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[转载]英文维基百科:环境同位素(environmental isotopes)

已有 617 次阅读 2024-1-29 15:49 |系统分类:科普集锦|文章来源:转载

From Wikipedia, the free encyclopedia

The environmental isotopes are a subset of isotopes, both stable and radioactive, which are the object of isotope geochemistry. They are primarily used as tracers to see how things move around within the ocean-atmosphere system, within terrestrial biomes, within the Earth's surface, and between these broad domains.

环境同位素是同位素地球化学的研究对象的一个子集,包括稳定同位素和放射性同位素。它们主要被用作示踪剂,以了解物质在海洋大气系统、陆地生物群落、地球表面以及这些广泛领域之间的运动方式。

Isotope geochemistry[edit]

Chemical elements are defined by their number of protons, but the mass of the atom is determined by the number of protons and neutrons in the nucleus. Isotopes are atoms that are of a specific element, but have different numbers of neutrons and thus different mass numbers. The ratio between isotopes of an element varies slightly in the world, so in order to study isotopic ratio changes across the world, changes in isotope ratios are defined as deviations from a standard, multiplied by 1000. This unit is a "per mil". As a convention, the ratio is of the heavier isotope to the lower isotope.

化学元素由其质子数量定义,但原子的质量由核中的质子和中子数量确定。同位素是属于特定元素的原子,但其中子数量不同,因此具有不同的质量数。元素的同位素比例在世界各地略有不同,因此为了研究世界各地同位素比率的变化,同位素比率的变化被定义为与标准的偏差,乘以1000。这个单位是“千分之一”。按照惯例,比率是较重同位素与较轻同位素之间的比值。

{.displaystyle .delta {.ce {^{13}C}}=.left({.frac {.left({.frac {{.ce {^{13}C}}}{{.ce {^{12}C}}}}.right)_{sample}}{.left({.frac {{.ce {^{13}C}}}{{.ce {^{12}C}}}}.right)_{standard}}}-1.right).times 1000} ‰

These variations in isotopes can occur through many types of fractionation. They are generally classified as mass independent fractionation and mass dependent fractionation. An example of a mass independent process is the fractionation of oxygen atoms in ozone. This is due to the kinetic isotope effect (KIE) and is caused by different isotope molecules reacting at different speeds.[1] An example of a mass dependent process is the fractionation of water as it transitions from the liquid to gas phase. Water molecules with heavier isotopes (18O and 2H) tend to stay in the liquid phase as water molecules with lighter isotopes (16O and 1H) preferentially move to the gas phase.[2]

Of the different isotopes that exist, one common classification is distinguishing radioactive isotopes from stable isotopes. Radioactive isotopes are isotopes that will decay into a different isotope. For example, 3H (tritium) is a radioactive isotope of hydrogen. It decays into 3He with a half-life of ~12.3 years. By comparison, stable isotopes do not undergo radioactive decay, and their fixed proportions are measured against exponentially decaying proportions of radioactive isotopes to determine the age of a substance. Radioactive isotopes are generally more useful on shorter timescales, such as investigating modern circulation of the ocean using 14C, while stable isotopes are generally more useful on longer timescales, such as investigating differences in river flow with stable strontium isotopes.

These isotopes are used as tracers to study various phenomena of interest. These tracers have a certain distribution spatially, and so scientists need to deconvolve the different processes that affect these tracer distributions. One way tracer distributions are set is by conservative mixing. In conservative mixing, the amount of the tracer is conserved.[3] An example of this is mixing two water masses with different salinities. The salt from the saltier water mass moves to the less salty water mass, keeping the total amount of salinity constant. This way of mixing tracers is very important, giving a baseline of what value of a tracer one should expect. The value of a tracer as a point is expected to be an average value of the sources that flow into that region. Deviations from this are indicative of other processes. These can be called nonconservative mixing, where there are other processes that do not conserve the amount of tracer. An example of this is 𝛿14C. This mixes between water masses, but it also decays over time, reducing the amount of 14C in the region.

