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  • About
  • The Global ETD Search service is a free service for researchers to find electronic theses and dissertations. This service is provided by the Networked Digital Library of Theses and Dissertations.
    Our metadata is collected from universities around the world. If you manage a university/consortium/country archive and want to be added, details can be found on the NDLTD website.
61

Tip Resistance Of A Miniature Cone Penetrometer Using Triaxial Apparatus For Clean And Silty Sand

Raju, K V S B 06 1900 (has links)
The static cone penetration tests are quite extensively used for carrying out in-situ geotechnical investigations both for onshore and offshore sites especially where the soil mass is expected to comprise of either soft to medium stiff clays or loose to medium dense sands. The wide use of the cone penetration tests (CPT) in geotechnical engineering has resulted in a great demand for developing necessary correlations between the cone penetration resistance and different engineering properties of soils. The successful interpretation of the cone penetration test data depends mainly on the various empirical correlations which are often derived with the help of a controlled testing in calibration chambers. The calibration chambers have been deployed in various sizes (diameter varying from 0.55 m to 2.10 m) by a number of researchers. It is quite an expensive and time consuming exercise to carry out controlled tests in a large size calibration chamber. The task becomes even much more difficult when a sample comprising of either silt or clay has to be prepared. As a result, most of the reported cone penetration tests in calibration chambers are mainly performed in a sandy material. Taking into account the various difficulties associated with performing tests in large calibration chambers, in the present study, it is attempted to make use of a miniature static cone penetrometer having a diameter of 19.5 mm. This cone was gradually penetrated at a uniform rate in a triaxial cell in which a soil sample of a given material was prepared; the diameter of the cone was intentionally chosen smaller so that the ratio of the diameter of the cell to that of the cone becomes a little larger. Two different diameters of the cells, namely, 91 mm and 140 mm, were used to explore the effect of the ratio of chamber (cell) size to that of the cone size. In addition, the rate of penetration rate was also varied from 0.6 mm/minute to 6.0 mm/minute (the maximum possible rate for the chosen triaxial machine with the larger cell) to examine the effect of the rate of the penetration of the miniature cone on the tip resistance. By using the chosen experimental setup, a large number of static miniature cone penetrometer tests were carried out on four different materials, namely, (i) clean sand, (ii) sand with 15% silt, (iii) sand with 25% silt, and (iv) sand with 15% fly ash. The cone tip resistance for each material was obtained for a wide range of three different relative densities. The effective vertical pressure (σv) for the tests on different samples was varied in between 100 kPa and 300 kPa. The variations of the tip resistance with axial deformation in all the cases were monitored so as to find the magnitude of the ultimate tip resistance. In contrast to the standard cone, the diameter of the piston shaft was intentionally kept a little smaller than that of the cone itself so as to restrict the development of the piston resistance. For each cell (chamber) size, two different sizes of the pistons were used to assess the resistance offered by the penetration of the piston shaft itself. It was noted that the resistance offered by the chosen piston shaft is not very substantial as compared to that of the cone tip itself. Most of the experimental observations noted from the present experiments were similar to those made by the penetration of the standard size cone in a large calibration chamber. The ultimate tip resistance of the cone was found to increase invariably with an increase in the magnitude of σv. An increase in the relative density of the soil mass leads to an increase in the value of qcu. For the same range of relative densities, an addition of fly ash in the sample of sand, leads to a considerable reduction in the magnitude of qcu. Even with the addition of 25% silt, the values of qcu were found to become generally lower as compared to clean sand and sand added with 15% silt. An employment of a larger ratio of the diameter of the cell to that of the miniature cone leads to an increased magnitude of qcu. An increase in the penetration rate from 0.6 mm/min to 6.0 mm/min, was found to cause a little increase in the magnitude of qcu especially for sand added with fly ash and silt. The effect of the penetration rate on the results was found to increase continuously with a reduction in the rate of penetration. At higher penetration rates, in a range closer to those normally employed in the field (20 mm/sec), it is expected that the rate of penetration of the cone will not have any substantial effects on the magnitude of qcu for clean sands. The magnitude of qcu obtained in this thesis at different values of σv for all the cases with the use of the miniature cone were compared with the two widely used correlations in literature. It is found that except for dense sands, in most of the cases, the present experimental data lie generally in between the two correlation curves from literature; for dense sands the measured values of qcu were found to be significantly lower than the chosen correlation curves. It was noted that with the use of the miniature cone penetrated in a given sample prepared in a triaxial cell, it is possible to obtain reasonably an accurate estimate of the tip resistance of the standard cone especially for loose to medium dense states of all the materials. Further, from the analysis of all the tests results, it was noted that approximately a linear correlation between qcu/σv and soil friction angle (φ) for different chosen materials exists provided the dependency of the φ on the stress level is taken into account. As compared to the standard cone penetrometer which is usually employed in the field, the miniature cone used in this study is expected to provide a little conservative estimate, of the tip resistance of the standard static cone penetrometer with reference to the different materials used in this study on account of the facts that (i) there is a reduced area behind the cone, (ii) the ratio of the diameter of the calibration chamber (cell) to that of cone is not very high, (iii) the chosen size of the cone is smaller than the standard cone, and (iv) the chosen penetration rate is much smaller than the standard rate of penetration. Further, in the case of clean sand, an attempt has also been made in this thesis, with the help of a number of direct shear tests at different stress levels, to generate an expression correlating peak friction angle, critical state friction angle, relative density of sand and vertical effective stress. A correlation has been generated with the help of which, the value of peak dilatancy angle can be obtained from the known values of peak friction angle and critical state friction angle. In confirmation with the available information in literature, this exercise on clean sand has clearly indicated that a decrease in the magnitude of vertical effective stress leads to an increase in the values of both peak friction angles and peak dilatancy angles.
62

