often enshroud Mather as she works and that eat away at her clothes. Mather describes navigating through thick jungle in Guatemala to collect samples of lava while volcanic blasts hurled plumes of ash into the sky. Repairs to broken equipment had to be improvised using duct tape and superglue. Mather once resorted to using an inverted children’s paddling pool to collect gases fizzing up inside the caldera of Santorini volcano in Greece. The effort is worth it, Mather explains, to help volcanologists to answer big questions, such as how eruptions alter the climate and our environment, and how they affect life on Earth.

    Volcanologists must exploit a vast array of knowledge, from planetary-scale shifts in Earth’s carbon cycle to the analysis of trapped gases in microscopic beads of glass. They must put eruptions in geological context, on timescales from Earth’s formation more than four billion years ago to the rapid radioactive decay of gases emitted by magma (such as radon-222, with a half-life of just under four days).

    Each rock tells a story

    Mather describes human experiences of volcanic eruptions, including her own time spent staring into churning lakes of molten rock, a “roiling, red and restless” fiery sea. She first encountered volcanoes and their hazards as a child, when she visited Vesuvius and the former Roman towns of Pompeii and Herculaneum. In ad 79, several scorching (350–550 ºC), fast-moving clouds of ash, pumice and gases surged down the flanks of Vesuvius, with devastating consequences for the people below, including hundreds who had taken refuge at the waterfront in Herculaneum, waiting to flee by boat.

    Today, tourists standing at the excavated pre-eruption shoreline are presented with an intimidating wall of volcanic deposits. After the eruption, the land surface gained up to 20 metres of elevation, and the coastline moved seawards by one kilometre. And all this happened in a geological blink of an eye.

    Looking down from the crater rim of Mount Vesuvius towards the urban sprawl of metropolitan Naples, now home to around three million people, it’s sobering to consider just how the city will respond to the next large eruption of the slumbering volcano. It’s hard to know when that will be, but managing a future evacuation will be a colossal task for the authorities.

    To prepare and plan, it is essential to better understand the hazards of volcanic regions. By ‘reading the rocks’ deposited by volcanoes, layer upon layer over thousands or millions of years, volcanologists can unravel the frequency, style and magnitudes of past eruptions. For example, rock stripes exposed in the walls of the Santorini caldera reveal how the catastrophic 1600 bc Minoan eruption unfolded; underwater studies of rocks point to other events that were much larger than previously thought. The consequences of another large eruption in the Eastern Mediterranean would be grave.

    Satellite image of the Hunga Tonga-Hunga Ha'apai volcano on 24 December 2021, before the eruption on 14 January 2022

    The Hunga Tonga-Hunga Ha’apai volcano in the South Pacific.Credit: Maxar via Getty

    Volcanic and sedimentary rocks, along with signals from deposited sulphate in ice cores, hold clues about how eruptions have altered conditions across our planet. The impacts can be temporary or permanent. Plumes of sulphur dioxide gas can trigger short periods of global cooling called volcanic winters, such as the one following the 1815 eruption of Tambora in Indonesia. Lengthy outpourings of lava can form large igneous provinces — huge accumulations of volcanic rocks, such as the Siberian Traps. In the past, such events might have led to significant changes in planetary conditions that affected the course of life on Earth. As Mather points out, four out of the five largest mass extinctions overlapped approximately in time with volcanic activity that formed large igneous provinces, which would have pumped out vast amounts of carbon dioxide over millions of years.

    Plan for big eruptions

    All this raises the question of how prepared we are for the next large-scale volcanic eruption. Not very, I would argue. Humans have short memories — the COVID-19 pandemic showed us that, only 100 years after the severe influenza pandemic that began in 1918, we were still not ready.

    Monitoring of volcanoes has advanced tremendously, with support from satellites in space, but they can still catch us off guard. For example, the powerful 2022 eruption of Hunga Tonga–Hunga Ha‘apai in Tonga was unexpected and had global ramifications. A shockwave and tsunamis reached the coasts of North and South America, resulting in an oil spill and two drownings in Peru. Tsunami warnings and evacuation orders were issued in Japan, and beaches were in Australia. Water vapour launched into the stratosphere by the blast could temporarily boost global temperatures.

    Population growth, technology dependency and the increased complexity of global systems have put the world at catastrophic risk from volcanic eruptions. Today, more than 800 million people in more than 85 countries live within 100 kilometres of an active volcano. An eruption near densely populated areas would have disastrous immediate impacts. Pyroclastic flows — fast-moving mixtures of hot gas, ash and rock fragments — could wipe out entire cities. Metres-thick ash falls would devastate crops and overwhelm power lines, water-treatment facilities, ventilation and heating systems, machinery and more. Farther away, flights might be grounded, power grids and undersea cables could be damaged and food security and supply chains could be affected, spreading economic losses.

    With little regard for international borders, large eruptions’ far-reaching impacts would require a rapid and coordinated national and international response. Yet, global preparedness for the impacts of volcanic eruptions is lacking. There is no international United Nations treaty organization for ‘operational volcanology’ (systematic monitoring of volcanoes and assessment of risk). There’s no global coordination on issuing cross-border volcanic hazard warnings that address the full range of threats: pyroclastic flow, tephra fall (deposits of lofted rock fragments), lava flow, lahar (volcanic mudflow), volcanic gases, rafting pumice, drifting ash, tsunami and lightning.

    Tambora-size eruptions occur somewhere in the world once or twice every millennium on average, and every 400 years in the Asia Pacific region. It’s not a matter of if, but when.

    Adventures in Volcanoland reminds us that we should all keep careful watch on the world’s volcanoes. They are more than alluring natural landmarks. They are powerful drivers of processes on our planet that are crucial to understand. Volcano enthusiasts, those interested in the history of this adventurous science and those questioning our place in the world will find much to enjoy in this absorbing book.