同位素的这些变化可以通过许多类型的分馏发生。它们通常被分类为质量独立分馏和质量依赖分馏。质量独立过程的一个例子是臭氧中氧原子的分馏。这是由于动力同位素效应(KIE),是由不同同位素分子以不同速度反应引起的。质量依赖过程的一个例子是水从液态过渡到气态时的分馏。具有较重同位素(18O和2H)的水分子倾向于留在液态,而具有较轻同位素(16O和1H)的水分子优先转移到气态。

在存在的不同同位素中,一种常见的分类是区分放射性同位素和稳定同位素。放射性同位素是将衰变为不同同位素的同位素。例如,3H(氚)是氢的放射性同位素。它以约12.3年的半衰期衰变成3He。相比之下,稳定同位素不会发生放射性衰变,其固定比例是根据指数衰减的放射性同位素比例来测量物质的年龄。放射性同位素通常在较短时间尺度上更有用,例如使用14C调查海洋现代环流,而稳定同位素通常在较长时间尺度上更有用,例如使用稳定的锶同位素调查河流流量的差异。

这些同位素被用作示踪剂来研究各种感兴趣的现象。这些示踪剂在空间上具有一定的分布,因此科学家需要解析影响这些示踪剂分布的不同过程。示踪剂分布的一种方式是通过保守混合来设定。在保守混合中,示踪剂的量是保持不变的。其中一种示踪剂混合的例子是将两个盐度不同的水团混合在一起。盐度较高的水团中的盐移动到盐度较低的水团中,保持总盐度量恒定。这种示踪剂混合方式非常重要,提供了预期的示踪剂值的基线。预期示踪剂值是预期为源流入该区域的平均值。与此相偏离的情况指示了其他过程。这些可以称为非保守混合,其中存在不保持示踪剂数量的其他过程。其中一个例子是𝛿14C。这种示踪剂在水团之间混合,但它也会随着时间衰减,减少该区域的14C数量。

Commonly used isotopes[edit]

The most used environmental isotopes are:

Ocean circulation[edit]

One topic that environmental isotopes are used to study is the circulation of the ocean. Treating the ocean as a box is only useful in some studies; in depth consideration of the oceans in general circulation models (GCMs) requires knowing how the ocean circulates. This leads to an understanding of how the oceans (along with the atmosphere) transfer heat from the tropics to the poles. This also helps deconvolve circulation effects from other phenomena that affect certain tracers such as radioactive and biological processes.

环境同位素被用于研究的一个话题是海洋环流。将海洋视为一个封闭的系统在某些研究中是有用的;但是在一般环流模型(GCMs)中深入考虑海洋需要了解海洋的循环方式。这有助于理解海洋(以及大气层)如何将热量从热带输送到极地。这也有助于将环流效应与其他影响特定示踪剂的现象(如放射性和生物过程)区分开来。

image.pngA summary of the path of the thermohaline circulation. Blue paths represent deep-water currents, while red paths represent surface currents.

Using rudimentary observation techniques, the circulation of the surface ocean can be determined. In the Atlantic basin, surface waters flow from the south towards the north in general, while also creating gyres in the northern and southern Atlantic. In the Pacific Ocean, the gyres still form, but there is comparatively very little large scale meridional (North-South) movement. For deep waters, there are two areas where density causes waters to sink into the deep ocean. These are in the North Atlantic and the Antarctic. The deep water masses formed are North Atlantic Deep Water (NADW) and Antarctic Bottom Water (AABW). Deep waters are mixtures of these two waters, and understanding how waters are composed of these two water masses can tell us about how water masses move around in the deep ocean.

This can be investigated with environmental isotopes, including 14C. 14C is predominantly produced in the upper atmosphere and from nuclear testing, with no major sources or sinks in the ocean. This 14C from the atmosphere becomes oxidized into 14CO2, allowing it to enter the surface ocean through gas transfer. This is transferred into the deep ocean through NADW and AABW. In NADW, the 𝛿14C is approximately -60‰, and in AABW, the 𝛿14C is approximately -160‰. Thus, using conservative mixing of radiocarbon, the expected amount of radiocarbon in various locations can be determined using the percent compositions of NADW and AABW at that location. This can be determined using other tracers, such as phosphate star or salinity.[4] Deviations from this expected value are indicative of other processes that affect the delta ratio of radiocarbon, namely radioactive decay. This deviation can be converted to a time, giving the age of the water at that location. Doing this over the world's ocean can yield a circulation pattern of the ocean and the rate at which water flow through the deep ocean. Using this circulation in conjunction with the surface circulation allows scientists to understand the energy balance of the world. Warmer surface waters flow northward while colder deep waters flow southward, leading to net heat transfer towards the pole.

