Disturbance, stream incision, and channel evolution: The roles of excess transport capacity and boundary materials in controlling channel response

Channel incision is part of denudation, drainage-network development, and landscape evolution. Rejuvenation of fluvial networks by channel incision often leads to further network development and an increase in drainage density as gullies migrate into previously non-incised surfaces. Large, anthropogenic disturbances, similar to large or catastrophic “natural” events, greatly compress time scales for incision and related processes by creating enormous imbalances between upstream sediment delivery and available transporting power. Field examples of channel responses to antrhopogenic and “natural” disturbances are presented for fluvial systems in the mid continent and Pacific Northwest, USA, and central Italy. Responses to different types of disturbances are shown to result in similar spatial and temporal trends of incision for vastly different fluvial systems. Similar disturbances are shown to result in varying relative magnitudes of vertical and lateral (widening) processes, and different channel morphologies as a function of the type of boundary sediments comprising the bed and banks. This apparent contradiction is explained through an analysis of temporal adjustments to flow energy, shear stress, and stream power with time. Numerical simulations of sand-bed channels of varying bank resistance and disturbed by reducing the upstream sediment supply by half, show identical adjustments in flow energy and the rate of energy dissipation. The processes that dominate adjustment and the ultimate stable geometries, however, are vastly different, depending on the cohesion of the channel banks and the supply of hydraulically-controlled sediment (sand) provided by bank erosion.The non-linear asymptotic nature of fluvial adjustment to incision caused by channelization or other causes is borne out in similar temporal trends of sediment loads from disturbed systems. The sediments emanating from incised channels can represent a large proportion of the total sediment yield from a landscape, with erosion from the channel banks generally the dominant source. Disturbances that effect available force, stream power or flow energy, or change erosional resistance such that an excess of flow energy occurs can result in incision. Channel incision, therefore, can be considered a quintessential feature of dis-equilibrated fluvial systems.     

Modeling nitrogen–carbon cycling and oxygen consumption in bottom sediments

A model framework is presented for simulating nitrogen and carbon cycling at the sediment–water interface, and predicting oxygen consumption by oxidation reactions inside the sediments. Based on conservation of mass and invoking simplifying assumptions, a coupled system of diffusive–reactive partial differential equations is formulated for two-layer conceptual model of aerobic–anaerobic sediments. Oxidation reactions are modeled as first-order rate processes and nitrate is assumed to be consumed entirely in the anoxic portion of the sediments. The sediments are delineated into a thin oxygenated surface layer whose thickness is equal to the oxygen penetration depth, and a lower, but much thicker anoxic layer. The sediments are separated from the overlying water column by a relatively thin boundary layer through which mass transfer is diffusion controlled. Transient solutions are derived using the method of Laplace transform and Green’s function, which relate pore-water concentrations of the constituents to their concentrations in the bulk water and to the flux of decomposable settling organic matter. Steady-state pore-water concentrations are also obtained including expressions for the extent of methane saturation zone and methane gas flux. A relationship relating the sediment oxygen demand (SOD) to bulk water oxygen is derived using the two-film concept, which in combination with the depth-integrated solutions forms the basis for predicting the extent of oxygen penetration in the sediment. Iterative procedure and simplification thereof are proposed to estimate the extent of methane saturation zone and thickness of the aerobic layer as functions of time. Sensitivity of steady-state solutions to key parameters illustrates sediment processes interactions and synergistic effects. Simulations indicate that for a relatively thin diffusive boundary layer, d, oxygen uptake is limited by biochemical processes inside the sediments, whereas for a thick boundary layer oxygen transfer through the diffusive boundary layer is limiting. The results show an almost linear relationship between steady-state sediment oxygen demand and bulk water oxygen. For small d methane and nitrogen fluxes are sediment controlled, whereas for large d they are controlled by diffusional transfer through the boundary layer. It is shown that the two-layer model solution converges to the one-layer model (anaerobic layer) solution as the thickness of the oxygenated layer approaches zero, and that the transient solutions approach asymptotically their corresponding steady-state solutions.     