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  • Geoscientists are using telecom ‘dark fibres’ to map Earth’s innards

    Geoscientists are using telecom ‘dark fibres’ to map Earth’s innards

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    Fibre optic cables designed to carry telecommunications can also be used to map Earth’s interior

    Connect world/Shutterstock

    Offline telecom cables called “dark fibres” can be used to sense underground seismic waves. Geophysicists are increasingly using such signals to study aspects of Earth’s subsurface, including hidden sources of geothermal energy and earthquake hazards.

    “If a large earthquake happens on the fibre on which we are speaking, the frequencies in my voice would be slightly distorted,” Andreas Fichtner at ETH Zurich in Switzerland told New Scientist on a video call.

    He is referring to…

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  • Taiwan hit by biggest earthquake in 25 years: why scientists weren’t surprised

    Taiwan hit by biggest earthquake in 25 years: why scientists weren’t surprised

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    Scientists warn that more shocks are likely after Taiwan was rocked by the most powerful earthquake to hit the island in 25 years, killing several people, flattening buildings, and triggering landslides. Geologists warn that the location of the epicentre is in a complex network of offshore faults, making aftershocks or even another quake a possibility.

    The magnitude-7.4 tremor struck under the ocean, 18 kilometres south of the east-coast city of Hualien just before 8am on Wednesday morning local time, according to measurements gathered by the US Geological Survey. Since then, dozens of aftershocks have rattled the island, including a 6.4 magnitude tremor that occurred roughly two hours after the main quake. “Everyone experienced the shaking,” says Kuo-Fong Ma, a seismologist at National Central University in Taoyuan City, Taiwan.

    The earthquake occurred at a relatively shallow 35 kilometres deep, resulting in stronger tremors than those produced by quakes that erupt farther below the Earth’s surface. Authorities issued tsunami warnings in Taiwan, Japan and the Philippines, though they later downgraded them. A 30-centimetre-high wave rolled into Yonaguni Island in the south of Japan about 15 minutes after the tremor. The earthquake’s effects were also reportedly felt in parts of mainland China.

    Taiwan’s vulnerability to earthquakes is no surprise given it is situated in one of the most seismically active regions in the world, says Meghan Miller, a seismologist at the Australian National University in Canberra. The east coast of the island sits on top of two converging tectonic plates: the Philippine Sea and Eurasian plates. Many of the earthquakes that occur on the eastern side of Taiwan are due to the Philippine Sea plate sliding underneath the Eurasian plate, says Miller.

    The location of the earthquake’s underwater epicentre offers clues to its mechanics, says Yu Wang, a geologist at National Taiwan University in Taipei. The earthquake occurred on a reverse fault, which means one chunk of rock shifted vertically relative to the other. “We believe this is the cause of the current earthquake,” says Wang. He adds that the area where the earthquake occurred contains a complex network of faults, and that the latest rupture probably produced a crack between 40 and 50 kilometres long.

    In the coming days, dozens of aftershocks are expected to shake Taiwan further, says Wang. The force of the earthquake has already triggered landslides in mountainous areas, which could worsen with more tremors and make rescue efforts more challenging, adds Miller. In flat areas, aftershocks could also lead to the ground becoming soft and water-logged, which can amplify seismic waves and damage compromised buildings further. “There can be additional damage on top of what originally occurred in the first event,” says Miller.

    Several earthquakes have occurred in Taiwan over the past century, with those reaching magnitude 7 usually occurring roughly every 30 years, says Ma. One of the most devastating earthquakes to hit the island occurred in 1999, when a magnitude-7.6 tremor struck the western side of the island. It resulted in more than 2,400 deaths and reduced thousands of buildings to rubble.

    But in the past two decades, Taiwan has ramped up its efforts to reduce the impact of earthquakes, says Ma. The island has an early warning system that alerts cities and regions via a telephone call a few seconds after an earthquake strikes. She adds that many buildings have been modified to withstand strong earthquakes, and several seismology stations have been installed across the island to take real-time measurements. Ma and her colleagues are also developing sensors for measuring the shaking intensity inside buildings to help people determine their risk during an earthquake. “I think that will be the future,” she says.

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  • A global timekeeping problem postponed by global warming

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  • Melting ice solves leap-second problem — for now

    Melting ice solves leap-second problem — for now

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    THE TOPIC IN BRIEF

    • Timekeeping is determined by ultraprecise devices called atomic clocks, but it is also aligned with Earth’s rotation, mainly for historical reasons.

    • Because the planet’s rate of rotation fluctuates, this alignment is maintained with the occasional addition of ‘leap seconds’ to the official time standard.

    • Now, Earth’s rotation seems to have accelerated, outpacing the time standard, and raising the possibility that an unprecedented ‘negative’ leap second might soon be required — a daunting prospect in a world reliant on consistent timekeeping.

    • Agnew1 reports that human-induced melting of polar ice exerts a slowing effect on Earth’s rotation, effectively delaying a decision on the need for a negative leap second.

    PATRIZIA TAVELLA: International timekeeping

    In 1967, the internationally accepted definition of the second changed. The time measurement standard had been linked to Earth’s rotation, but instead became determined by a quantum transition between two states of a caesium atom. The change was motivated by accuracy: caesium atomic clocks keep time on the basis of the ultrastable frequency of the photons exchanged in the quantum transition. This seemed like a safer bet than Earth’s movements, which weren’t as regular as was first assumed.

    But sailors still relied on the Sun and stars to navigate, and they wanted a time standard that remained tied in some way to Earth’s rotation. It was therefore decided that the new international reference, known as coordinated universal time (utc), would be set by atomic clocks, but kept apace with the rotational angle of Earth, which is known as universal time (ut1). Since 1972, utc has been adjusted to meet this goal by adding a leap second whenever the discrepancy between the two standards approaches one second.

