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101.
V. M. Hamza R. R. Cardoso C. F. Ponte Neto 《International Journal of Earth Sciences》2008,97(2):205-226
A reappraisal of the international heat flow database has been carried out and the corrected data set was employed in spherical
harmonic analysis of the conductive component of global heat flow. Procedures used prior to harmonic analysis include analysis
of the heat flow data and determination of representative mean values for a set of discretized area elements of the surface
of the earth. Estimated heat flow values were assigned to area elements for which experimental data are not available. However,
no corrections were made to account for the hypothetical effects of regional-scale convection heat transfer in areas of oceanic
crust. New sets of coefficients for 12° spherical harmonic expansion were calculated on the basis of the revised and homogenized
data set. Maps derived on the basis of these coefficients reveal several new features in the global heat flow distribution.
The magnitudes of heat flow anomalies of the ocean ridge segments are found to have mean values of less than 150 mW/m2. Also, the mean global heat flow values for the raw and binned data are found to fall in the range of 56–67 mW/m2, down by nearly 25% compared to the previous estimate of 1993, but similar to earlier assessments based on raw data alone.
To improve the spatial resolution of the heat flow anomalies, the spherical harmonic expansions have been extended to higher
degrees. Maps derived using coefficients for 36° harmonic expansion have allowed identification of new features in regional
heat flow fields of several oceanic and continental segments. For example, lateral extensions of heat flow anomalies of active
spreading centers have been outlined with better resolution than was possible in earlier studies. Also, the characteristics
of heat flow variations in oceanic crust away from ridge systems are found to be typical of conductive cooling of the lithosphere,
there being little need to invoke the hypothesis of unconfined hydrothermal circulation on regional scales. Calculations of
global conductive heat loss, compatible with the observational data set, are found to fall in the range of 29–34 TW, nearly
25% less than the 1993 estimate, which rely on one-dimensional conductive cooling models. 相似文献
102.
空间管治视角下京津冀协同发展类型区划 总被引:4,自引:2,他引:2
京津冀协同发展的核心是基于问题导向和底线思维,打破行政区划,在更大区域尺度上优化资源配置,实现区域整体发展目标。因此,从优化空间规划体系的高度,开展京津冀区域协同发展的类型区划和类型区管理,实现分区施策的精细化管治极为重要。本文首先立足于京津冀区域发展差异,利用空间属性双聚类的方法将京津冀划分为中部核心功能引领区、东部沿海重点发展区、南部门户功能拓展区、西部和北部生态涵养保护区等四大区域;然后以区县为最小分析单元,从现状开发强度、用地增量预测和生态保护责任等三大维度构建类型划分指标体系,并利用三维空间坐标划分方法将京津冀划分为五大类型区,即:城镇优化发展区、城镇重点拓展区、现代农业发展区、适度建设发展区和严格生态保护区;最后,在空间管治视角下提出京津冀区域分区管治与区域协同管理的建议。 相似文献
103.
Computation of spherical harmonic coefficients and their error estimates using least-squares collocation 总被引:4,自引:0,他引:4
C. C. Tscherning 《Journal of Geodesy》2001,75(1):12-18
Equations expressing the covariances between spherical harmonic coefficients and linear functionals applied on the anomalous
gravity potential, T, are derived. The functionals are the evaluation functionals, and those associated with first- and second-order derivatives
of T. These equations form the basis for the prediction of spherical harmonic coefficients using least-squares collocation (LSC).
The equations were implemented in the GRAVSOFT program GEOCOL. Initially, tests using EGM96 were performed using global and
regional sets of geoid heights, gravity anomalies and second-order vertical gravity gradients at ground level and at altitude.
The global tests confirm that coefficients may be estimated consistently using LSC while the error estimates are much too
large for the lower-order coefficients. The validity of an error estimate calculated using LSC with an isotropic covariance
function is based on a hypothesis that the coefficients of a specific degree all belong to the same normal distribution. However,
the coefficients of lower degree do not fulfil this, and this seems to be the reason for the too-pessimistic error estimates.