利用基本的观测技术,可以确定海洋表面的环流。在大西洋盆地,表层水通常从南向北流动,同时在北大西洋和南大西洋形成旋涡。在太平洋,旋涡仍然形成,但整体上较少有大规模的经向(南北)运动。对于深层水域,有两个区域的密度使水体沉入深海。这些区域分别位于北大西洋和南极。形成的深层水团有北大西洋深层水(NADW)和南极底层水(AABW)。深层水是这两种水的混合物,了解水体是如何由这两种水团组成的可以告诉我们深海水团是如何运动的。

这可以通过使用包括14C在内的环境同位素来研究。14C主要在上层大气中产生,来自核试验,海洋中没有主要的来源或汇。大气中的这种14C被氧化成14CO2,使其通过气体转移进入表面海洋。这通过NADW和AABW转移到深海。在NADW中,𝛿14C约为-60‰,在AABW中,𝛿14C约为-160‰。因此,使用放射性碳的保守混合,可以使用该位置的NADW和AABW的百分比组成确定各个位置的放射性碳的预期量。这可以通过其他示踪剂进行确定,例如磷酸盐星或盐度。与预期值的偏离指示了影响放射性碳𝛿比的其他过程,即放射性衰变。这种偏差可以转换为时间,从而确定该位置的水的年龄。在世界范围内进行这项工作可以得出海洋的环流模式以及水体在深海中流动的速率。将这种环流与表面环流结合起来,科学家可以了解世界的能量平衡。更温暖的表层水向北流动,而更冷的深层水向南流动,导致净热量向极地传递。

Paleoclimate[edit]

Isotopes are also used to study paleoclimate. This is the study of how climate was in the past, from hundreds of years ago to hundreds of thousands of years ago. The only records of these times that we have are buried in rocks, sediments, biological shells, stalagmites and stalactites, etc. The isotope ratios in these samples were affected by the temperature, salinity, circulation of the ocean, precipitation, etc. of the climate at the time, causing a measurable change from the standards for isotope measurements. This is how climate information is encoded in these geological formations. Some of the many isotopes useful for environmental science are discussed below.

δ18O[edit]

One useful isotope for reconstructing past climates is oxygen-18. It is another stable isotope of oxygen along with oxygen-16, and its incorporation into water and carbon dioxide/carbonate molecules is strongly temperature dependent. Higher temperature implies more incorporation of oxygen-18, and vice versa. Thus, the ratio of 18O/16O can tell something about temperature. For water, the isotope ratio standard is Vienna Standard Mean Ocean Water, and for carbonates, the standard is Pee Dee Belemnite. Using ice cores and sediment cores that record information about the water and shells from past times, this ratio can tell scientists about the temperature of those times.

Climate record as reconstructed by Lisiecki and Raymo (2005) showing oscillations in the Earth's temperature over time. These oscillations have a 41 kyr cycle until about 1.2 million years ago, switching to a 100 kyr cycle that we see now.

This ratio is used with ice cores to determine the temperature at the spot in the ice core. Depth in an ice core is proportional to time, and it is "wiggle-matched" with other records to determine the true time of the ice at that depth. This can be done by comparing δ18O in calcium carbonate shells in sediment cores to these records to match large scale changes in the temperature of the Earth. Once the ice cores are matched to sediment cores, highly accurate dating methods such as U-series dating can be used to accurately determine the time of these events. There are some processes that mix water from different times into the same depth in the ice core, such as firn production and sloped landscape floes.

Lisiecki and Raymo (2005) used measurements of δ18O in benthic foraminifera from 57 globally distributed deep sea sediment cores, taken as a proxy for the total global mass of glacial ice sheets, to reconstruct the climate for the past five million years.[5] This record shows oscillations of 2-10 degrees Celsius over this time. Between 5 million and 1.2 million years ago, these oscillations had a period of 41,000 years (41 kyr), but about 1.2 million years ago the period switch to 100 kyr. These changes in global temperature match with changes in orbital parameters of the Earth's orbit around the Sun. These are called Milankovitch cycles, and these are related to eccentricity, obliquity (axial tilt), and precession of Earth around its axis. These correspond to cycles with periods of 100 kyr, 40 kyr, and 20 kyr.