    Atomic clocks have enabled the development of great technologies, such as satellite navigation and, in an age of the global navigation satellite system (GNSS), celestial navigation is much less relevant than it was in 1972. GNSS satellites themselves have onboard atomic clocks that regulate their timekeeping, and the insertion of a leap second generates risk of failures. Perhaps more importantly, the addition of leap seconds can have drastic effects on computer infrastructure in the increasingly connected modern world (see go.nature.com/44y88yp).

    For these reasons, after more than 20 years of discussion, metrologists proposed that utc be kept in line with Earth’s rotation, but that the tolerance for adding an adjustment be increased to a value larger than one second2. This proposal, which delays the need to make any adjustment for at least another century, was adopted by the General Conference on Weights and Measures (CGPM) in 2022.

    The CGPM resolution stipulates that the maximum difference between the two times (denoted ut1 − utc) will be increased in or before 2035, and that the details of the new maximum and how it is to be implemented will be decided at the next CGPM meeting in 2026 (see go.nature.com/3vqddy2). Most delegates urge a quick implementation of the new rules, although others ask for more time to adapt their systems. The radiocommunication sector of the International Telecommunication Union — the organization that regulates the transmission of time signals — endorsed the CGPM decisions at the World Radiocommunication Conference in 2023.

    utc is currently computed using data from about 450 atomic clocks, which are maintained in more than 80 institutions around the world. It is disseminated in real time by these time laboratories, by means such as radio or telephone signals, the Internet or optical fibre protocols, and also through GNSS signals. Since 1972, irregularities in Earth’s movement have called for 27 leap seconds to be added — at irregular intervals and with a maximum of only 6 months’ notice each time. The irony is that metrologists now face the challenge of removing a leap second from utc for the first time, because Earth’s rotation is gradually getting faster than the time standard set by atomic clocks (Fig. 1).

    figure 1

    Figure 1 | Synchronizing the international time with Earth’s rotation. Agnew1 calculated the difference between international atomic time (tai), which is measured using ultraprecise quantum devices known as atomic clocks, and universal time (ut1), which is determined by Earth’s rotation. tai, with the addition of occasional ‘leap seconds’, defines coordinated universal time (utc), which is kept in alignment with ut1. Earth’s current rate of rotation suggests that the first negative leap seconds might soon be necessary owing to a combination of geophysical effects. Agnew’s calculation shows that accelerated melting of the polar ice caps has delayed the need for these adjustments. (Adapted from Fig. 2d of ref. 1.)

    A negative leap second has never been added or tested, so the problems it could create are without precedent. Metrologists around the world are following the unfolding discussion attentively, with the view to avoiding any unnecessary risks. What would be necessary, as in good metrological practice, is to calculate the uncertainty associated with predictions of Earth’s rotation. This information would allow researchers to evaluate the probability that a negative leap second will be required — and assess the related risks — so that they can anticipate any such change before 2035. Unfortunately, this task remains formidable (ref. 3 and go.nature.com/4armrvz), so Agnew’s suggestion that the change could be delayed is welcome news indeed.

    JERRY X. MITROVICA: In search of lost time

    Earth’s rotation is an imperfect timekeeper. This imperfection is imperceptible to humans, but the exquisite accuracy of atomic clocks makes it clear that the time taken for the planet to make one full turn varies from day to day.

    On a millennial timescale, changes in Earth’s rotation reflect the combined effect of three geophysical processes4. First, friction between ocean water and the sea floor — both in shallow seas and in the deep ocean — has progressively slowed Earth’s rotation. This effect is known as tidal dissipation. Second, since the last ice age ended, Earth has undergone shape adjustments that have increased its rotation rate. These ongoing changes have brought the planet back to a shape that is more spherical than the flattened form it took when massive ice sheets existed in its polar regions. Finally, the coupling between Earth’s iron core and its outer rocky mantle and crust means that any change in the angular momentum of the core must be balanced by a change of equal magnitude and opposite sign in the mantle and crust.

    Although the individual contribution of each process is somewhat uncertain, their sum is known precisely: it has led to an increase in Earth’s rotation period of 6 millionths of a second per year4. This slowing might seem trivially small, but its effect is responsible for a phenomenon known as clock error. This error describes a discrepancy in the timing of eclipses: events recorded by ancient astronomers seem to have occurred at times that differ from those predicted by assuming that Earth’s rotation rate has remained unchanged since ancient times. Clock error increases with the age of the eclipse and reaches around 4 hours for eclipses that were observed 2,500 years ago5.

    The effects of tidal dissipation and shape adjustments have not changed appreciably since the advent of modern atomic timekeeping, but the impact of core–mantle coupling on Earth’s rotation varies on multiple timescales as a result of the fluid nature of the outer core. And herein lies the probable cause of timekeeping’s most recent dilemma: leap seconds have been required with much lower frequency since 2000 than in the previous 30 years, which indicates that Earth’s rotation rate is accelerating. Given the stability of tidal dissipation and shape-adjustment effects over this period, the main culprit must be core–mantle coupling. However, Agnew’s findings suggest that there is another factor at play.

    Agnew analysed changes in Earth’s rotation and in its gravity field — changes in the latter arising through the redistribution of mass on Earth’s surface. His analysis demonstrates persuasively that core–mantle coupling has led to accelerated rotation, but that there has also been a pronounced deceleration owing to the onset of major melting of polar ice sheets that began near the end of the twentieth century. This human-induced process is slowing rotation by moving melted ice mass from the poles to lower latitudes.

    Core–mantle coupling alone could have necessitated a negative leap second in about two years’ time. According to Agnew’s calculations, changes in polar ice mass have delayed this eventuality by another three years, to 2029. But no realistic projection of future ice-mass changes will thwart the need for a negative leap second beyond the next decade. Unless international timekeeping guidelines change soon, the myriad technological foundations of human society must be updated in preparation for this unprecedented event, and for the disappearance of 23:59:59 on a single day in the not-too-distant future.

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  • Climate change has slowed Earth’s rotation — and could affect how we keep time

    Climate change has slowed Earth’s rotation — and could affect how we keep time

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    Climate change is starting to alter how humans keep time.

