Slow slip events (SSEs) have been observed in spatial and temporal proximity to megathrust earthquakes in various subduction zones, including the 2014 Mw 7.3 Guerrero, Mexico earthquake which was preceded by a Mw 7.6 SSE. However, the underlying physics connecting SSEs to earthquakes remains elusive. Here, we link 3D slow-slip cycle models with dynamic rupture simulations across the geometrically complex flat-slab Cocos plate boundary. Our physics-based models reproduce key regional geodetic and teleseismic fault slip observations on timescales from decades to seconds. We find that accelerating SSE fronts transiently increase shear stress at the down-dip end of the seismogenic zone, modulated by the complex geometry beneath the Guerrero segment. The shear stresses cast by the migrating fronts of the 2014 Mw 7.6 SSE are significantly larger than those during the three previous episodic SSEs that occurred along the same portion of the megathrust. We show that the SSE transient stresses are large enough to nucleate earthquake dynamic rupture and affect rupture dynamics. However, additional frictional asperities in the seismogenic part of the megathrust are required to explain the observed complexities in the coseismic energy release and static surface displacements of the Guerrero earthquake. We conclude that it is crucial to jointly analyze the long- and short-term interactions and complexities of SSEs and megathrust earthquakes across several (a)seismic cycles accounting for megathrust geometry. Our study has important implications for identifying earthquake precursors and understanding the link between transient and sudden megathrust faulting processes.
{"title":"Linking 3D Long-Term Slow-Slip Cycle Models With Rupture Dynamics: The Nucleation of the 2014 Mw 7.3 Guerrero, Mexico Earthquake","authors":"Duo Li, Alice-Agnes Gabriel","doi":"10.1029/2023AV000979","DOIUrl":"https://doi.org/10.1029/2023AV000979","url":null,"abstract":"<p>Slow slip events (SSEs) have been observed in spatial and temporal proximity to megathrust earthquakes in various subduction zones, including the 2014 <i>M</i><sub>w</sub> 7.3 Guerrero, Mexico earthquake which was preceded by a <i>M</i><sub>w</sub> 7.6 SSE. However, the underlying physics connecting SSEs to earthquakes remains elusive. Here, we link 3D slow-slip cycle models with dynamic rupture simulations across the geometrically complex flat-slab Cocos plate boundary. Our physics-based models reproduce key regional geodetic and teleseismic fault slip observations on timescales from decades to seconds. We find that accelerating SSE fronts transiently increase shear stress at the down-dip end of the seismogenic zone, modulated by the complex geometry beneath the Guerrero segment. The shear stresses cast by the migrating fronts of the 2014 <i>M</i><sub>w</sub> 7.6 SSE are significantly larger than those during the three previous episodic SSEs that occurred along the same portion of the megathrust. We show that the SSE transient stresses are large enough to nucleate earthquake dynamic rupture and affect rupture dynamics. However, additional frictional asperities in the seismogenic part of the megathrust are required to explain the observed complexities in the coseismic energy release and static surface displacements of the Guerrero earthquake. We conclude that it is crucial to jointly analyze the long- and short-term interactions and complexities of SSEs and megathrust earthquakes across several (a)seismic cycles accounting for megathrust geometry. Our study has important implications for identifying earthquake precursors and understanding the link between transient and sudden megathrust faulting processes.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-03-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV000979","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140331162","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Natan Holtzman, Brandon Sloan, Aaron Potkay, Gabriel Katul, Xue Feng, Alexandra G. Konings
Stomatal optimization theory is a commonly used framework for modeling how plants regulate transpiration in response to the environment. Most stomatal optimization models assume that plants instantaneously optimize a reward function such as carbon gain. However, plants are expected to optimize over longer timescales given the rapid environmental variability they encounter. There are currently no observational constraints on these timescales. Here, a new stomatal model is developed and is used to analyze the timescales over which stomatal closure is optimized. The proposed model assumes plants maximize carbon gain subject to the constraint that they cannot draw down soil moisture below a critical value. The reward is integrated over time, after being weighted by a discount factor that represents the timescale (τ) that a plant considers when optimizing stomatal conductance to save water. The model is simple enough to be analytically solvable, which allows the value of τ to be inferred from observations of stomatal behavior under known environmental conditions. The model is fitted to eddy covariance data in a range of ecosystems, finding the value of τ that best predicts the dynamics of evapotranspiration at each site. Across 82 sites, the climate metrics with the strongest correlation to τ are measures of the average number of dry days between rainfall events. Values of τ are similar in magnitude to the longest such dry period encountered in an average year. The results here shed light on which climate characteristics shape spatial variations in ecosystem-level water use strategy.
