Undisturbed soil-core sampler for submerged puddled soils

1991 ◽  
Vol 4 (3) ◽  
pp. 315-317
Author(s):  
P.K. Sharma ◽  
R.M. Bhagat
1990 ◽  
Vol 70 (1) ◽  
pp. 115-118 ◽  
Author(s):  
S. TESSIER ◽  
H. STEPPUHN

The design for a sleeve-type, quick-mount soil core sampler for bulk density and soil water content determination and for collection of undisturbed soil samples is described and its performance discussed. This core sampler has been used to collect undisturbed soil core samples 47.5 mm in diameter and 300 mm long in tillage and seeding studies. Less than 2 min is required to retrieve, seal and store each soil core sample. The soil samples are contained in 50.8-mm-diameter aluminum liners which are easily sealed with plastic caps and stored for later laboratory analysis. This sampler resulted in very good measurement repeatability and provided subsamples suitable for water retention curve determinations. Key words: Soil sampler, coring device, bulk density, soil moisture, undisturbed cores


Soil Science ◽  
1975 ◽  
Vol 120 (2) ◽  
pp. 153-155 ◽  
Author(s):  
C. W. HAYDEN ◽  
C. W. ROBBINS

1991 ◽  
Vol 55 (6) ◽  
pp. 1792-1795 ◽  
Author(s):  
J. M. H. Hendrickx ◽  
C. J. Ritsema ◽  
O. H. Boersma ◽  
L. W. Dekker ◽  
W. Hamminga ◽  
...  

2005 ◽  
Vol 62 (5) ◽  
pp. 493-497 ◽  
Author(s):  
Herdjania Veras de Lima ◽  
Álvaro Pires da Silva ◽  
Sílvia Imhoff ◽  
Afrânio Ferreira Neves Junior

Due to the narrow window of ideal moisture conditions required for collecting undisturbed soil samples from hardsetting horizons in the field, this study compared the efficiency of an alternative method of soil core removal in the laboratory with that of the traditional field method by using measurements of soil bulk density data (Db). In a first sampling, cylinders were removed with a soil sampler in the field. In a second sampling, large soil blocks were removed with Kubiena-type zinc (brass) boxes in the field. Volumetric core cylinder samples were removed from these blocks in the laboratory with a manual hydraulic pump. There were no differences between the Db values determined from the laboratory and the field coring method. The laboratory method was considered more efficient than the field method because it allowed reductions in the errors made by operators in the field, and those caused by differences in soil water content. The laboratory method allows sampling in hardsetting horizons throughout the year, and collecting soil core samples under conditions of controlled moisture and applied force.


2011 ◽  
Vol 50 (No. 6) ◽  
pp. 250-256 ◽  
Author(s):  
P. Prikner ◽  
F. Lachnit ◽  
F. Dvořák

The portable soil core sampler was engineered for gradual sampling of soil profile in the depth up to 0.5 m, which ensures extraction of the whole sample volume of soil profile in determinable depth. The portable soil core sampler was compared with the professional soil probe Eijkelkamp P1.31 (Eijkelkamp Agrisearch Equipment, Netherlands) in field conditions. The portable sampler was compared with the physical soil sample rings in laboratory conditions to eliminate all of possible restrictive aspects affecting the procedure of measurement. The portable soil core sampler with inner diameter 71 mm, depth 120 mmenables gradually take samples of soil profile by step of 50 mmand is able to detect possible local extremes. On the other hand a soil probe is not able to reach desired accuracy in taking of a&nbsp;soil sample. Values measured from a soil probe approximately taken by step of 150 mmare inaccurate. The values of bulk density of both sampling methods were variable at significant interval from 40 into 80 kg/m<sup>3</sup>. Different values could be caused by soil profile condition and by the use of different sampling methods. The design of a portable soil sampler should be of assistance in fast and precise soil profiling sample collection, which is required to determine bulk density of the soil, its variance depending on moisture content in soil compaction determining criteria.


1982 ◽  
Vol 46 (2) ◽  
pp. 433-434 ◽  
Author(s):  
S. K. Chong ◽  
M. A. Khan ◽  
R. E. Green
Keyword(s):  

Soil Science ◽  
1958 ◽  
Vol 85 (6) ◽  
pp. 297-301 ◽  
Author(s):  
L. A. ANDREWS ◽  
W. M. BROADFOOT
Keyword(s):  