δ18O can also be used to investigate smaller scale climate phenomena. Koutavas et al. (2006) used δ18O of G. ruber foraminifera to study the El Niño–Southern Oscillation (ENSO) and it's variability through the mid-Holocene.[6] By isolating individual foram shells, Koutavas et al. were able to obtain a spread of δ18O values at a specific depth. Because these forams live for approximately a month and that the individual forams were from many different months, clumped together in a small depth range in the coral, the variability of δ18O was able to be determined. In the eastern Pacific, where these cores were taken, the primary driver of this variability is ENSO, making this a record of ENSO variability over the core's time span. Koutavas et al. found that ENSO was much less variable in the mid Holocene (~6,000 years ago) than it is currently.

Strontium isotopes[edit]

Another set of environmental isotopes used in paleoclimate is strontium isotopes. Strontium-86 and strontium-87 are both stable isotopes of strontium, but strontium-87 is radiogenic, coming from the decay of rubidium-87. The ratio of these two isotopes depends on the concentration of rubidium-87 initially and the age of the sample, assuming that the background concentration of strontium-87 is known. This is useful because 87Rb is predominantly found in continental rocks. Particles from these rocks come into the ocean through weathering by rivers, meaning that this strontium isotope ratio is related to the weathering ion flux coming from rivers into the ocean. The background concentration in the ocean for 87Sr/86Sr is 0.709 ± 0.0012.[7] Because the strontium ratio is recorded in sedimentary records, the oscillations of this ratio over time can be studied. These oscillations are related to the riverine input into the oceans or into the local basin. Richter and Turekian have done work on this, finding that over glacial-interglacial timescales (105 years), the 87Sr/86Sr ratio varies by 3*10−5.[8]

Decay series of Actinides, including Uranium, Protactinium, Thorium, and Lead

Uranium and related isotopes[edit]

Uranium has many radioactive isotopes that continue emitting particles down a decay chainUranium-235 is in one such chain, and decays into protactinium-231 and then into other products. Uranium-238 is in a separate chain, decaying into a series of elements, including thorium-230. Both of these series end up forming lead, either lead-207 from uranium-235 or lead-206 from uranium-238. All of these decays are alpha or beta decays, meaning that they all follow first order rate equations of the form {.displaystyle dN/dt=.lambda N}, where λ is the half-life of the isotope in question. This makes it simple to determine the age of a sample based on the various ratios of radioactive isotopes that exist.

One way uranium isotopes are used is to date rocks from millions to billions of years ago. This is through uranium-lead dating. This technique uses zircon samples and measures the lead content in them. Zircon incorporates uranium and thorium atoms into its crystal structure, but strongly rejects lead. Thus, the only sources of lead in a zircon crystal are through decay of uranium and thorium. Both the uranium-235 and uranium-238 series decay into an isotope of lead. The half-life of converting 235U to 207Pb is 710 million years, and the half-life of converting 238U to 206Pb is 4.47 billion years. Because of high resolution mass-spectroscopy, both chains can be used to date rocks, giving complementary information about the rocks. The large difference in half-lives makes the technique robust over long time scales, from on the order of millions of years to on the order of billions of years.

Another way uranium isotopes are used in environmental science is the ratio of 231Pa/230Th. These radiogenic isotopes have different uranium parents, but have very different reactivities in the ocean. The uranium profile in the ocean is constant because uranium has a very large residence time compared to the residence time of the ocean. The decay of uranium is thus also isotropic, but the daughter isotopes react differently. Thorium is readily scavenged by particles, leading to rapid removal from the ocean into sediments.[9] By contrast, 231Pa is not as particle-reactive, feeling the circulation of the ocean in small amounts before settling into the sediment.[9] Thus, knowing the decay rates of both isotopes and the fractions of each uranium isotopes, the expected ratio of 231Pa/230Th can be determined, with any deviation from this value being due to circulation. Circulation leads to a higher 231Pa/230Th ratio downstream and a lower ratio upstream, with the magnitude of the deviation being related to flow rate. This technique has been used to quantify the Atlantic Meridional Overturning Circulation (AMOC) during the Last Glacial Maximum (LGM) and during abrupt climate change events in Earth's past, such as Heinrich events and Dansgaard-Oeschger events.[9][10]

Neodymium[edit]