{"title":"Ecosystem Water-Saving Timescale Varies Spatially With Typical Drydown Length","authors":"Natan Holtzman, Brandon Sloan, Aaron Potkay, Gabriel Katul, Xue Feng, Alexandra G. Konings","doi":"10.1029/2023AV001113","DOIUrl":"https://doi.org/10.1029/2023AV001113","url":null,"abstract":"<p>Stomatal optimization theory is a commonly used framework for modeling how plants regulate transpiration in response to the environment. Most stomatal optimization models assume that plants <i>instantaneously</i> optimize a reward function such as carbon gain. However, plants are expected to optimize over longer timescales given the rapid environmental variability they encounter. There are currently no observational constraints on these timescales. Here, a new stomatal model is developed and is used to analyze the timescales over which stomatal closure is optimized. The proposed model assumes plants maximize carbon gain subject to the constraint that they cannot draw down soil moisture below a critical value. The reward is integrated over time, after being weighted by a discount factor that represents the timescale (<i>τ</i>) that a plant considers when optimizing stomatal conductance to save water. The model is simple enough to be analytically solvable, which allows the value of <i>τ</i> to be inferred from observations of stomatal behavior under known environmental conditions. The model is fitted to eddy covariance data in a range of ecosystems, finding the value of <i>τ</i> that best predicts the dynamics of evapotranspiration at each site. Across 82 sites, the climate metrics with the strongest correlation to <i>τ</i> are measures of the average number of dry days between rainfall events. Values of <i>τ</i> are similar in magnitude to the longest such dry period encountered in an average year. The results here shed light on which climate characteristics shape spatial variations in ecosystem-level water use strategy.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-03-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV001113","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140329047","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Jing Liu-Zeng, Zhijun Liu, Xiaoli Liu, Chris Milliner, Alba M. Rodriguez Padilla, Shiqing Xu, Jean-Philippe Avouac, Wenqian Yao, Yann Klinger, Longfei Han, Yanxiu Shao, Xiaodong Yan, Saif Aati, Zhigang Shao
Fault maturity has been proposed to exert a first order control on earthquake rupture, yet direct observations linking individual rupture to long-term fault growth are rare. The 2021 Mw 7.4 Maduo earthquake ruptured the east-growing end of the slow-moving (∼1 mm/yr) Jiangcuo fault in north Tibet, providing an opportunity to examine the relation between rupture characteristics and fault structure. Here we combine field and multiple remote sensing techniques to map the surface rupture at cm-resolution and document comprehensively on-fault offsets and off-fault deformation. The 158 km-long surface rupture consists of misoriented structurally inherited N110°-striking segments and younger optimally oriented N093°-striking segments, relative to the regional stress field. Despite being comparatively newly formed, the ∼N093°-striking fault segments accommodate more localized strain, with up to 3 m on-fault left-lateral slip and 25%–50% off-fault deformation, and possibly faster rupture speed. These results are in contrast with previous findings showing more localized strain and faster rupture speed on more mature fault segments; instead, our observations suggest that fault orientation with respect to the regional stress can exert a more important control than fault maturity on coseismic rupture behavior when both factors are at play.