MAST solution of advection problems in irrotational flow fields

A new numerical–analytical Eulerian procedure is proposed for the solution of convection-dominated problems in the case of existing scalar potential of the flow field. The methodology is based on the conservation inside each computational elements of the 0th and 1st order effective spatial moments of the advected variable. This leads to a set of small ODE systems solved sequentially, one element after the other over all the computational domain, according to a MArching in Space and Time technique. The proposed procedure shows the following advantages: (1) it guarantees the local and global mass balance; (2) it is unconditionally stable with respect to the Courant number, (3) the solution in each cell needs information only from the upstream cells and does not require wider and wider stencils as in most of the recently proposed higher-order methods; (4) it provides a monotone solution. Several 1D and 2D numerical test have been performed and results have been compared with analytical solutions, as well as with results provided by other recent numerical methods.     

电离层上行O+离子沿不同经度处的磁力线向磁层的传输

根据解析求解引导中心近似的动力学方程得到的离子分布函数 ,研究了不同Kp指数条件下起源于不同电离层区域的上行O⁺离子通量密度沿不同经度处的磁力线的定态分布 ,并研究了上行O⁺离子向不同磁层区域传输的特性 .主要结果为 :（ 1 ）起源于向阳面极光带外侧及更低纬区的电离层离子基本上传输到向阳面磁层区 ;起源于背阳面极光带及更低纬区的电离层离子基本上传输到背阳面磁尾等离子体片区和闭合磁力线区 ;起源于极盖区及向阳面极光带内侧的电离层离子基本上传输到等离子体幔区和磁瓣区 .（ 2 ）上行离子主要分布在近地空间 ,其通量密度相对于地心距离呈负梯度 .（ 3）地磁活动指数Kp 增高时上行离子进入磁层的概率增大 ,因而上行离子起动力学作用的地球空间范围增大 .所得结果可解释有关地顶的观测特征 ,理论估算的上行离子在磁尾的通量密度与观测结果相符合.     

Sharing as sociomaterial practice: Car sharing and the material reconstitution of automobility

Sharing has become one of the buzzwords of contemporary urban life and scholarship, as cities and social lives are transformed by the share economy and collaborative consumption. This paper advances critical analysis of sharing economies through an investigation of the ways in which objects are mobilized in the practice of sharing. Drawing on an empirical base of 35 interviews conducted with Sydney residents using car sharing as a form of transport, we explicate the material entanglements that constitute car sharing in order to highlight the complex intersections of the object being shared, the constellations of objects brought into the orbit of the practice, and the code that flows through each. Bringing together a material-focused analysis into conversation with the concepts of share economies as both performed and hybrid, we advance the concepts of sharing as a set of socio-material entanglements. We argue that the divergent spatialities and temporalities of objects and humans both hold together and tear apart the experiences of sharing, which in turn underpins car sharing’s implications for the reconstitution of automobility.     

中亚热带2种天然林表层土壤N2O排放速率

运用静态箱-气相色谱法对中亚热带地区米槠天然林和阿丁枫天然林土壤N2O排放速率进行了1年（2012年1月—2013年1月）原位观测,分析了土壤温度及含水量对土壤N2O排放速率的影响,并探讨土壤无机N含量变化与土壤N2O排放速率的关系。结果表明,观测期间,2种天然林均表现为大气N2O排放源,米槠天然林和阿丁枫天然林平均土壤N2O排放速率分别为7.29μg·m^-2·h^-1、7.41μg·m^-2·h^-1;米槠天然林和阿丁枫天然林土壤N2O排放速率季节变化明显,最高排放速率均出现在夏季6月,分别为16.51μg·m^-2·h^-1、18.86μg·m^-2·h^-1;2个林分N2O排放速率最低值分别出现在2012年1月和2012年9月,分别为3.04μg·m^-2·h^-1和2.17μg·m^-2·h^-1。2种天然林土壤N2O排放速率均与土壤温度无显著相关性,与土壤含水量显著正相关（P〈0.05）;2种天然林土壤N2O排放速率与NH4＋含量均无显著相关性,米槠天然林和阿丁枫天然土壤N2O排放速率与NO3-含量分别呈显著负相关和显著正相关（P〈0.05）。研究结果表明,土壤含水量及NO3-含量的变化对中亚热带天然林土壤N2O排放速率有着重要的影响。     

