Recent Global Sea Levels and Land Levels
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Eustatic Curve for the Middle Jurassic–Cretaceous Based on Russian Platform and Siberian Stratigraphy: Zonal Resolution1
Eustatic Curve for the Middle Jurassic–Cretaceous Based on Russian Platform and Siberian Stratigraphy: Zonal Resolution1 D. Sahagian,2 O. Pinous,2 A. Olferiev,3 and V. Zakharov4 ABSTRACT sediment gaps left by unconformities in the cen- tral part of the Russian platform with data from We have used the stratigraphy of the central part stratigraphic information from the more continu- of the Russian platform and surrounding regions to ous stratigraphy of the neighboring subsiding construct a calibrated eustatic curve for the regions, such as northern Siberia. Although these Bajocian through the Santonian. The study area is sections reflect subsidence, the time scale of vari- centrally located in the large Eurasian continental ations in subsidence rate is probably long relative craton, and was covered by shallow seas during to the duration of the stratigraphic gaps to be much of the Jurassic and Cretaceous. The geo- filled, so the subsidence rate can be calculated graphic setting was a very low-gradient ramp that and filtered from the stratigraphic data. We thus was repeatedly flooded and exposed. Analysis of have compiled a more complete eustatic curve stratal geometry of the region suggests tectonic sta- than would be possible on the basis of Russian bility throughout most of Mesozoic marine deposi- platform stratigraphy alone. tion. The paleogeography of the region led to Relative sea level curves were generated by back- extremely low rates of sediment influx. As a result, stripping stratigraphic data from well and outcrop accommodation potential was limited and is inter- sections distributed throughout the central part of preted to have been determined primarily by the Russian platform. -
Sam White the Real Little Ice Age Between C.1300 and C.1850 A.D
Journal of Interdisciplinary History, xliv:3 (Winter, 2014), 327–352. THE REAL LITTLE ICE AGE Sam White The Real Little Ice Age Between c.1300 and c.1850 a.d. the world became, on average, slightly but signiªcantly colder. The change varied over time and space, and its causes remain un- certain. Nevertheless, this cooling constitutes a meaningful climate event, with signiªcant historical consequences. Both the cooling trend and its effects on humans appear to have been particularly Downloaded from http://direct.mit.edu/jinh/article-pdf/44/3/327/1706251/jinh_a_00574.pdf by guest on 28 September 2021 acute from the late sixteenth to the late seventeenth century in much of the Northern Hemisphere. This article explains why climatologists and historians are conªdent that these changes occurred. On close examination, the objections raised in this issue of the journal by Kelly and Ó Gráda turn out to be entirely unfounded. The proxy data for early mod- ern global cooling (such as tree rings and ice cores) are robust, and written weather descriptions and observations of physical phenom- ena (such as glacial movements and river freezings) by and large of- fer independent conªrmation. Kelly and Ó Gráda’s proposed alter- native measures of climate and climate change suffer from serious ºaws. As we review the evidence and refute their criticisms, it will become clear just how solid the case for the Little Ice Age (lia) has become. the case for the little ice age The evidence for early modern global cooling comes, ªrst and foremost, from extensive research into physical proxies, including ice cores, tree rings, corals, and speleothems (stalagmites and stalactites). -
Sea Level and Global Ice Volumes from the Last Glacial Maximum to the Holocene