    An analysis1 published in Nature on 27 March has predicted that melting ice caps are slowing Earth’s rotation to such an extent that the next leap second — the mechanism used since 1972 to reconcile official time from atomic clocks with that based on Earth’s unstable speed of rotation — will be delayed by three years.

    “Enough ice has melted to move sea level enough that we can actually see the rate of theEarth’s rotation has been affected,” says Duncan Agnew, a geophysicist at the Scripps Institution of Oceanography in La Jolla, California, and author of the study.

    According to his analysis, global warming will push back the need for another leap second from 2026 to 2029. Leap seconds cause so much havoc for computing that scientists have voted to get rid of them, but not until 2035. Researchers are especially dreading the next leap second, because, for the first time, it is likely to be a negative, skipped second, rather than an extra one added in.

    “We do not know how to cope with one second missing. This is why time metrologists are worried,” says Felicitas Arias, former director of the Time Department at the International Bureau of Weights and Measures in Sèvres, France.

    In metrology terms, the three-year delay “is good news”, she says, because even if a negative leap second is still needed, it will happen later, and the world might see fewer of them before 2035 than would otherwise have been anticipated.

    But this should not be seen as a point in favour of global warming, Agnew says. “It’s completely outweighed by all the negative aspects.”

    Synchronizing clocks

    For millennia, people measured time using Earth’s rotation, and the second became defined as a fraction of the time it takes for the planet to turn once on its axis. But since 1967, atomic clocks — which tick using the frequency of light emitted by atoms — have served as more precise timekeepers. Today, a suite of around 450 atomic clocks defines official time on Earth, known as Coordinated Universal Time (utc), and leap seconds are used every few years to keep utc in line with the planet’s natural day.

    Atomic clocks are better timekeepers than Earth, because they are stable over millions of years, whereas the planet’s rotation rate varies. In his analysis, Agnew used mathematical models to tease apart the contributions of known geophysical phenomena to Earth’s rotation and to predict their effects on future leap seconds.

    Many metrologists anticipated that leap seconds would only ever be added, because on the scale of millions of years, Earth’s spin is slowing down, meaning that, occasionally, a minute in utc needs to be 61 seconds long, to allow Earth to catch up. This reduction in the planet’s rotation rate is caused by the Moon’s pull on the oceans, which creates friction. It also explains, for example, why eclipses 2,000 years ago were recorded at different times in the day from what we would expect on the basis of today’s rotation rate, and why analyses of ancient sediments suggest that 1.4 billion years ago a day was only around 19 hours long.

    But on shorter timescales, geophysical phenomena make the rotation rate fluctuate, says Agnew. Right now, the rate at which Earth spins is being affected by currents in the liquid core of the planet, which since the 1970s have caused the rotation speed of the outer crust to increase. This has meant that added leap seconds are needed less frequently, and if the trend continues, a leap second will need to be removed from utc.

    Agnew’s analysis finds that this could happen later than was previously thought, because of climate change. Data from satellites mapping Earth’s gravity show that since the early 1990s the planet has become less spherical and more flattened, as ice from Greenland and Antarctica has melted and moved mass away from the poles towards the Equator. Just as a spinning ice skater slows down by extending their arms away from their body (and speeds up by pulling them in), this flow of water away from Earth’s axis of rotation slows the planet’s spin.

    The net result of core currents and of climate change is still an accelerating Earth. But Agnew found that without the effect of melting ice, a negative leap second would be needed three years earlier than is now predicted. “Human activities have a profound impact on climate change. The postponing of a leap second is just one more example,” says Jianli Chen, a geophysicist at the Hong Kong Polytechnic University.

    Precision problems

    A delayed leap second would be welcomed by metrologists. Leap seconds are a “big problem” already, because in a society that is increasingly based on precise timing, they lead to major failures in computing systems, says Elizabeth Donley, who heads the time and frequency division at the National Institute of Standards and Technology in Boulder, Colorado.

    An unprecedented negative leap second could be even worse. “There’s no accounting for it in all the existing computer codes,” she says.

    Agnew’s paper is useful in making predictions, but Donley says that there is still high uncertainty about when a negative leap second will be needed. The calculations rely on Earth’s acceleration continuing at its present rate, but activity in the inner core is almost impossible to predict, cautions Christian Bizouard, an astrogeophysicist at the International Earth Rotation and Reference Systems Service in Paris, which is responsible for deciding when to introduce a leap second. “We do not know when that mean acceleration will stop and reverse itself,” he says.

    Agnew hopes that seeing the influence of climate change on timekeeping will jolt some people into action. “I’ve been around climate change for a long time, and I can worry about it plenty well without this, but it’s yet another way of impressing upon people just how big a deal this is,” he says.

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  • Disappearing cities on US coasts

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    VLM data

    High-resolution VLM data are based on the Virginia Tech Earth Observation and Innovation (EOI) Lab VLM product, with spatially continuous coverage for the Pacific, Atlantic and Gulf coasts of the USA27,28,51,52,53. The dataset provides VLM measurements at millimetre-level accuracy and a resolution of about 50 m within a 100-km strip along the coasts of the USA. For each coast, the VLM rates were determined by integrating SAR images from Sentinel-1 A/B and ALOS-1 satellites between 2007 and 2020 (see Supplementary Table 23 for satellite frames used for each coast) with observations of horizontal and vertical velocities at global navigation satellite system (GNSS) stations. To produce the spatially continuous surface-deformation map, InSAR line-of-sight (LOS) displacements were generated for the numerous SAR frames along the coasts.