2020 ◽  
Author(s):  
Kirill Gerke ◽  
Marina Karsanina

&lt;p&gt;Classic soil physics relies heavily on the concept of representative elementary volume (REV), which is necessary to perform upscaling from the studied soil samples and parameterize continuum scale hydrological models (e.g., based on Richards equation). In this paper we explore the boundaries of the classic REV concept and conventional representativity studies that claim REV for a given physical property if its values converge to a steady value with increasing sample&amp;#8217;s volume. We chose two conventional undisturbed soil samples from Ah and B horizons and performed pore-scale flow simulations based on their X-ray microtomography scans. The volumes of the simulation domains were 729 million of voxels with a physical volume within the order of magnitude of the whole soil core. Based on 3D pore geometry images and resulting flow velocity and pressure fields we performed REV analysis for saturated hydraulic conductivity and porosity. To further facilitate the REV analysis, we also evaluated the stationarity of pore structures by computing directional correlation functions for studied images. We concluded that neither of the studied samples can be considered to be representative due to its structural non-stationarity, which reflects on the behavior of Ksat values within the subcubes of different volume within the samples. In this contribution we extensively discuss the implications of such results. While it was possible to show that studied soil samples are not REVs for saturated hydraulic conductivity, we were unable to establish any relevant domain length scale. The latter may require tensorial flow property analysis with correct boundary conditions (Gerke et al., 2019), multi-scale soil structure imaging (Gerke et al., 2015; Karsanina et al., 2018; Karsanina and Gerke, 2018) and pore-scale simulations on fused multi-scale images (Miao et al., 2017; Gerke et al., 2018).&lt;/p&gt;&lt;p&gt;This work was supported by Russian Foundation for Basic Research grant 20-54-12030 &amp;#1053;&amp;#1053;&amp;#1048;&amp;#1054;_&amp;#1072; and 18-34-20131 &amp;#1084;&amp;#1086;&amp;#1083;_&amp;#1072;_&amp;#1074;&amp;#1077;&amp;#1076;.&lt;/p&gt;&lt;p&gt;References:&lt;/p&gt;&lt;p&gt;Karsanina, M. V., Gerke, K. M., Skvortsova, E. B., Ivanov, A. L., &amp; Mallants, D. (2018). Enhancing image resolution of soils by stochastic multiscale image fusion. Geoderma, 314, 138-145.&lt;/p&gt;&lt;p&gt;Gerke, K. M., Karsanina, M. V., &amp; Mallants, D. (2015). Universal stochastic multiscale image fusion: an example application for shale rock. Scientific reports, 5, 15880.&lt;/p&gt;&lt;p&gt;Gerke, K. M., Vasilyev, R. V., Khirevich, S., Collins, D., Karsanina, M. V., Sizonenko, T. O., Korost D.V., Lamontagne S., &amp; Mallants, D. (2018). Finite-difference method Stokes solver (FDMSS) for 3D pore geometries: Software development, validation and case studies. Computers &amp; Geosciences, 114, 41-58&lt;/p&gt;&lt;p&gt;Karsanina, M. V., &amp; Gerke, K. M. (2018). Hierarchical Optimization: Fast and Robust Multiscale Stochastic Reconstructions with Rescaled Correlation Functions. Physical Review Letters, 121(26), 265501.&lt;/p&gt;&lt;p&gt;Miao, X., Gerke, K. M., &amp; Sizonenko, T. O. (2017). A new way to parameterize hydraulic conductances of pore elements: A step towards creating pore-networks without pore shape simplifications. Advances in Water Resources, 105, 162-172.&lt;/p&gt;&lt;p&gt;Gerke, K. M., Karsanina, M. V., &amp; Katsman, R. (2019). Calculation of tensorial flow properties on pore level: Exploring the influence of boundary conditions on the permeability of three-dimensional stochastic reconstructions. Physical Review E, 100(5), 053312.&lt;/p&gt;


2021 ◽  
Author(s):  
Giorgio Capello ◽  
Marcella Biddoccu ◽  
Simone Di Prima ◽  
Laurent Lassabatere

&lt;p&gt;Adopting integrated measurement techniques may enhance our understanding of hydropedological processes within the critical zone. To investigate lateral subsurface flow due to lithological discontinuities, a ponding infiltration test, two GPR surveys, and soil penetration resistance (PR) measurements were conducted on a 1 m&lt;sup&gt;2&lt;/sup&gt; plot in a vegetated area located in the university campus of Doua (Lyon, France). A GPR grid with 0.2 m intervals was established. In the center of the grid, around the root system of a hawthorn shrub, an infiltration test was conducted using an automated single-ring infiltrometer proposed by Concialdi et al. (2020), to infiltrate a shear-thinning viscous solution (1 g L&lt;sup&gt;&amp;#8722;1&lt;/sup&gt; Xanthan gum powder). The viscous solution was expected to fill preferential pathways due to the roots, with limited infiltration into the soil matrix, and thus reveal complex geometries or macropore networks in highly heterogeneous soils. To create three-dimensional (3D) representations of the infiltrated solution, two GPR surveys were carried out just before and 20 min after the infiltration test, using a GSSI (Geophysical Survey System Inc., Salem, NH) SIR 3000 system with a 900 MHz antenna. A total of 24 radargrams were collected in time mode by moving the antenna along the survey lines and recording the markers position along the survey line intersections. After the second GPR survey, PR was measured at each of the 36 intersection points of the grid using an electronic hand-pushed cone penetrometer. The cone had a 30&amp;#176; angle and a base area of 1 cm&lt;sup&gt;2&lt;/sup&gt;, inserted into the soil at a constant speed of 2 cm s&lt;sup&gt;&amp;#8722;1&lt;/sup&gt; to a depth of 0.8 m. These measurements were aimed to highlight contrasting penetration resistance characteristics between different soil horizons. We also determined the soil bulk density from 24 undisturbed soil cores (~ 100 cm&lt;sup&gt;3&lt;/sup&gt;) collected at different depths from 0 to 50 cm. Finally, an auger was used to extract a 0.69-m-depth soil core for the direct observation of lithological heterogeneities.&lt;/p&gt;&lt;p&gt;Differenced radargrams from pre- and post-infiltration surveys allowed to detect the 3D infiltration bulb, which was vertically elongated and irregularly shaped, but with an evident horizontal divergence between the depth of 20 and 30 cm. Below 30 cm depth, a significant increasing of soil PR and BD (respectively higher than 2.5 MPa and 1.50 g cm&lt;sup&gt;-3&lt;/sup&gt;, between 30 and 50 cm depth) was detected, indicating the presence of a underlying layer, which was also identifiable by visual observation of the soil core. This dense layer impeded water flow. Consequently, the liquid solution partially diverged laterally and accumulated upside this layer, and partially infiltrated into the dense layer along preferential flow paths in correspondence with the plant root system, as detected by the 3D GPR diagram. Summing up and considering every aspect, this study allowed to identify water perching above a shallow restrictive layer for a better understanding of the water dynamics of the investigated soil. This study shows the benefits to couple different types of soil physics approaches to relate hydrological processes to the soil hydraulic and mechanical properties.&lt;/p&gt;


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