In order to test this the coefficients of EGM96 were perturbed, so that the pertubations for a specific degree all belonged
to a normal distribution with the variance equal to the mean error variance of the coefficients. The pertubations were used
to generate residual geoid heights, gravity anomalies and second-order vertical gravity gradients. These data were then used
to calculate estimates of the perturbed coefficients as well as error estimates of the quantities, which now have a very good
agreement with the errors computed from the simulated observed minus calculated coefficients. Tests with regionally distributed
data showed that long-wavelength information is lost, but also that it seems to be recovered for specific coefficients depending
on where the data are located.
Received: 3 February 2000 / Accepted: 23 October 2000 相似文献
104.
Spatially restricted data distributions on the sphere: the method of orthonormalized functions and applications 总被引:1,自引:0,他引:1
In many geoscientific applications data are irregularly distributed and not globally available, e.g. caps around the poles
which are uncovered due to non-polar satellite orbits, or signals being defined solely on bounded regions on the globe. Starting
from a sequence of base functions with global support, which in the present case is composed of spherical harmonics being
initially non-orthogonal on a bounded subdomain, a set of functions is generated that constitutes an orthonormal basis. Different
approaches to realize this transformation are studied and compared with respect to numerical stability and computational effort,
and the corresponding effects on the coefficient recovery are investigated. A number of synthetic tests demonstrate the applicability,
the benefit, but also the limitations, of this method.
Received: 24 March 2000 / Accepted: 9 October 2000 相似文献
105.
The main advantages of constant potential enthalpy as a vertical coordinate are weaker horizontal velocity gradients in frontal
regions and a higher vertical resolution. A disadvantage is the intersection of isentropes with the ground and folding of
these surfaces. A numerical model is proposed to overcome the difficulties imposed by the intersection of isentropes with
the ground. The model contains a physical and computational domain. The top and bottom surfaces of the computational domain
are isentropes whereas the physical domain of the flow confined above by a free surface of constant pressure, and the bottom
of this domain is the surface of the earth. In the present study the top surfaces of these two domains coincide (θ
T, PTare constants in space and time). The model was tested for the study of frontogenesis and cyclogenesis and integrated for
7 days. The results correspond to enstrophy-conserving finite difference scheme. 相似文献
106.
P. M. Bakker 《Pure and Applied Geophysics》1996,148(3-4):583-589
A 4×4-propagator matrix formalism is presented for anisotropic dynamic ray tracing, including the propagation across curved interfaces. The computations are organised in the same way as in ervený's well-known isotropic propagator matrix formalism. Attention is paid to cases where double eigenvalues of the Christoffel matrix result in unstable expressions in the dynamic ray tracing system, but where geometrical spreading is well-behaved. 相似文献
107.
Hideo Kawai 《Journal of Oceanography》2003,59(2):163-172
Using natural coordinates, we have derived a criterion for the inertial instability of arbitrarily meandering currents. Such
currents, governed by the eccentrically cyclogeostrophic equation, are adopted as the basic current field for the parcel method.
We assume that any virtual displacement which is given to a water parcel moving in the basic field has no influence on this
field. From the conservation of mechanical energy for a virtual displacement we derive an inertial instability frequency ω
m
= [(f + 2u/r)Z]0.5 for the eccentrically cyclogeostrophic current, where f is the Coriolis parameter, u the velocity (always positive), r the radius of curvature of a streamline (negative for an anticyclonic meander), and Z the vertical component of absolute vorticity. If ω
m
2 is negative, the eccentrically cyclogeostrophic current becomes unstable. Although the conventional, centrifugal instability
criterion, derived from the conservation of angular momentum in a circularly symmetric current field, has a certain meaning
for a monopolar vortex, it contains a radial shear vorticity that is difficult to use in arbitrarily meandering currents.