    We use GAMMA software to process SAR datasets54,55 and the wavelet-based InSAR (WabInSAR) algorithm to perform post-processing and multitemporal analysis56,57,58,59,60 (Supplementary Fig. 4a). To this end, thousands of high-quality interferograms were generated and several wavelet‐based analyses were applied to the interferograms to denoise the pixels and reduce the effects of spatially uncorrelated DEM error56,57 and topographically correlated atmospheric phase delay57. Next, the velocity along the LOS direction for each pixel is calculated as the slope of the best-fitting line to the associated time series using a reweighted least-squares estimation. Last, the numerous SAR frames are mosaiced following Ojha et al.61 and a stochastic model, which combines the LOS velocities with the GNSS datasets, was adopted to generate a high-resolution map of the VLM rate (Supplementary Fig. 4b).

    To implement the stochastic model, we resampled the LOS velocities of Sentinel-1 tracks onto the ALOS track and interpolated the GNSS velocities on the pixels within the ALOS track using a Kriging interpolation technique with inverse distance weighting. Thus, we obtain several (5) observations per pixel for each coast, including LOS observations and GNSS velocities. Let {y0, y1,…, ym} and \(\{{\sigma }_{0}^{2},{\sigma }_{1}^{2},\ldots {\sigma }_{m}^{2}\}\) be the interpolated LOS velocities and variances, respectively, for a given pixel, in which subscripts 0, 1,…, m indicate the available satellite observations (Sentinel-1/ALOS-1) and orbits (ascending/descending) for a given US coast (Atlantic/Gulf/Pacific), as defined in Supplementary Table 23. The stochastic model to combine the LOS velocities with the velocities of GNSS datasets to generate a seamless, high-resolution and accurate map of east (E), north (N) and vertical (U) motions is given by equation (1):

    $$\begin{array}{c}{y}_{0,1,\ldots m}={C}_{{\rm{e}}}^{0,1,\ldots m}E+{C}_{{\rm{n}}}^{0,1,\ldots m}N+{C}_{{\rm{u}}}^{0,1,\ldots m}U+{\varepsilon }^{0,1,\ldots m}\\ {E}_{{\rm{G}}}=E+{\varepsilon }^{{\rm{e}}}\\ \begin{array}{c}{N}_{{\rm{G}}}=N+{\varepsilon }^{{\rm{n}}}\\ {U}_{{\rm{G}}}=U+{\varepsilon }^{{\rm{u}}}\end{array}\end{array}$$

    (1)

    in which C represents the unit vectors projecting 3D displacements onto the LOS, which is a function of the satellite heading and incidence angles, ε is the observation errors equal to the standard deviations (σ), E, N and U are the unknowns and EG, NG and UG are the observed interpolated east, north and up GNSS velocities, respectively. The solution to equation (1) is given by equation (2):

    $$X={\left({A}^{{\rm{T}}}PA\right)}^{-1}{A}^{{\rm{T}}}PL$$

    (2)

    in which X represents the unknowns, A is the Green’s function given by the unit vectors (C), L is the observation and P is the weight matrix, which is inversely proportional to the observant variance (σ2). The parameters variance-covariance matrix is \({Q}_{XX}=\frac{{r}^{{\rm{T}}}Pr}{{\rm{df}}}{({A}^{{\rm{T}}}PA)}^{-1}\), in which r = L − AX and df is the degrees of freedom. The standard deviations (precision of the results) for each pixel on the Atlantic/Gulf/Pacific coasts are shown in Supplementary Fig. 5a. The spatial distribution of the standard deviation shows that most values are below 3 mm per year for the US Atlantic and Gulf coasts. However, there are a few hotspots of high standard deviation around the Chesapeake Bay area (US Atlantic coast) and around the coast of Florida (US Gulf coast). We note higher estimated standard deviation values in the US Pacific coast, specifically in Northern California and the Orange County basin27 (Supplementary Fig. 5a). Generally, higher standard deviation values represent areas of lower precision. The observed lower precision in some pixels may be attributed to lower interferometric phase signal-to-noise ratio caused by surface vegetation, nonlinearity in the rates between the ALOS and Sentinel-1 observation periods owing to aquifer recharge and depletion, a limited number of GNSS stations used for the adjustment and a comparatively higher standard deviation of the GNSS station in the particular regions20,27,28. Furthermore, we validate the VLM rates using 756 GNSS stations (US Atlantic coast: 218; US Gulf coast: 157; US Pacific coast: 381) from the Nevada Geodetic Laboratory62 and Shirzaei et al.48. To perform the validation, we computed the average InSAR VLM rates within a 200-m radius around each GNSS station for comparison with the corresponding GNSS vertical rates (Extended Data Figs. 2–4). We obtained a standard deviation of 1.5 mm per year and a mean difference of less than 0.3 mm per year for the US Atlantic, Gulf and Pacific coasts (Supplementary Fig. 5b–d).

    Spatial analysis of the complied VLM map (Fig. 1 and Extended Data Figs. 2–4) reveals extensive coastal areas with subsidence rates of more than 3 mm per year. Figure 1e highlights the spatially variable VLM for the 32 major coastal cities selected for this study: US Atlantic coast: Boston, MA; New York City, NY; Jersey City, NJ; Atlantic City, NJ; Virginia Beach, VA; Wilmington, NC; Myrtle Beach, SC; Charleston, SC; Savannah, GA; Jacksonville, FL; Miami, FL; US Gulf coast: Naples, FL; Mobile, AL; Biloxi, MS; New Orleans, LA; Slidell, LA; Lake Charles, LA; Port Arthur, TX; Galveston, TX; Texas City, TX; Freeport, TX; Corpus Christi, TX; US Pacific coast: Richmond, CA; Oakland, CA; San Francisco, CA; South San Francisco, CA; Foster City, CA; Santa Cruz, CA; Long Beach, CA; Huntington Beach, CA; Newport Beach, CA; San Diego, CA.