{"title":"Fault Orientation Trumps Fault Maturity in Controlling Coseismic Rupture Characteristics of the 2021 Maduo Earthquake","authors":"Jing Liu-Zeng, Zhijun Liu, Xiaoli Liu, Chris Milliner, Alba M. Rodriguez Padilla, Shiqing Xu, Jean-Philippe Avouac, Wenqian Yao, Yann Klinger, Longfei Han, Yanxiu Shao, Xiaodong Yan, Saif Aati, Zhigang Shao","doi":"10.1029/2023AV001134","DOIUrl":"https://doi.org/10.1029/2023AV001134","url":null,"abstract":"<p>Fault maturity has been proposed to exert a first order control on earthquake rupture, yet direct observations linking individual rupture to long-term fault growth are rare. The 2021 Mw 7.4 Maduo earthquake ruptured the east-growing end of the slow-moving (∼1 mm/yr) Jiangcuo fault in north Tibet, providing an opportunity to examine the relation between rupture characteristics and fault structure. Here we combine field and multiple remote sensing techniques to map the surface rupture at cm-resolution and document comprehensively on-fault offsets and off-fault deformation. The 158 km-long surface rupture consists of misoriented structurally inherited N110°-striking segments and younger optimally oriented N093°-striking segments, relative to the regional stress field. Despite being comparatively newly formed, the ∼N093°-striking fault segments accommodate more localized strain, with up to 3 m on-fault left-lateral slip and 25%–50% off-fault deformation, and possibly faster rupture speed. These results are in contrast with previous findings showing more localized strain and faster rupture speed on more mature fault segments; instead, our observations suggest that fault orientation with respect to the regional stress can exert a more important control than fault maturity on coseismic rupture behavior when both factors are at play.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-03-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV001134","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140321809","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
P. A. Delamere, R. J. Wilson, S. Wing, A. R. Smith, B. Mino, C. Spitler, P. Damiano, K. Sorathia, A. Sciola, J. Caggiano, J. R. Johnson, X. Ma, F. Bagenal, B. Zhang, F. Allegrini, R. Ebert, G. Clark, O. Brambles
Jupiter's magnetosphere exhibits notable distinctions from the terrestrial magnetosphere. The structure and dynamics of Jupiter's dawnside magnetosphere can be characterized as a competition between internally driven sunward flow and solar wind-driven tailward flow. During the prime mission, Juno acquired extensive data from dawn to midnight, sampling the magnetodisc and higher latitude regions. Numerical moments from the Jovian Auroral Distributions Experiment (JADE-I) plasma (ion) instrument revealed a mid-latitude region of anticorotational (−vϕ) flow. While the magnitude of the flow is subject to uncertainty due to low count rates in these rarefied regions, we demonstrate in the raw JADE-I data that the sign of vϕ is a robust measurement. Global Grid Agnostic Magnetohydrodyamics for Extended Research Applications simulations show a similar region of strongly reduced flow in proximity to open field lines. Additionally, we use Jupiter Energetic-particle Detector Instrument integral moments to determine the Hen+/H+ ratio (where n refers to He+ or He++) and show that a transition to solar wind-like composition occurs in the same region as the anticorotational flow. We conclude that the global simulations are consistent with the Juno data, where the simulations show a crescent of open magnetic flux that is bounded by the magnetodisc and a closed high-latitude polar region (nominally the polar cap), which is never observed in the terrestrial magnetosphere. The distinct distribution of open flux in Jupiter's dawnside magnetosphere suggests the significance of planetary rotation and may represent a characteristic feature of rotating giant magnetospheres for future exploration.
{"title":"Signatures of Open Magnetic Flux in Jupiter's Dawnside Magnetotail","authors":"P. A. Delamere, R. J. Wilson, S. Wing, A. R. Smith, B. Mino, C. Spitler, P. Damiano, K. Sorathia, A. Sciola, J. Caggiano, J. R. Johnson, X. Ma, F. Bagenal, B. Zhang, F. Allegrini, R. Ebert, G. Clark, O. Brambles","doi":"10.1029/2023AV001111","DOIUrl":"https://doi.org/10.1029/2023AV001111","url":null,"abstract":"<p>Jupiter's magnetosphere exhibits notable distinctions from the terrestrial magnetosphere. The structure and dynamics of Jupiter's dawnside magnetosphere can be characterized as a competition between internally driven sunward flow and solar wind-driven tailward flow. During the prime mission, Juno acquired extensive data from dawn to midnight, sampling the magnetodisc and higher latitude regions. Numerical moments from the Jovian Auroral Distributions Experiment (JADE-I) plasma (ion) instrument revealed a mid-latitude region of anticorotational (−<i>v</i><sub><i>ϕ</i></sub>) flow. While the magnitude of the flow is subject to uncertainty