The ecology and utilization of dryland lucerne pastures on deep sands in the upper South East of South Australia

Smith, Murray V. January 1972 (has links) (PDF)
Bibliography: p. 219-237.
63

Shaking Table Tests to Study the Influence of Ground Motion, Soil and Site Parameters on the Initiation of Liquefaction in Sands

Varghese, Renjitha Mary January 2014 (has links) (PDF)
Liquefaction is a phenomenon in which soil loses a large percentage of its shear resistance due to increased pore water pressure and flows like a liquid. Undrained cyclic loading conditions during earthquakes cause liquefaction of soils, which can lead to catastrophic failures such as bearing capacity failures, slope failures and lateral spreads. The concepts and mechanisms of liquefaction were studied extensively by many researchers. Though the factors affecting the liquefaction response of soils during earthquakes are well documented in literature, there are still some gray areas in understanding the individual and combined effects of factors like frequency, gradation, fines content and surcharge pressure on the initiation of liquefaction. The objective of this thesis is to study the influence of ground motion, soil and site parameters on the initiation of liquefaction in saturated sand beds through laboratory shaking table model tests and numerical studies. Shaking table tests are carried out using a uniaxial shaking table on sand beds of 600 mm thickness. The initiation of liquefaction was observed and identified by measuring the pore water pressure developed during the sinusoidal cyclic loading. Free field liquefaction studies are carried out on sand beds to study the influence of ground motion parameters, namely, input acceleration and frequency of shaking on liquefaction. These studies revealed that acceleration is one of the important parameters that can affect the initiation of liquefaction in sands. Increase in acceleration reduces the liquefaction resistance of sand and a small increase in acceleration can trigger liquefaction. Frequency of shaking did not affect the initiation of liquefaction at lower frequencies but a threshold frequency which triggered instant increase in the excess pore pressures is observed. Liquefaction caused slight initial amplification followed by de-amplification of accelerations due to the stiffness reduction in soils during liquefaction, the effect being more pronounced in the top layers of the sand bed. Pore water pressure ratios during dynamic loading decreased with depth below the surface of the sand bed due to the low initial effective vertical stress and upward transmission of pore pressure during undrained loading. Shaking table tests are carried out to study the influence of soil parameters such as relative density, thickness of dry overlying sand layer and gradation. Relative density of sand can influence the liquefaction potential of sand to a great extent, about 10% increase in relative density bringing down the probability of liquefaction by about 50%. With the increase in height of dry overlying sand layer, liquefaction potential has decreased nonlinearly. Change in grain size altered the pattern of liquefaction and pore pressure development and it is observed that the liquefaction in finer sands is influenced by the frequency of shaking to a larger extent. Surcharge pressure from building loads increased the liquefaction potential and heavier structures got liquefied at lower pore water pressure ratios. Significant post-liquefaction de-amplification was observed in sand beds with surcharge pressure. Parametric numerical analyses are carried out using finite difference program FLAC (Fast Lagrangian Analysis of Continua) with FINN model to measure pore water pressures in the sand bed. Results from numerical analyses with change in the acceleration, surcharge pressure and thickness of dry overlying layer agreed well with the experimental results. However, effect of frequency in numerical studies did not match with the experimental observations, because of the inherent boundary effects in the experimental models. Results from this thesis provided important insights into the development of pore water pressures in sand beds during cyclic loading events, apart from enhancing the understanding towards the effect of various ground motion, site and soil parameters on the initiation of liquefaction in sand beds.
64