Sea level and global ice volumes from the Last Glacial Maximum to the Holocene Kurt Lambecka,b,1, Hélène Roubya,b, Anthony Purcella, Yiying Sunc, and Malcolm Sambridgea aResearch School of Earth Sciences, The Australian National University, Canberra, ACT 0200, Australia; bLaboratoire de Géologie de l’École Normale Supérieure, UMR 8538 du CNRS, 75231 Paris, France; and cDepartment of Earth Sciences, University of Hong Kong, Hong Kong, China This contribution is part of the special series of Inaugural Articles by members of the National Academy of Sciences elected in 2009. Contributed by Kurt Lambeck, September 12, 2014 (sent for review July 1, 2014; reviewed by Edouard Bard, Jerry X. Mitrovica, and Peter U. Clark) The major cause of sea-level change during ice ages is the exchange for the Holocene for which the direct measures of past sea level are of water between ice and ocean and the planet’s dynamic response relatively abundant, for example, exhibit differences both in phase to the changing surface load. Inversion of ∼1,000 observations for and in noise characteristics between the two data [compare, for the past 35,000 y from localities far from former ice margins has example, the Holocene parts of oxygen isotope records from the provided new constraints on the fluctuation of ice volume in this Pacific (9) and from two Red Sea cores (10)]. interval. Key results are: (i) a rapid final fall in global sea level of Past sea level is measured with respect to its present position ∼40 m in <2,000 y at the onset of the glacial maximum ∼30,000 y and contains information on both land movement and changes in before present (30 ka BP); (ii) a slow fall to −134 m from 29 to 21 ka ocean volume. -
Sea Level and Climate Introduction
Sea Level and Climate Introduction Global sea level and the Earth’s climate are closely linked. The Earth’s climate has warmed about 1°C (1.8°F) during the last 100 years. As the climate has warmed following the end of a recent cold period known as the “Little Ice Age” in the 19th century, sea level has been rising about 1 to 2 millimeters per year due to the reduction in volume of ice caps, ice fields, and mountain glaciers in addition to the thermal expansion of ocean water. If present trends continue, including an increase in global temperatures caused by increased greenhouse-gas emissions, many of the world’s mountain glaciers will disap- pear. For example, at the current rate of melting, most glaciers will be gone from Glacier National Park, Montana, by the middle of the next century (fig. 1). In Iceland, about 11 percent of the island is covered by glaciers (mostly ice caps). If warm- ing continues, Iceland’s glaciers will decrease by 40 percent by 2100 and virtually disappear by 2200. Most of the current global land ice mass is located in the Antarctic and Greenland ice sheets (table 1). Complete melt- ing of these ice sheets could lead to a sea-level rise of about 80 meters, whereas melting of all other glaciers could lead to a Figure 1. Grinnell Glacier in Glacier National Park, Montana; sea-level rise of only one-half meter. photograph by Carl H. Key, USGS, in 1981. The glacier has been retreating rapidly since the early 1900’s. -
Deglacial Permafrost Carbon Dynamics in MPI-ESM
Clim. Past Discuss., https://doi.org/10.5194/cp-2018-54 Manuscript under review for journal Clim. Past Discussion started: 6 June 2018 c Author(s) 2018. CC BY 4.0 License. Deglacial permafrost carbon dynamics in MPI-ESM Thomas Schneider von Deimling1,2, Thomas Kleinen1, Gustaf Hugelius3, Christian Knoblauch4, Christian Beer5, Victor Brovkin1 1Max Planck Institute for Meteorology, Bundesstr. 53, 20146 Hamburg, Germany 2 5 now at Alfred Wegener Institute Helmholtz Centre for Polar and Marine Research, 14473 Potsdam, Germany 3Department of Physical Geography and Bolin Climate Research Centre, Stockholm University, SE10693, Stockholm, Sweden 4Institute of Soil Science, Universität Hamburg, Allende-Platz 2, 20146 Hamburg, Germany 5Department of Environmetal Science and Analytical Chemistry and Bolin Centre for Climate Research, Stockholm 10 University, 10691 Stockholm, Sweden Correspondence to: Thomas Schneider von Deimling ([email protected]) Abstract We have developed a new module to calculate soil organic carbon (SOC) accumulation in perennially frozen ground in the 15 land surface model JSBACH. Running this offline version of MPI-ESM we have modelled permafrost carbon accumulation and release from the Last Glacial Maximum (LGM) to the Pre-industrial (PI). Our simulated near-surface PI permafrost extent of 16.9 Mio km2 is close to observational evidence. Glacial boundary conditions, especially ice sheet coverage, result in profoundly different spatial patterns of glacial permafrost extent. Deglacial warming leads to large-scale changes in soil temperatures, manifested in permafrost disappearance in southerly regions, and permafrost aggregation in formerly glaciated 20 grid cells. In contrast to the large spatial shift in simulated permafrost occurrence, we infer an only moderate increase of total LGM permafrost area (18.3 Mio km2) – together with pronounced changes in the depth of seasonal thaw. -