due to low count rates in these rarefied regions, we demonstrate in the raw JADE-I data that the sign of <i>v</i><sub><i>ϕ</i></sub> is a robust measurement. Global Grid Agnostic Magnetohydrodyamics for Extended Research Applications simulations show a similar region of strongly reduced flow in proximity to open field lines. Additionally, we use Jupiter Energetic-particle Detector Instrument integral moments to determine the He<sup><i>n</i>+</sup>/H<sup>+</sup> ratio (where <i>n</i> refers to He<sup>+</sup> or He<sup>++</sup>) and show that a transition to solar wind-like composition occurs in the same region as the anticorotational flow. We conclude that the global simulations are consistent with the Juno data, where the simulations show a crescent of open magnetic flux that is bounded by the magnetodisc and a closed high-latitude polar region (nominally the polar cap), which is never observed in the terrestrial magnetosphere. The distinct distribution of open flux in Jupiter's dawnside magnetosphere suggests the significance of planetary rotation and may represent a characteristic feature of rotating giant magnetospheres for future exploration.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-03-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV001111","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140192356","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
K. R. Miner, R. K. Braghiere, C. E. Miller, N. Schlegel, D. Schimel
Since 2007, the National Academy for Sciences Engineering and Medicine (NASEM) has recommended Earth Science research and investment priorities every 10 years. The Decadal Survey balances the continuation of essential climate variable time series against unmet measurement needs and new Earth Observations made possible by technological breakthroughs. The next survey (2027–2028, DS28) will be framed by a rapidly changing world, and it will be critical to anticipate the observational needs of the 2030s–2040s, a world increasingly dominated by climate extremes and a rapidly changing Earth system. Here, we highlight some of the changes that factor into a framework for the DS28.
{"title":"A Decadal Survey Without Analogs: Earth Observation Needs for a Warming World","authors":"K. R. Miner, R. K. Braghiere, C. E. Miller, N. Schlegel, D. Schimel","doi":"10.1029/2023AV001148","DOIUrl":"https://doi.org/10.1029/2023AV001148","url":null,"abstract":"<p>Since 2007, the National Academy for Sciences Engineering and Medicine (NASEM) has recommended Earth Science research and investment priorities every 10 years. The Decadal Survey balances the continuation of essential climate variable time series against unmet measurement needs and new Earth Observations made possible by technological breakthroughs. The next survey (2027–2028, DS28) will be framed by a rapidly changing world, and it will be critical to anticipate the observational needs of the 2030s–2040s, a world increasingly dominated by climate extremes and a rapidly changing Earth system. Here, we highlight some of the changes that factor into a framework for the DS28.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV001148","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140161434","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
H. Moftakhari, D. F. Muñoz, A. Akbari Asanjan, A. AghaKouchak, H. Moradkhani, D. A. Jay
Sea-level rise (SLR) increasingly threatens coastal communities around the world. However, not all coastal communities are equally threatened, and realistic estimation of hazard is difficult. Understanding SLR impacts on extreme sea level is challenging due to interactions between multiple tidal and non-tidal flood drivers. We here use global hourly tidal data to show how and why tides and surges interact with mean sea level (MSL) fluctuations. At most locations around the world, the amplitude of at least one tidal constituent and/or amplitude of non-tidal residual have changed in response to MSL variation over the past few decades. In 37% of studied locations, “Potential Maximum Storm Tide” (PMST), a proxy for extreme sea level dynamics, co-varies with MSL variations. Over all stations, the median PMST will be 20% larger by the mid-century, and conventional approaches that simply shift the current storm tide regime up at the rate of projected SLR may underestimate the flooding hazard at these locations by up to a factor of four. Micro- and meso-tidal systems and those with diurnal tidal regime are generally more susceptible to altered MSL than other categories. The nonlinear interactions of MSL and storm tide captured in PMST statistics contribute, along with projected SLR, to the estimated increase in flood hazard at three-fourth of studied locations by mid-21st century. PMST is a threshold that captures nonlinear interactions between extreme sea level components and their co-evolution over time. Thus, use of this statistic can help direct assessment and design of critical coastal infrastructure.