    We find subsidence rates greater than 2 mm per year in 24 out of 32 major cities along the US Atlantic, Gulf and Pacific coasts, with notable subsidence rates (>5 mm per year) in cities such as Charleston (city number 8), Biloxi (city number 14), Galveston (city number 20) and Corpus Christi (city number 22) (Fig. 1e). On the US Pacific coast, we observe lower rates of land subsidence compared with the Atlantic and Gulf coasts, with some cities characterized by marked uplift (such as Richmond: city number 23; Long Beach: city number 29; Huntington Beach: city number 30; and Newport Beach: city number 31).

    Subsidence along the coast is driven by natural and human processes and is a notable contributor to relative sea-level change2,19,48,49,63,64,65. Earlier studies suggested that complex processes drive observed subsidence along the US coasts27,66,67,68,69. These drivers include a combination of natural and anthropogenic processes, such as GIA, compaction of sediments, groundwater withdrawal, hydrocarbon extraction, surficial drainage/dewatering activities and regional tectonic activities. On a broad scale, disentangling the contribution of natural-driven and anthropogenic-driven processes is important for developing effective strategies to mitigate or adapt to the impacts of subsidence in low-lying coastal cities. On the one hand, in cities in which subsidence is a result of GIA and other natural processes, effective subsidence mitigation will probably involve an adaptive response, such as raised structures and infrastructure and flood-protection measures. On the other hand, for anthropogenic processes, proactive policy interventions and mitigation measures to reduce and control resulting subsidence, such as reducing groundwater and oil and gas extraction or changes in land use, may be helpful in sinking cities. As GIA is the main natural driver, we used the GIA ICE-6G-D model70 to estimate the GIA contributions at the SAR pixels and subtracted its effect from the observed VLM to assess the non-GIA contributions to the estimated VLM along US coasts (Supplementary Fig. 2). The relative reduction of subsidence by 46%, 4% and 20% for the Atlantic, Gulf and Pacific coasts, respectively, suggests that the effect of GIA on subsidence is dominant primarily along the US Atlantic coast and minimal for the Gulf and Pacific coasts (Supplementary Fig. 2c–e). Although the median rates of subsidence are reduced for all 32 major coastal cities, several areas with subsidence rates greater than 2 mm per year remain apparent in more than half of the selected cities, such as Boston, Atlantic City, Charleston, Biloxi, New Orleans, Texas City, San Francisco, Foster City and San Diego (Supplementary Fig. 3).

    Coastal cities selection and elevation data

    To select the 32 cities for analysis, we considered 41 major US coastal cities with VLM and LiDAR DEMs data. We conducted a preliminary analysis to determine the exposed area of each city, considering the IPCC localized (relative) SLR projections and mean high water (MHW) of the nearest tide gauge. Next, we screened the cities on the basis of the largest exposed area and selected ten cities from each US coastal region as follows: US Atlantic coast: Boston, MA; New York City, NY; Atlantic City, NJ; Virginia Beach, VA; Wilmington, NC; Myrtle Beach, SC; Charleston, SC; Savannah, GA; Jacksonville, FL; Miami, FL; US Gulf coast: Naples, FL; Mobile, AL; Biloxi, MS; New Orleans, LA; Slidell, LA; Lake Charles, LA; Port Arthur, TX; Texas City, TX; Freeport, TX; Corpus Christi, TX; US Pacific coast: Richmond, CA; Oakland, CA; San Francisco, CA; South San Francisco, CA; Foster City, CA; Santa Cruz, CA; Long Beach, CA; Huntington Beach, CA; Newport Beach, CA; San Diego, CA.

    On the Pacific coast, we focused only on future inundation hazards for cities in California. The absence of coastal cities from Oregon and Washington is a result of the lack of high-resolution VLM data for the US northwest coast (Fig. 1) and the complexities of future inundation hazards in the region driven by earthquake and tsunami hazards. The aftermath of earthquake and tsunami hazards can cause substantial subsidence followed by inundation from tsunami waves. Evaluating such hazards requires a probabilistic analysis of future earthquake and tsunami hazards beyond this study.

    Also, we added two cities, Jersey City, NJ and Texas City, TX that were located near other selected cities (New York City, NY and Galveston, TX, respectively) and are also important urban centres in their respective regions.

    We use LiDAR DEM for the coastal-elevation data. The high-resolution LiDAR DEMs hosted by the National Oceanic and Atmospheric Administration (NOAA) Office for Coastal Management are available for the coastal USA71. In this study, we used a 3-m × 3-m grid resolution for the 32 cities, except Savannah (GA), Jacksonville (FL), Miami (FL) and all cities on the Pacific coast, which were obtained at a 5-m × 5-m grid resolution (Supplementary Table 23). All DEMs for each city use the North American Vertical Datum of 1988 (NAVD 88) vertical datum. Details on the implementation, vertical and horizontal accuracy, errors and temporal range are available with the data download71.

    Population, properties and racial demographic data

    We estimate the population and property datasets for each city using the Topologically Integrated Geographic Encoding and Referencing (TIGER) system demographic and economic data records available from the US Census Bureau (https://www.census.gov/geographies/mapping-files/time-series/geo/tiger-data.2010.html). The dataset provides population and property estimates for each city in the USA, subdivided into census blocks based on the 2010 census data. We used the 2010 dataset because it is the most recent census data available from the US Census Bureau. The racial demographic dataset is based on the decennial Census data (https://data.census.gov/cedsci/advanced) corresponding to the 2010 census. For this study, we selected eight races: ‘White’, ‘Black or African American’, ‘American Indian and Alaska Native’, ‘Asian’, ‘Native Hawaiian and Other Pacific Islander’, ‘Hispanic or Latino’ and others (‘Some Other Race’ alone and ‘Two or More Races’), as defined by the decennial data.