Hurricane Waves in the Ocean
WAVE-INDUCED SURGES DURING HURRICANE OPAL Chung-Sheng Wu*, Arthur A. Taylor, Jye Chen and Wilson A. Shaffer Meteorological Development Laboratory National Weather Service/NOAA, Silver Spring, Maryland 1. INTRODUCTION Hurricanes storm surges and waves at the coastline Holliday (1977) developed a simple formula relating the have been the cause of damages in the coastal zone. cyclone’s pressure drop to maximum sustained wind for On the U.S. Gulf Coast, for example, Hurricane Opal the Western Pacific. A more general form was (1995) made landfall near the time of low tide and proposed by Holland (1980). The merit of these models resulted in severe flooding by storm surges and waves. is that they are analytical models for the surface wind Storm surge can penetrate miles inland from the coast. profile in a hurricane. A similar formulation was applied Waves ride above the surge levels, causing wave runup to the wave model in the present work. The framework and mean water level set-up. These wave effects are of the hurricane wave model is described below. significant near the landfall area and are affected by the process that hurricane approaches the coastline. 2.1 HURRICANE WIND AND STORM SURGES During 1950-1977, hurricane wave models based on Holland (1980) employed a standard pressure profile for significant wave height and period were developed (e.g. a tropical cyclone and obtained the popular gradient Bretschneider, 1957; Ross, 1976) for marine weather wind profile. Jelesnianski and Taylor (1976) assumed a prediction and offshore oil industry design. Cardone surface wind profile in the pressure equation. -
The Antarctic Contribution to Holocene Global Sea Level Rise
The Antarctic contribution to Holocene global sea level rise Olafur Ing6lfsson & Christian Hjort The Holocene glacial and climatic development in Antarctica differed considerably from that in the Northern Hemisphere. Initial deglaciation of inner shelf and adjacent land areas in Antarctica dates back to between 10-8 Kya, when most Northern Hemisphere ice sheets had already disappeared or diminished considerably. The continued deglaciation of currently ice-free land in Antarctica occurred gradually between ca. 8-5 Kya. A large southern portion of the marine-based Ross Ice Sheet disintegrated during this late deglaciation phase. Some currently ice-free areas were deglaciated as late as 3 Kya. Between 8-5 Kya, global glacio-eustatically driven sea level rose by 10-17 m, with 4-8 m of this increase occurring after 7 Kya. Since the Northern Hemisphere ice sheets had practically disappeared by 8-7 Kya, we suggest that Antarctic deglaciation caused a considerable part of the global sea level rise between 8-7 Kya, and most of it between 7-5 Kya. The global mid-Holocene sea level high stand, broadly dated to between 84Kya, and the Littorina-Tapes transgressions in Scandinavia and simultaneous transgressions recorded from sites e.g. in Svalbard and Greenland, dated to 7-5 Kya, probably reflect input of meltwater from the Antarctic deglaciation. 0. Ingcilfsson, Gotlienburg Universiw, Earth Sciences Centre. Box 460, SE-405 30 Goteborg, Sweden; C. Hjort, Dept. of Quaternary Geology, Lund University, Sdvegatan 13, SE-223 62 Lund, Sweden. Introduction dated to 20-17 Kya (thousands of years before present) in the western Ross Sea area (Stuiver et al. -
Chart Datum and Bathymetry Correction to Support Managing Coral Grouper in Lepar and Pongok Island Waters, South Bangka Regency
ILMU KELAUTAN Desember 2018 Vol 23(4):179-186 ISSN 0853-7291 Chart Datum and Bathymetry Correction to Support Managing Coral Grouper in Lepar and Pongok Island Waters, South Bangka Regency Sudirman Adibrata1,2*, Fredinan Yulianda3, Mennofatria Boer3, and I Wayan Nurjaya4 1Program of Coastal and Marine Resource Management, Bogor Agricultural University Jl. Agatis Campus IPB Darmaga Bogor 16680, Indonesia 2Program of Aquatic Resource Management, Faculty Agriculture, Fishery and Biology, Bangka Belitung Unversity Jl. Balunijuk Merawang District, Bangka, Bangka Belitung, Indonesia 3Department of Aquatic Resource Management, Fisheries and Marine Science Faculty, Bogor Agricultural University; Jl. Agatis Campus IPB