海平面上升日益威胁着世界各地的沿海社区。然而,并非所有沿海社区都受到同样的威胁,而且很难对灾害进行实际估算。由于多种潮汐和非潮汐洪水驱动因素之间的相互作用,了解 SLR 对极端海平面的影响具有挑战性。在此,我们使用全球每小时潮汐数据来说明潮汐和涌浪如何以及为何与平均海平面(MSL)波动相互作用。在过去几十年中,全球大多数地方至少有一种潮汐成分和/或非潮汐残余物的振幅随着 MSL 的变化而变化。在 37% 的研究地点,"潜在最大风暴潮"(PMST)--极端海平面动态的替代物--与 MSL 变化共同变化。在所有站点中,到本世纪中期,"潜在最大风暴潮 "的中位数将增加 20%,如果只是按照预测的可持续海平面上升速度将当前的风暴潮机制上移,那么传统方法可能会低估这些地点的洪水危害,最高可达四倍。与其他类别相比,微潮汐和中潮汐系统以及昼夜潮汐系统通常更容易受到 MSL 变化的影响。在 PMST 统计中捕捉到的 MSL 与风暴潮的非线性相互作用,加上预测的可持续土地变率,估计到 21 世纪中叶,四分之三研究地点的洪水灾害会增加。PMST 是一个阈值,可捕捉极端海平面成分之间的非线性相互作用及其随时间的共同演变。因此,使用该统计量有助于指导关键沿海基础设施的评估和设计。
{"title":"Nonlinear Interactions of Sea-Level Rise and Storm Tide Alter Extreme Coastal Water Levels: How and Why?","authors":"H. Moftakhari, D. F. Muñoz, A. Akbari Asanjan, A. AghaKouchak, H. Moradkhani, D. A. Jay","doi":"10.1029/2023AV000996","DOIUrl":"https://doi.org/10.1029/2023AV000996","url":null,"abstract":"<p>Sea-level rise (SLR) increasingly threatens coastal communities around the world. However, not all coastal communities are equally threatened, and realistic estimation of hazard is difficult. Understanding SLR impacts on extreme sea level is challenging due to interactions between multiple tidal and non-tidal flood drivers. We here use global hourly tidal data to show how and why tides and surges interact with mean sea level (MSL) fluctuations. At most locations around the world, the amplitude of at least one tidal constituent and/or amplitude of non-tidal residual have changed in response to MSL variation over the past few decades. In 37% of studied locations, “Potential Maximum Storm Tide” (PMST), a proxy for extreme sea level dynamics, co-varies with MSL variations. Over all stations, the median PMST will be 20% larger by the mid-century, and conventional approaches that simply shift the current storm tide regime up at the rate of projected SLR may underestimate the flooding hazard at these locations by up to a factor of four. Micro- and meso-tidal systems and those with diurnal tidal regime are generally more susceptible to altered MSL than other categories. The nonlinear interactions of MSL and storm tide captured in PMST statistics contribute, along with projected SLR, to the estimated increase in flood hazard at three-fourth of studied locations by mid-21st century. PMST is a threshold that captures nonlinear interactions between extreme sea level components and their co-evolution over time. Thus, use of this statistic can help direct assessment and design of critical coastal infrastructure.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV000996","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140145630","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Angus K. Moore, Kimberly Méndez Méndez, K. Stephen Hughes, Darryl E. Granger
Volcanic arcs are chemical weathering hotspots that may contribute disproportionately to global CO2 consumption through silicate weathering. Accurately modeling the impact of volcanic-arc landscapes on the Earth's long-term carbon cycle requires understanding how climate and physical erosion control weathering fluxes from arc landscapes. We evaluate these controls by examining the covariation of stream solutes, sediment geochemistry, and long-term physical erosion fluxes inferred from cosmogenic 36Cl in magnetite in volcanic watersheds in Puerto Rico that span a ca. 15-fold gradient in specific discharge. Analysis of this data using power-law relationships demonstrates that CO2 consumption from arc-rock weathering in the humid tropics is more strongly limited by physical erosion and the supply of primary minerals to the weathering zone than by temperature or the flux of fresh, chemically reactive waters through the critical zone. However, a positive correlation between long-term physical erosion fluxes and specific discharge is also observed. This indicates that fresh mineral supply in arc environments may ultimately depend on precipitation rates, which may maintain a coupling between arc-rock weathering fluxes and climate under principally supply limited weathering conditions.