    Sea-level projections

    We use the localized sea-level projections from the IPCC Sixth Assessment Report17,34. The projections consider the contributions to future sea levels from sterodynamic effects (ocean steric and ocean dynamic effects), ice sheets (Antarctic and Greenland ice sheets), land water storage, glacier and ice cap surface mass balance, thermal expansion and the IPCC estimates of total VLM based on tide-gauge observations—reflecting the sum of GIA and other VLM processes. To prevent double counting of VLM, we acquired the SLR projections without the effect of VLM for our analysis (geocentric SLR). The database provides projections of sea level at tide-gauge stations worldwide under five SSP scenarios (SSP1-1.9, SSP1-2.6, SSP2-4.5, SSP3-7.0 and SSP5-8.5). SSP1-1.9 limits warming to 1.5 °C above 1850–1900 levels by 2100, implying net-zero CO2 emissions around the middle of the century. SSP1-2.6 keeps warming below 2.0 °C relative to 1850–1900, with projected net-zero emissions in the second half of the century. The SSP2-4.5 scenario projects best-estimate warming of approximately 2.7 °C by the end of the twenty-first century relative to 1850–1900. SSP3-7.0 is a medium to high reference scenario resulting from no further climate policy with particularly high non-CO2 and aerosol emissions and a warming of 2.8–4.6 °C. SSP5-8.5 is a high reference scenario with the highest emission levels (above the current emissions trajectory) and warming of 3.3–5.7 °C. In this study, we apply the 17th (lower bound), 50th (median) and 83rd (upper bound) percentile projections under SSP2-4.5, which represents the current emissions trajectory. Supplementary Table 24 summarizes the tide-gauge stations used for the SLR projections in each city.

    High-tide estimates

    We used MHW at tide gauges to estimate the high-tide events for each coastal city. The tide-gauge measurements were obtained from NOAA tide and currents data72, using the NAVD 88 datum, consistent with the elevation datum and mean measurement for the present epoch. Tide-gauge stations used for each city were selected on the basis of the proximity to the city, which provides localized data crucial for accurate evaluation of the current exposure to high tide in the urban areas (Supplementary Table 24).

    Inundation model

    Using a bathtub model2,51,73,74,75 (see Supplementary Fig. 4c), we projected the inundation hazards for 32 cities on the US coasts. The input data for the inundation model are as follows:

    1. 1.

      3-m or 5-m grid LiDAR DEM for each city.

    2. 2.

      About 50-m resolution VLM data for each city.

    3. 3.

      MHW levels at tide gauges adjacent to each city (Supplementary Table 24).

    4. 4.

      IPCC geocentric SLR projections at the stations adjacent to each city (Supplementary Table 24).

    To provide a comprehensive exposure assessment, we incorporate two temporal scales—the current (2020) and projected exposure (2050). First, the current exposure to high tide is assessed using MHW levels. Subsequently, projected exposure is evaluated by considering both VLM and geocentric SLR. Thus, the projected exposure represents further exposure, providing a baseline of current exposure against which future scenarios can be compared. To implement the inundation model, first, we resample the VLM rates on the LiDAR DEM. Next, we modify the elevation model to account for VLM projections, assuming a linear VLM rate from the base year of the DEM to the target years of 2020 and 2050 (refs. 34,48,51). Last, we evaluated the current (2020) scenario by subtracting the modified DEM height, which accounts for VLM projections up to the year 2020, from MHW levels (equation (3)). Subsequently, for the 2050 scenario, we apply SLR projections by subtracting the modified DEM height, updated for VLM projections to the year 2050, from both the geocentric SLR projection height and the MHW levels (equation (3)). Areas with a projected height below zero are inundated. This simplified static model is useful for local-scale simulations of inundated locations hydrologically connected to the coast74. However, it may overestimate or underestimate inundated areas on the coast owing to the reduced complexity of the model74. To reduce the errors associated with this approach, we implemented connected-component analysis to remove solitary grid cells from the inundation model, which represents topographically isolated low regions. Furthermore, we first present our inundation model as an undefended inundation map that does not account for the presence of levees or sea walls and we introduce and discuss the possible implications of flood-control structures on the impacts of relative SLR. For the defended scenario, we account for existing levees and sea walls by modifying the DEM height at the location of flood-control structures above the threshold for potential flooding.

    To account for all error sources in the input data, we consider the uncertainties in the DEM, VLM and SLR datasets. Specifically, we propagate the 17th and 83rd percentiles for geocentric SLR projections, ±1 standard deviation for VLM and errors inherent in the DEM (equation (3)). These measures provide an error bound for the inundation analysis, ensuring robust estimation of the uncertainties associated with the projections.

    $$\begin{array}{l}{{\rm{Inun}}}_{{\rm{med}}}={{\rm{DEM}}}_{{\rm{mod}}}-({{\rm{SLR}}}_{50}+{\rm{MHW}})\\ {{\rm{Inun}}}_{{\rm{low}},{\rm{up}}}={{\rm{Inun}}}_{{\rm{med}}}\pm (\sqrt{{{\rm{DEM}}}_{{\rm{err}}}^{2}+{((t-{t}_{0}){{\rm{VLM}}}_{{\rm{SD}}})}^{2}+{(({{\rm{SLR}}}_{83}-{{\rm{SLR}}}_{17})/2)}^{2}})\end{array}$$

    (3)

    in which Inunlow, Inunmed and Inunup represent the median, lower and upper bounds, respectively, for the inundation models. DEMmod is the modified DEM height, updated using the VLM projections. DEMerr is the vertical accuracy of the DEM. t represents the projection target years of 2020 or 2050. t0 represents the base year of the DEM. VLMSD is one standard deviation from the VLM data. MHW represents mean high water. SLR17, SLR50 and SLR83 represent the 17th, 50th and 83rd percentiles, respectively, from the geocentric SLR projections. Note that, for evaluating the current/baseline scenario (2020), SLR17, SLR50 and SLR83 are zero.