Darmaga Bogor 16680, Indonesia 4Department of Marine Science and Technology, Fisheries and Marine Science, Bogor Agricultural University, Jl. Agatis Campus IPB Darmaga Bogor 16680, Indonesia Email: [email protected] Abstract Corrected bathimetry data is highly required to improve the quality of sea floor map, for a range of purposes including coastal environmental monitoring and management. This research was aimed to know chart datum values used for correctting bathymetry data at Bar-cheeked coral trout grouper (Plectropomus maculates) fishing ground in Lepar and Pongok Island waters 02o57’00”S and 106o50’00”E and 02o53’00”S and 107o03’00”E, respectively, South Bangka Regency, Indonesia. The study was carried out from November 2016 to October 2017, tidal data used for 15 days from September 16–30, 2017 using simple random sampling technique with the total of 845 points of measurements. To calculate tyde harmonic constituents values this study employed admiralty method resulting 10 major components. Results of this research indicated that harmonic coefficient values of M2, M2, S2, N2, K1, O1, M4, MS4, K2, and P1, were 0.0345 m, 0.0608 m, 0.0276 m, 0.4262 m, 0.2060 m, 0.0119 m, 0.0082 m, 0.0164 m, and 0.1406 m, respectively. -
Coastal Tide Gauge Tsunami Warning Centers
Products and Services Available from NOAA NCEI Archive of Water Level Data Aaron Sweeney,1,2 George Mungov, 1,2 Lindsey Wright 1,2 Introduction NCEI’s Role More than just an archive. NCEI: NOAA's National Centers for Environmental Information (NCEI) operates the World Data Service (WDS) for High resolution delayed-mode DART data are stored onboard the BPR, • Quality controls the data and Geophysics (including tsunamis). The NCEI/WDS provides the long-term archive, data management, and and, after recovery, are sent to NCEI for archive and processing. Tide models the tides to isolate the access to national and global tsunami data for research and mitigation of tsunami hazards. Archive gauge data is delivered to NCEI tsunami waves responsibilities include the global historic tsunami event and run-up database, the bottom pressure recorder directly through NOS CO-OPS and • Ensures meaningful data collected by the Deep-ocean Assessment and Reporting of Tsunami (DART®) Program, coastal tide gauge Tsunami Warning Centers. Upon documentation for data re-use data (analog and digital marigrams) from US-operated sites, and event-specific data from international receipt, NCEI’s role is to ensure • Creates standard metadata to gauges. These high-resolution data are used by national warning centers and researchers to increase our the data are available for use and enable search and discovery understanding and ability to forecast the magnitude, direction, and speed of tsunami events. reuse by the community. • Converts data into standard formats (netCDF) to ease data re-use The Data • Digitizes marigrams Data essential for tsunami detection and warning from • Adds data to inventory timeline the Deep-ocean Assessment and Reporting of to ensure no gaps in data Tsunamis (DART®) stations and the coastal tide gauges. -
SC1 Some Comments on 'Bardsey – an Island in a Strong Tidal Stream
SC1 Some comments on ’Bardsey – an island in a strong tidal stream Underestimating coastal tides due to unresolved topography’ by Green and Pugh I am not the topical editor or one of the reviewers for this paper, but I gave it a read and have some detailed comments that I hope are useful. I thought it was an interesting paper but the text is not very good and there are many minor problems, especially in the first half. I list these below. I will leave the official reviewers to comment more on the science. 19, 21, 24, 25 and many other places in the text - there are often mentions of ’altimeter data’ or ’altimetry database’ but the authors do not use that but instead use the outputs of a hydrodynamic tide model (TPXO9) in which altimeter data (and possibly tide gauge data) have been assimilated. There is a difference between these things and ’altimeter data’ is a complete misnomer. On the other hand, sometimes the language is correct e.g. line 18 ’altimetry constrained product’. Fine. - Corrected to “altimetry constrained product” or, more specifically, “TPXO9” throughout. Also everyone knows that altimetry has a coarse spatial (and temporal) sampling and provides elevations and not currents. But on line 14 we read about tidal streams and next line says they will be unresolved by altimetry. Well, yes, of course they will, whatever the spatial resolution. - This sentence (on line 19) has been rewritten: “…and that even in this latest [TPXO9] altimetry constrained product the derived tidal stream is seriously under-represented due to the island not being resolved.” So I think the text has to be gone through and the misleading language corrected. -