Neodymium isotopes are also used to determine circulation in the ocean. All of the isotopes of neodymium are stable on the timescales of glacial-interglacial cycles, but 143Nd is a daughter of 147Sm, a radioactive isotope in the ocean. Samarium-147 has higher concentrations in mantle rocks vs crust rocks, so areas that receive river inputs from mantle-derived rocks have higher concentrations of 147Sm and 143Nd. However, these differences are so small, the standard notation of a delta value are no blunt for it; a more precise epsilon value is used to describe variations in this ratio of neodymium isotopes. It is defined as {.displaystyle .epsilon {.ce {_{Nd}}}=.left({.frac {.left({.frac {{.ce {^{143}Nd}}}{{.ce {^{144}Nd}}}}.right)_{sample}}{.left({.frac {{.ce {^{143}Nd}}}{{.ce {^{144}Nd}}}}.right)_{standard}}}-1.right).times 10000}

The only major sources of this in the ocean are in the North Atlantic and in the deep Pacific Ocean. Because one of the end-members is set in the interior of the ocean, this technique has the potential to tell us complementary information about paleoclimate compared to all other ocean tracers that are only set in the surface ocean.[9]

References[edit]
  1. ^ Gao, Yi Qin; Marcus, R. A. (2001-07-13). "Strange and Unconventional Isotope Effects in Ozone Formation". Science293 (5528): 259–263. Bibcode:2001Sci...293..259Gdoi:10.1126/science.1058528ISSN 0036-8075PMID 11387441S2CID 867229.

  2. ^ Kendall, Carol"USGS -- Isotope Tracers -- Resources -- Isotope Geochemistry"wwwrcamnl.wr.usgs.gov. Retrieved 2018-05-21.

  3. ^ Philp, R. Paul (2006-08-16). "The emergence of stable isotopes in environmental and forensic geochemistry studies: a review"Environmental Chemistry Letters5 (2): 57–66. doi:10.1007/s10311-006-0081-yISSN 1610-3653.

  4. ^ Rae, J. W. B.; Broecker, W. (2018-01-11). "What Fraction of the Pacific and Indian Oceans' Deep Water is formed in the North Atlantic?"Biogeosciences Discussions2018: 1–29. doi:10.5194/bg-2018-8ISSN 1810-6285.

  5. ^ Lisiecki, Lorraine E.; Raymo, Maureen E. (2005-01-18). "A Pliocene-Pleistocene stack of 57 globally distributed benthic δ18O records" (PDF)Paleoceanography20 (1): n/a. Bibcode:2005PalOc..20.1003Ldoi:10.1029/2004pa001071hdl:2027.42/149224ISSN 0883-8305S2CID 12788441.

  6. ^ Koutavas A, Demenocal PB, Olive GC, Lynch-Stieglitz J. 2006. Mid-Holocene El Ni˜ no-Southern Oscillation (ENSO) attenuation revealed by individual foraminifera in eastern tropical Pacific sediments. Geology 34:993–96

  7. ^ Murthy, V. Rama; Beiser, E. (1968-10-01). "Strontium isotopes in ocean water and marine sediments". Geochimica et Cosmochimica Acta32 (10): 1121–1126. Bibcode:1968GeCoA..32.1121Mdoi:10.1016/0016-7037(68)90111-7ISSN 0016-7037.

  8. ^ Richter, Frank M.; Turekian, Karl K. (1993-08-01). "Simple models for the geochemical response of the ocean to climatic and tectonic forcing". Earth and Planetary Science Letters119 (1–2): 121–131. Bibcode:1993E&PSL.119..121Rdoi:10.1016/0012-821X(93)90010-7ISSN 0012-821X.

  9. Jump up to:a b c d Lynch-Stieglitz, Jean; Adkins, Jess F.; Curry, William B.; Dokken, Trond; Hall, Ian R.; Herguera, Juan Carlos; Hirschi, Joël J.-M.; Ivanova, Elena V.; Kissel, Catherine (2007-04-06). "Atlantic meridional overturning circulation during the Last Glacial Maximum". Science316 (5821): 66–69. Bibcode:2007Sci...316...66Ldoi:10.1126/science.1137127ISSN 1095-9203PMID 17412948S2CID 44803349.

  10. ^ Lynch-Stieglitz, Jean (2017-01-03). "The Atlantic Meridional Overturning Circulation and Abrupt Climate Change". Annual Review of Marine Science9 (1): 83–104. Bibcode:2017ARMS....9...83Ldoi:10.1146/annurev-marine-010816-060415ISSN 1941-1405PMID 27814029.



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