{"title":"Volcanic Arc Weathering Rates in the Humid Tropics Controlled by the Interplay Between Physical Erosion and Precipitation","authors":"Angus K. Moore, Kimberly Méndez Méndez, K. Stephen Hughes, Darryl E. Granger","doi":"10.1029/2023AV001066","DOIUrl":"https://doi.org/10.1029/2023AV001066","url":null,"abstract":"<p>Volcanic arcs are chemical weathering hotspots that may contribute disproportionately to global CO<sub>2</sub> consumption through silicate weathering. Accurately modeling the impact of volcanic-arc landscapes on the Earth's long-term carbon cycle requires understanding how climate and physical erosion control weathering fluxes from arc landscapes. We evaluate these controls by examining the covariation of stream solutes, sediment geochemistry, and long-term physical erosion fluxes inferred from cosmogenic <sup>36</sup>Cl in magnetite in volcanic watersheds in Puerto Rico that span a ca. 15-fold gradient in specific discharge. Analysis of this data using power-law relationships demonstrates that CO<sub>2</sub> consumption from arc-rock weathering in the humid tropics is more strongly limited by physical erosion and the supply of primary minerals to the weathering zone than by temperature or the flux of fresh, chemically reactive waters through the critical zone. However, a positive correlation between long-term physical erosion fluxes and specific discharge is also observed. This indicates that fresh mineral supply in arc environments may ultimately depend on precipitation rates, which may maintain a coupling between arc-rock weathering fluxes and climate under principally supply limited weathering conditions.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-03-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV001066","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140053093","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Zheng Shi, Forrest M. Hoffman, Min Xu, Umakant Mishra, Steven D. Allison, Jizhong Zhou, James T. Randerson
Soil carbon (C) responses to environmental change represent a major source of uncertainty in the global C cycle. Feedbacks between soil C stocks and climate drivers could impact atmospheric CO2 levels, further altering the climate. Here, we assessed the reliability of Earth system model (ESM) predictions of soil C change using the Coupled Model Intercomparison Project phases 5 and 6 (CMIP5 and CMIP6). ESMs predicted global soil C gains under the high emission scenario, with soils taking up 43.9 Pg (95% CI: 9.2–78.5 Pg) C on average during the 21st century. The variation in global soil C change declined significantly from CMIP5 (with average of 48.4 Pg [95% CI: 2.0–94.9 Pg] C) to CMIP6 models (with average of 39.3 Pg [95% CI: 23.9–54.7 Pg] C). For some models, a small C increase in all biomes contributed to this convergence. For other models, offsetting responses between cold and warm biomes contributed to convergence. Although soil C predictions appeared to converge in CMIP6, the dominant processes driving soil C change at global or biome scales differed among models and in many cases between earlier and later versions of the same model. Random Forest models, for soil carbon dynamics, accounted for more than 63% variation of the global soil C change predicted by CMIP5 ESMs, but only 36% for CMIP6 models. Although most CMIP6 models apparently agree on increased soil C storage during the 21st century, this consensus obscures substantial model disagreement on the mechanisms underlying soil C response, calling into question the reliability of model predictions.