Deglaciation of Central Long Island
159 FIELD TRIP I: DEGLACIATION OF CENTRAL LON(; ISLAND· Les Sirkin Earth Science Adelphi University Garden City, NY 11530 This trip covers the geology of a south to north transect through the sequence oflate Wisconsinan glacial deposits--the· Terminal Moraine, Recessional Moraines, Outwash Plains, Proglacial Lakes and a Prominent Meltwater Channel-- in central Long Island. The Connetquot Rivers which drains southcentral Long Island from north to south, and the Nissequogue River, which flows through northcentral Long Island from south to north, have nearly coalescing drainage basins in central Long Island (Figure 1. The route crosses, from south to north, the USGS 7.5' Quadrangle Maps: Bay Shore East, Central Islip and Saint James). These two underfit rivers together appear to cinch the waist of Long Island and reveal an intriguing stream valley system that originated as a late glacial meltwater channel draining a series of proglaciallakes north of the terminal moraine, flowing through a gap in the moraine and across the outwash plain and continental shelf. The trip straddles the arbitrary geographic boundary between eastern and western Long Island. Geologically, it is situated east of the late Wisconsinan Interlobate Zone between the Hudson and Connecticut glacial lobes in the vicinity of Huntington. The Interlobate Zone resulted in the complex ofinterlobate morainal deposits, meltwater channel gravels and proglaciallake beds that make up the north-south range of hills: Manetto Hills, Half Hollow Hills and Dix Hills. The route of the field trip lines up roughly with the axis of the last interlobate angle between the receding glacial lobes and trends northward toward the interlobate angle formed at the inferred junction of the Sands Point Moraine of the Hudson Lobe and the Roanoke Point Moraine of the Connecticut Lobe projected beneath Smithtown Bay. -
Geophysical Abstracts 156-159 January-December 1954
Geophysical Abstracts 156-159 January-December 1954 GEOLOGICAL SURVEY BULLETIN 1022 Abstracts of current literature pertaining to the physics of the solid earth and geophysicq,l exploration UNITED STATES GOVERNMENT PRINTING OFFICE, WASHINGTON : 1955 UNITED STATESlDEPARTMENT OF THE INTERIOR Douglas McKay, Secretary GEOLOGICAL SURVEY W. ~· Wrather, Director CONTENTS [The letters in parentheses are those used to designate the chapters for separate publication] Page (A) Geophysical Abstracts 156, January-March------------------------ 1 (B) Geophysical Abstracts 157, April-June---------------------------- 71 (C) Geophysical Abstracts 158, July-September________________________ 135 (D) Geophysical Abstracts 159, October-December_____________________ 205 Under department orders, Geophysical Abstracts have been published at different times by the Bureau of Mines or the Geological Survey as noted below: 1-86, May 1929-June· 1936, Bureau of Mines Information Circulars. [Mimeo- graphed] 87, July-December 1936, Geological Survey Bulletin 887. 88-91, January-December 1937, Geological Survey Bulletin 895. 92-95, January-December 1938, Geological Survey Bulletin 909. 96-99, January-December 1939, Geological Survey Bulletin 915. 100-103, January-December 1940, Geological Survey Bulletin 925. 104-107, January-December 1941, Geological Survey Bulletin 932. 108-111, January-December 1942, Geological Survey Bulletin 939. 112-127, January 1943-December 1946, Bureau of Mines Information Circulars. [Mimeographed] 128-131, January-December 1947, Geological Survey Bulletin 957. 132-135, January-December 1948, Geological Survey Bulletin 959. 136-139, January-December 1949, Geological Survey Bulletin 966. 140-143, January-December 1950, Geological Survey Bulletin 976. 144-147, January-December 1951, Geological Survey Bulletin 981. 148-151, January-December 1952, Geological Survey Bulletin 991. 152-155, January-December 1953, Geological Survey Bulletin 1002.