[en] INFLUENCE OF ADDITION OF BUTADIENE COPOLYMER AND MODIFIED STYRENE ON THE MECHANICAL BEHAVIOR OF A SAND / [pt] INFLUÊNCIA DA ADIÇÃO DE COPOLÍMERO DE BUTADIENO E ESTIRENO MODIFICADO NO COMPORTAMENTO MECÂNICO DE UMA AREIA

THIAGO MANES BARRETO 19 May 2021 (has links)
[pt] O estudo avalia o comportamento mecânico de uma areia reforçada com polímero, em comparação à areia pura. Foram realizados ensaios cisalhamento direto em amostras de areia pura e desta com a adição do copolímero de butadieno e estireno modificado (XSBR). O copolímero de butadieno e estireno é um elastômero composto de aproximadamente 75 porcento de butadieno e 25 porcento de estireno, presente em solução aquosa, sendo muito utilizada na indústria automobilística, para a produção de pneus. Pode ser produzido a partir dos processos de polimerização em emulsão ou polimerização em solução. A escolha destes materiais está relacionada às suas propriedades serem compatíveis as exigências para melhoramento de solos em obras geotécnicas. As amostras de areia com polímero apresentavam 50 porcento de densidade relativa, 10 porcento de umidade, nas proporções em volume água-polímero de 1:1, 1:2 e 1:4, sem tempo de cura, ou com tempos de cura de 24, 48, 72, 96, 576, 720 e 1080 horas. Foram constatadas melhorias nos parâmetros de resistência das amostras de areia com adição de polímero, em comparação aos parâmetros da areia pura, mostrando que a melhoria de solos com polímero é satisfatória para a aplicação em obras geotécnicas, como por exemplo: aterros sobre solos moles, solos de fundações superficiais e para a estabilidade de taludes. / [en] The study evaluates the mechanical behavior of a sand reinforced with polymer compared to pure sand. Direct-cut tests were carried out on pure sand samples and with the addition of modified styrene butadiene-styrene (XSBR) copolymer. The copolymer of butadiene and styrene is an elastomer composed of approximately 75 percent butadiene and 25 percent styrene, purchased in aqueous solution, being widely used in the automotive industry for the production of tires. It may be produced from the emulsion polymerization or solution polymerization processes. The choice of these materials is related to their properties being compatible the requirements for soil improvement in geotechnical works. Polymer sand samples had 50 percent relative density, 10% moisture, in water-polymer volume ratios of 1:1, 1:2 and 1:4, without curing time, or with times of cure 24, 48, 72, 96, 576, 720 and 1080 hours. Improvements in the resistance parameters of the sand samples with polymer addition were verified in comparison to the pure sand parameters, showing that the improvement of soils with polymers is satisfactory for the application in geotechnical works, such as: landfills on soft soils, soils of shallow foundations and for slope stability.
65