{"title":"Global-Scale Convergence Obscures Inconsistencies in Soil Carbon Change Predicted by Earth System Models","authors":"Zheng Shi, Forrest M. Hoffman, Min Xu, Umakant Mishra, Steven D. Allison, Jizhong Zhou, James T. Randerson","doi":"10.1029/2023AV001068","DOIUrl":"https://doi.org/10.1029/2023AV001068","url":null,"abstract":"<p>Soil carbon (C) responses to environmental change represent a major source of uncertainty in the global C cycle. Feedbacks between soil C stocks and climate drivers could impact atmospheric CO<sub>2</sub> levels, further altering the climate. Here, we assessed the reliability of Earth system model (ESM) predictions of soil C change using the Coupled Model Intercomparison Project phases 5 and 6 (CMIP5 and CMIP6). ESMs predicted global soil C gains under the high emission scenario, with soils taking up 43.9 Pg (95% CI: 9.2–78.5 Pg) C on average during the 21st century. The variation in global soil C change declined significantly from CMIP5 (with average of 48.4 Pg [95% CI: 2.0–94.9 Pg] C) to CMIP6 models (with average of 39.3 Pg [95% CI: 23.9–54.7 Pg] C). For some models, a small C increase in all biomes contributed to this convergence. For other models, offsetting responses between cold and warm biomes contributed to convergence. Although soil C predictions appeared to converge in CMIP6, the dominant processes driving soil C change at global or biome scales differed among models and in many cases between earlier and later versions of the same model. Random Forest models, for soil carbon dynamics, accounted for more than 63% variation of the global soil C change predicted by CMIP5 ESMs, but only 36% for CMIP6 models. Although most CMIP6 models apparently agree on increased soil C storage during the 21st century, this consensus obscures substantial model disagreement on the mechanisms underlying soil C response, calling into question the reliability of model predictions.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV001068","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140015114","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
<p>Ice shelves play an important role in controlling how fast ice moves off the Antarctic continent into the oceans, promoting sea-level rise. These floating bodies of ice effectively buttress the grounded ice behind them, hindering the flow of ice off land while also somewhat reducing the exposure of the grounding line to ocean melting (Gudmundsson, <span>2013</span>). Their importance can perhaps be exemplified by comparing Antarctic ice streams terminating at ice shelves to Greenland's directly exposed calving fronts (Benn et al., <span>2017</span>), where ice is currently being lost at a far greater rate (Oppenheimer et al., <span>2019</span>). However, Antarctic ice shelves are vulnerable to rifting (Larour et al., <span>2021</span>) and catastrophic breakup (Glasser & Scambos, <span>2008</span>). Olinger et al. (<span>2024</span>) use seismology to shed new light on how such rifting can be limited by ocean coupling.</p><p>Olinger et al. (<span>2024</span>) use observations combined with numerical modeling to highlight how vulnerable ice shelves can be to rifting, and in particular how the ocean can play a role in setting rifting velocity (see Figure 1). This work is particularly exciting for two reasons. First, they combine satellite and seismic observations with a numerical model, to not only understand but also quantify the rifting process. Second, they find that coupling of the ice shelf rift with the ocean actually limits the rate of rift propagation. This is contrary to the majority of ice shelf-ocean interactions, which generally act to exacerbate ice shelf instability (e.g., Holland et al. (<span>2008</span>)).</p><p>Satellite observations are one of the most effective means of observing ice shelf rifting. Olinger et al. (<span>2024</span>) use Synthetic Aperture Radar (SAR) imagery to map changes in the rift extent at Pine Island Glacier (PIG) ice shelf, before and after a major rifting event. However, one of the greatest challenges posed by such remote sensing data is the poor temporal sampling (Baumhoer et al., <span>2018</span>). This is evident in the data used by Olinger et al. (<span>2024</span>), where they analyze images six days apart, only capturing the rift extent prior to and post the major rifting episode. During this time, they find that the rift lengthens by 10.5 km. Capturing higher resolution temporal behavior of the rift is critical for understanding rifting in more detail. Olinger et al. (<span>2024</span>) use seismic observations from instruments deployed on the ice shelf to provide continuous temporal sampling of the rift. They searched through the continuous data to identify the dominant rifting event, which they assume accommodated the majority of rifting observed in the satellite data. From this rifting event, they observe an increase in seismic energy from surface waves of 300 s duration, which allows them to quantify a rifting velocity of 35 m s<sup>−1</sup>. Although this velocity may appear fast from