Cross helicity and related dynamo

The turbulent cross helicity is directly related to the coupling coefficients for the mean vorticity in the electromotive force and for the mean magnetic-field strain in the Reynolds stress tensor. This suggests that the cross-helicity effects are important in the cases where global inhomogeneous flow and magnetic-field structures are present. Since such large-scale structures are ubiquitous in geo/astrophysical phenomena, the cross-helicity effect is expected to play an important role in geo/astrophysical flows. In the presence of turbulent cross helicity, the mean vortical motion contributes to the turbulent electromotive force. Magnetic-field generation due to this effect is called the cross-helicity dynamo. Several features of the cross-helicity dynamo are introduced. Alignment of the mean electric-current density J with the mean vorticity Ω , as well as the alignment between the mean magnetic field B and velocity U , is supposed to be one of the characteristic features of the dynamo. Unlike the case in the helicity or α effect, where J is aligned with B in the turbulent electromotive force, we in general have a finite mean-field Lorentz force J ?×? B in the cross-helicity dynamo. This gives a distinguished feature of the cross-helicity effect. By considering the effects of cross helicity in the momentum equation, we see several interesting consequences of the effect. Turbulent cross helicity coupled with the mean magnetic shear reduces the effect of turbulent or eddy viscosity. Flow induction is an important consequence of this effect. One key issue in the cross-helicity dynamo is to examine how and how much cross helicity can be present in turbulence. On the basis of the cross-helicity transport equation, its production mechanisms are discussed. Some recent developments in numerical validation of the basic notion of the cross-helicity dynamo are also presented.     

Cenozoic Evolution of Sediments and Climate Change and Response to Tectonic Uplift of the Northeastern Tibetan Plateau

Through a comprehensive study of magnetostratigraphy and sedimentology of several basins in the northeastern Tibetan Plateau, we reveal that the study area mainly experienced six tectonic uplift stages at approximately 52 Ma, 34–30 Ma, 24–20 Ma, 16–12 Ma, 8–6 Ma, and 3.6–2.6 Ma. Comprehensive analyses of pollen assemblages from the Qaidam, Linxia, Xining, and West Jiuquan Basins show that the northeastern Tibetan Plateau has undergone six major changes in vegetation types and climate: 50–40 Ma for the warm-humid forest vegetation, 40–23 Ma for the warm-arid and temperate-arid forest steppe vegetation, 23–18.6 Ma for the warm-humid and temperatehumid forest vegetation, 18.6–8.5 Ma for the warm-humid and cool-humid forest steppe vegetation, 8.6–5 Ma for the temperate sub-humid savanna steppe vegetation, and 5–1.8 Ma for the cold-arid steppe vegetation. Comprehensive comparisons of tectonic uplift events inferred from sedimentary records, climatic changes inferred from pollen, and global climate changes show that in the northeastern Tibetan Plateau the climate in the Paleogene at low altitude was mainly controlled by the global climate change, while that in the Neogene interval with high altitude landscapes of mountains and basins is more controlled by altitude and morphology.     

Portable seiche gauge

A portable instrument with a power consumption of less than 1 W has been developed to measure water height at temporary locations. The full scale range of the recorder is 500 mm, and resolution is better than 5 mm water height. Results obtained with the instrument are given, showing seiche activity in a lake.     

Eimeria anguillae léger & hollande, 1922 parasitic in New Zealand eels

Eimeria anguillae Léger & Hollande, 1922 (Sporozoa: Coccidia) is recorded from Anguilla australis Richardson, 1848 and A. dieffenbachii Gray, 1842 introduced as elvers into a New Zealand eel farm. The parasite is identified by the hexagonal cross section of the sporocysts, dimensions, and lack of asexual and early sexual stages in the mucosal and submucosal tissues. Discrepancies in previously published details of the micropyle and sporocyst vestigal body are attributed to the limitations of earlier microscopes.

In heavy infections the mucosa and submucosa are partially or totally destroyed, and both oocysts and sporocysts are passed out with necrotic tissue.