Treibhausgasminderung auf Sandböden: Potenziale in verschiedenen Nutzungssystemen

Klepatzki, Julian 15 December 2017 (has links)
Die Ergebnisse aus den beiden Dauerfeldversuchen verdeutlichen, dass die mineralische N Düngung wie erwartet den größten Einfluss auf die Höhe der THG Emissionen hat. Die höchsten THG Minderungspotenziale zeigten sich folglich in der Reduktion der mineralischen N Düngung, insbesondere wenn die N Düngung oberhalb des standortspezifischen Ertragsoptimums liegt. Die Anpassung der Fruchtfolge kann zur Erhöhung der Bodenkohlenstoff-Vorräte beitragen und letztendlich die THG Emissionen mindern, allerdings bedarf diese These weiterer Untersuchungen. Die Ergebnisse haben weiterhin gezeigt, dass mit dem Aufbau organischer Bodensubstanz durch Stalldung erhebliche Potenziale zur THG-Minderung verbunden sind. Je nach methodischem Ansatz zur Berücksichtigung von Bodenkohlenstoff-Veränderungen ergaben sich allerdings große Unterschiede in den THG-Bilanzen und letztendlich auch in den ermittelten THG-Minderungspotenzialen. Die Entwicklung eines einheitlichen wissenschaftlichen Verfahrens zur Berücksichtigung von Bodenkohlenstoff-Veränderungen wird deshalb empfohlen. Die Ergebnisse aus der Fallstudie haben gezeigt, dass die THG Minderung in der landwirtschaftlichen Praxis eine Veränderung der Ackerflächenverhältnisse erfordert. In diesem Zusammenhang ist der Anbau emissionsintensiver Fruchtarten mit einer intensiven mineralischen N Düngung wie beispielsweise Winterraps zu reduzieren und durch den Anbau emissionsarmer Fruchtarten zu ersetzen. Im untersuchten landwirtschaftlichen Betrieb erwiesen sich Mais mit organischer N Düngung sowie der Anbau von Leguminosen als besonders emissionsarm. In der vorliegenden Arbeit konnte darüber hinaus gezeigt werden, dass ein positiver Beitrag der ackerbaulichen Bodennutzung zur THG Minderung nicht zwangsläufig mit höheren Kosten für den Landwirtschaftsbetrieb verbunden sein muss, wenn bei der betriebswirtschaftlichen Optimierung die THG Emissionen angebauter Fruchtarten berücksichtigt werden. / The aim of this study was to analyze the potential for reducing greenhouse gas (GHG) emissions in different land use systems on sandy soils in the Brandenburg region in Germany, based on two long-term field experiments at Thyrow and Groß Kreutz and an on farm case study. The calculations of the GHG balances are based on the LCA standard and the German emission report guidelines. There is currently no scientific consensus on how soil organic carbon changes are to be included in GHG balances. Therefore, different approaches to include soil organic carbon changes in GHG calculations from long-term field experiments were examined. The results of the long-term field experiments showed that mineral nitrogen fertilization had the greatest influence on GHG emissions. The reduction of mineral nitrogen fertilization consequently showed the biggest GHG reduction potential especially if nitrogen fertilization was above the local level. The adaptation of crop rotations may increase soil organic carbon content and thereby mitigate GHG emissions, but this hypothesis requires further research. An increase of soil organic carbon stocks by organic fertilization was shown for the use of farmyard manure. Although this had a high GHG reduction potential, there were large differences between the analytical approaches. This highlights the need to develop standardized scientific methods for assessing GHG emissions from cropping systems. The results of the case study showed that changing the proportions of different crop species can be used for GHG reduction. In particular, the reduction of crops with high mineral nitrogen demand, e.g. oilseed rape, and the substitution with crops having low GHG emissions is recommended. Maize, receiving high rates of organic fertilizer, as well as legumes showed low GHG emissions on the evaluated farm. Furthermore, this study elaborates the potential economic benefit for agricultural enterprises with regards to the correlation of GHG reduction and an optimized crop rotation.
66