{"title":"Seismic Waves Used to Measure How Ice Shelf Rifting Velocity Is Limited by Ocean Coupling","authors":"T. Hudson","doi":"10.1029/2024AV001189","DOIUrl":"https://doi.org/10.1029/2024AV001189","url":null,"abstract":"<p>Ice shelves play an important role in controlling how fast ice moves off the Antarctic continent into the oceans, promoting sea-level rise. These floating bodies of ice effectively buttress the grounded ice behind them, hindering the flow of ice off land while also somewhat reducing the exposure of the grounding line to ocean melting (Gudmundsson, <span>2013</span>). Their importance can perhaps be exemplified by comparing Antarctic ice streams terminating at ice shelves to Greenland's directly exposed calving fronts (Benn et al., <span>2017</span>), where ice is currently being lost at a far greater rate (Oppenheimer et al., <span>2019</span>). However, Antarctic ice shelves are vulnerable to rifting (Larour et al., <span>2021</span>) and catastrophic breakup (Glasser & Scambos, <span>2008</span>). Olinger et al. (<span>2024</span>) use seismology to shed new light on how such rifting can be limited by ocean coupling.</p><p>Olinger et al. (<span>2024</span>) use observations combined with numerical modeling to highlight how vulnerable ice shelves can be to rifting, and in particular how the ocean can play a role in setting rifting velocity (see Figure 1). This work is particularly exciting for two reasons. First, they combine satellite and seismic observations with a numerical model, to not only understand but also quantify the rifting process. Second, they find that coupling of the ice shelf rift with the ocean actually limits the rate of rift propagation. This is contrary to the majority of ice shelf-ocean interactions, which generally act to exacerbate ice shelf instability (e.g., Holland et al. (<span>2008</span>)).</p><p>Satellite observations are one of the most effective means of observing ice shelf rifting. Olinger et al. (<span>2024</span>) use Synthetic Aperture Radar (SAR) imagery to map changes in the rift extent at Pine Island Glacier (PIG) ice shelf, before and after a major rifting event. However, one of the greatest challenges posed by such remote sensing data is the poor temporal sampling (Baumhoer et al., <span>2018</span>). This is evident in the data used by Olinger et al. (<span>2024</span>), where they analyze images six days apart, only capturing the rift extent prior to and post the major rifting episode. During this time, they find that the rift lengthens by 10.5 km. Capturing higher resolution temporal behavior of the rift is critical for understanding rifting in more detail. Olinger et al. (<span>2024</span>) use seismic observations from instruments deployed on the ice shelf to provide continuous temporal sampling of the rift. They searched through the continuous data to identify the dominant rifting event, which they assume accommodated the majority of rifting observed in the satellite data. From this rifting event, they observe an increase in seismic energy from surface waves of 300 s duration, which allows them to quantify a rifting velocity of 35 m s<sup>−1</sup>. Although this velocity may appear fast from","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-02-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2024AV001189","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139987434","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Steven. D. Dibb, Erik Asphaug, James F. Bell, Richard P. Binzel, William F. Bottke, Saverio Cambioni, John M. Christoph, Linda T. Elkins-Tanton, Ralf Jaumann, David J. Lawrence, Rona Oran, Joseph G. O’Rourke, Carol Polansky, Benjamin P. Weiss, Mark Wieczorek, David. A. Williams
Astronomical observations indicate that asteroid (16) Psyche is a large, high-density (likely >3,400 kg·m−3), metal-rich (30–55 vol. %) asteroid. Psyche may be remnant core material or it could be a primordial, undifferentiated metal-rich object. We discuss the science objectives of the upcoming Psyche mission, which will employ three instruments (the Magnetometer, Multispectral Imager, and Gamma-Ray and Neutron Spectrometer) and will use Doppler tracking of the spacecraft to explore the asteroid. This mission will shed light on the nature and origins of metal-rich objects in the solar system and beyond, including the cores of the terrestrial planets.
{"title":"A Post-Launch Summary of the Science of NASA's Psyche Mission","authors":"Steven. D. Dibb, Erik Asphaug, James F. Bell, Richard P. Binzel, William F. Bottke, Saverio Cambioni, John M. Christoph, Linda T. Elkins-Tanton, Ralf Jaumann, David J. Lawrence, Rona Oran, Joseph G. O’Rourke, Carol Polansky, Benjamin P. Weiss, Mark Wieczorek, David. A. Williams","doi":"10.1029/2023AV001077","DOIUrl":"https://doi.org/10.1029/2023AV001077","url":null,"abstract":"<p>Astronomical observations indicate that asteroid (16) Psyche is a large, high-density (likely >3,400 kg·m<sup>−3</sup>), metal-rich (30–55 vol. %) asteroid. Psyche may be remnant core material or it could be a primordial, undifferentiated metal-rich object. We discuss the science objectives of the upcoming Psyche mission, which will employ three instruments (the Magnetometer, Multispectral Imager, and Gamma-Ray and Neutron Spectrometer) and will use Doppler tracking of the spacecraft to explore the asteroid. This mission will shed light on the nature and origins of metal-rich objects in the solar system and beyond, including the cores of the terrestrial planets.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 2","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-02-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2023AV001077","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139976361","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}