    Socioeconomic exposure analysis

    We used the TIGER demographic and economic data to assess the population and property exposure, which estimates the total population and properties subdivided into census blocks. We consider a census block inundated if greater than 20% of its area is inundated and assign the population and property for that block as exposed population or properties. To select the 20% threshold for the exposure of each census block, we conducted an empirical analysis across six representative cities. The distribution of exposed areas within these census blocks followed an extreme-value distribution. Statistical metrics revealed a median value of exposed area ranging from 18% to 23% for the six cities (Supplementary Fig. 6). Furthermore, the distribution exhibited a sharp decline beyond 10% (Supplementary Fig. 6). Therefore, a 20% criterion was established as a suitable threshold for quantifying the exposed population and properties. To quantify the home-value exposure, we used the ZIP Code ZHVI as a metric for housing cost. The estimated home-value exposure was calculated by multiplying the number of exposed properties within each city by the corresponding ZHVI (https://www.zillow.com/research/data/). We adjusted the ZHVI for the recent economic inflation using the mid-2021 housing price. The Zillow home-value data for each ZIP code used in this study is reported in Supplementary Table 25.

    To investigate the disparate sociodemographic and socioeconomic impacts of relative SLR on vulnerable groups, we focused on analysing both racial and economic disparities in the exposed communities. To examine the racial disparities in the exposed communities, we considered eight races as defined by the US census decennial data: ‘White’, ‘Black or African American’, ‘American Indian and Alaska Native’, ‘Asian’, ‘Native Hawaiian and Other Pacific Islander’, ‘Hispanic or Latino’, ‘Some Other Race’ alone and ‘Two or More Races’. Racial minoritized groups are defined as individuals identifying as Black or African American; American Indian or Alaska Native; Asian; Native Hawaiian or Other Pacific Islander; Hispanic or Latino; and two or more groups38. The analysis shows an overrepresentation of the white population on the Atlantic and Pacific coasts, whereas minoritized populations are overrepresented on the Gulf coast. On the Atlantic coast, the white population makes up 55.1–71.4% of the exposed population by 2050, which is higher than their 38.3% share in the total population (Extended Data Fig. 7 and Supplementary Table 13). Minoritized groups make up 43.0% of the total population on the Gulf coast while accounting for 64.2–71.5% of the exposed population by 2050 (Extended Data Fig. 7 and Supplementary Table 14). On the Pacific coast, white residents comprise 57.6–70.9% of the exposed population by 2050, despite making up only 41.8% of the total population (Extended Data Fig. 7 and Supplementary Table 15). In cities such as Jersey City, New Orleans, Port Arthur and Oakland, minority groups are disproportionately represented among the exposed population (Supplementary Tables 13–15).

    To assess the impacts of relative SLR on economic inequality, we used the property value as a proxy for economic status. Using a Kolmogorov–Smirnov statistical method, we compare the median home values in regions exposed to relative SLR by 2050 against those in each city, using an alpha value of 0.05 for statistical significance. Supplementary Tables 16–18 summarize the statistical test for the 32 cities. Note that 9–22 cities (considering lower to upper bound relative SLR projections) were excluded from the analysis because of limitations imposed by the central limit theorem. Across the 14 cities examined (considering median relative SLR projection), we find statistically significant economic disparities in 12 cities (Extended Data Fig. 8). In eight of these cities, we find that the median home value for the exposed population is higher than the total home value in the cities (that is, exposed properties are overvalued). However, in Atlantic City, New Orleans, Port Arthur and Foster City, we find that the median exposed-home values are lower than the overall median home value within the cities, highlighting their disproportionate economic exposure.

    Subsidence hazard exposure analysis for levees

    The polygon features for the levees across the US coasts were obtained from the United States Army Corps of Engineers (USACE)76. To determine the exposure to subsidence for the levees, we extracted the VLM rate for each point along the polygon feature. The subsidence exposure for levees in five cities (Miami, FL; New Orleans, LA; Port Arthur, TX; Freeport, TX; and Foster City, CA) are shown in Extended Data Fig. 9.

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  • Huge deposit of natural hydrogen gas detected deep in Albanian mine

    Huge deposit of natural hydrogen gas detected deep in Albanian mine

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    The team of scientists exploring the mine galleries

    An Albanian mine where hydrogen naturally seeps up through the rock

    F-V. Donzé

    The largest flow of natural hydrogen gas ever recorded has been measured deep in an Albanian mine. The find could help us work out where to locate underground deposits of this clean fuel.

    “The bubbling is really, really intense,” says Laurent Truche at the University of Grenoble Alpes in France, who measured the gas in a pool of water nearly a kilometre underground. “It’s like a Jacuzzi.”

    Companies are now searching for deposits of natural hydrogen all over the world as a source of clean fuel, but evidence for large accumulations of this “gold hydrogen” is sparse. Most claims about vast hydrogen deposits beneath the surface rely on extrapolation, rather than direct measurements.

    In search of more substantial proof, Truche and his colleagues descended into the Bulqizë chromite mine in Albania, where hydrogen gas seeping out of the rocks has caused several explosions. The mine is also located within an exposure of iron-rich rock, known as an ophiolite. Water is known to react with such rock to generate hydrogen in other places, such as Oman.

    The researchers found that the gas bubbling from the pool was more than 80 per cent hydrogen, with methane and a small amount of nitrogen mixed in. It was flowing at a rate of 11 tonnes per year, almost an order of magnitude greater than any other flows of hydrogen gas measured from single-point sources elsewhere on Earth’s surface.

    To determine the source of the gas, the researchers also modelled different geological scenarios that could produce such a flow. They found the most likely scenario was that the gas was coming from a deeper reservoir of hydrogen accumulated in a fault beneath the mine. Based on the geometry of the fault, they estimate this reservoir contains at least 5000 to 50,000 tonnes of hydrogen.

    “It’s one of the largest volumes of natural hydrogen that has ever been measured,” says Eric Gaucher, an independent geochemist focused on natural hydrogen.

    But it still isn’t a huge amount, says Geoffrey Ellis at the US Geological Survey. However, evidence for a stable accumulation of hydrogen supports the notion that much more is stored underground, he says. “We really should be looking deeper.”

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