The new criterion ω
m
2 contains a lateral shear vorticity that is applicable to arbitrarily meandering currents. Examining instabilities of concentric
rings with radii of 50–100 km, we consider reasons why the anticyclonic supersolid rotation has been very much less frequently
observed than the cyclonic supersolid rotation, despite a prediction of some common stability and a rapid change in radial
velocity gradient for the former. Classifying eccentric streamlines into the large and small curvature-gradient types, we
point out that the large-gradient curvature in anticyclonic rings is apt to be unstable.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
108.
Sensitivity studies with a new generalized coordinate ocean model are performed in order to compare the behavior of bottom boundary layers (BBLs) when terrain-following (sigma or combined sigma and z-level) or z-level vertical grids are used, but most other numerical aspects remain unchanged. The model uses a second-order turbulence closure scheme that provides surface and BBL mixing and results in a quite realistic climatology and deep water masses after 100 year simulations with a coarse resolution (1° × 1°) basin-scale terrain-following grid. However, with the same turbulence scheme but using a z-level grid, the model was unable to produce dense water masses in the deep ocean. The latter is a known problem for coarse resolution z-level models, unless they include highly empirical BBL schemes.A set of dense water overflow experiments with high-resolution grids (10 and 2.5 km) are used to investigate the influence of model parameters such as horizontal diffusivity, vertical mixing, horizontal resolution, and vertical resolution on the simulation of bottom layers for the different coordinate systems. Increasing horizontal diffusivity causes a thinner BBL and a bottom plume that extends further downslope in a sigma grid, but causes a thicker BBL and limited downslope plume extension in a z-level grid. A major difference in the behavior of the BBL in the two grids is due to the larger vertical mixing generated by the turbulence scheme over the step-like topography in the z-level grid, compared to a smaller vertical mixing and a more stably stratified BBL in the sigma grid. Therefore, the dense plume is able to maintain its water mass better and penetrates farther downslope in the sigma grid than in the z-level grid. Increasing horizontal and vertical resolution in the z-level grid converges the results toward those obtained by a much coarser resolution sigma coordinate grid, but some differences remain due to the basic differences in the mixing process in the BBL. 相似文献
109.
In the present study, a Fourier analysis is used to develop expressions for phase and group speeds for both continuous and discretized, linearized two-dimensional shallow water equations, in Cartesian coordinates. The phase and group speeds of the discrete equations, discretized using a three-point scheme of second order, five-point scheme of fourth order and a three-point compact scheme of fourth order in an Arakawa C grid, are calculated and compared with the corresponding values obtained for the continuous system. The three-point second-order scheme is found to be non-dispersive with grid resolutions greater than 30 grids per wavelength, while both the fourth-order schemes are non-dispersive with grid resolutions greater than six grids per wavelength. A von Neumann stability analysis of the two- and three-time-level temporal schemes showed that both schemes are stable. A wave deformation analysis of the two-time-level Crank–Nicolson scheme for one-dimensional and two-dimensional systems of shallow water equations shows that the scheme is non- dispersive, independent of the Courant number and grid resolution used. The phase error or the dispersion of the scheme decreases with a decrease in the time step or an increase in grid resolution. 相似文献
110.
在曲线坐标系下,建立了缓变水深水域波浪传播的数值模拟模型.模型适宜于复杂变化的边界形状,克服了各种代数坐标变换的局限性.在建立模型时,将原始的椭圆型缓坡方程的近似型式——依赖时间变化的抛物型方程,作为控制方程,既克服了一般抛物近似方法的缺点,又便利了方程的求解;从开边界条件、不同反射特性的固壁边界条件相统一的表达式出发,对边界条件进行处理;用ADI法数值求解控制方程.对模型的验证表明,数值解与物模实验值吻合良好,模型对于具有复杂边界的工程实际有较强的适应性. 相似文献