Interference Effects On The Collapse Loads For Footings And Anchors Using An Upper Bound Finite Element Limit Analysis

Kouzer, K M 04 1900 (has links)
The present thesis is an attempt to investigate the interference effects on the magnitudes of the ultimate failure loads for a group of closely spaced strip footings and strip plate anchors. On account of an increase in the number of different civil engineering structures, footings and anchors are often need to be placed very close to each other. In such a situation, the ultimate bearing capacity/pullout capacity of an interfering footing/anchor becomes significantly different from that of a single isolated footing/anchor. The effect of interference on the magnitude of failure load is usually expressed in terms of an efficiency factor (%y); where £,y is defined as the ratio of the magnitude of the failure load for a strip footing/anchor of a given width in the presence of other footings/anchors to that of the magnitude of the failure load for an isolated single strip footing/anchor having exactly the same width. No rigorous analysis seems to have been carried out so far in literature to investigate the interference effect for a group of footings and anchors. In the present study, it is intended to use rigorous numerical upper bound limit analysis in combination with finite elements and linear programming in order to determine the collapse loads for the problems of both isolated and a group of footings and anchors. Three noded triangular elements are used throughout the thesis for carrying out the analysis for different problems. The velocity discontinuities are employed along the interfaces of all the elements. The plastic strains within the elements are incorporated by using an associated flow rule. The Mohr Coulomb yield surface is linearised by means of an exterior regular polygon circumscribing the actual failure surface so that the finite element formulation leads to a linear programming problem. In solving the different problems taken in this thesis, computer programs were developed using 'MATLAB' with the usage of 'LINPROG' - a library subprogram for doing the necessary optimization. The bearing capacity factor Ny for an isolated single rigid strip footing placed on a cohesionless ground surface has been computed and its variation with respect to the footing-soil roughness angle (8) has been examined in detail. It is clearly noted that an increase in 8 leads to a continuous increase in Ny. The solution is also obtained for a perfectly rough footing without considering any velocity discontinuity surface along the footing-soil interface. With 5 = <|), the magnitude of NY becomes almost the same as that for a perfectly rough footing. The size of the plastic zone increases with an increase in the values of 8 and <j). The obtained values of Ny for 5=0 and § compare quite favorably with the solutions reported earlier in literature. The ultimate bearing capacity for a group of two and an infinite number of multiple interfering rough strip footings placed on a cohesionless medium has been computed; all the footings are assumed to be perfectly rigid. It is specified that the footings are loaded simultaneously to failure exactly at the same magnitude of the failure load. For different clear spacing (S) between the adjacent footings, the magnitude of the efficiency factor (£,y) is determined. In the case of two footings, the value of E,y at S/B = 0 becomes exactly equal to 2.0, and the maximum ^occurs at a critical spacing (Scr). For S/B < Sor/B, the ultimate bearing pressure for a footing becomes equal to that of an isolated footing having the width (2B+S), and the ground mass encompassed between the two footings deforms mainly in the downward direction. In contrast, for S/B > Scr/B, ground heave is noticed along both the sides of the footing. As compared to the available theories in literature, the analysis presented in this thesis provides generally lower values of ^y for S/B > Scr/B. ' In the case of a group of multiple strip footings, the value of £y is found to increase continuously with a decrease in S/B. The effect of the variation of spacing on §y is found to be very extensive for small values of S/B; the magnitude of ^y approaches infinity at S/B = 0. For all the values of S/B ground heave is invariably observed on both the sides of the footings. The magnitudes of ^Y for given values of S/B and <|) for the two footings case are found to be smaller than the multiple footings case. The vertical uplift capacity of an isolated strip anchor embedded horizontally at shallow depths in sand has been examined; the anchor plate is assumed to be perfectly rigid and rough. The collapse load is expressed in terms of a non-dimensional uplift factor FY, the value of which needs to be known before calculating the failure load for an interfering anchor. The magnitude of Fr is found to increase continuously with increase in both embedment ratio (k) and the friction angle (<|>) of sand. Even though the analysis considers the development of plastic strain within all elements, however, at collapse, the soil mass just above the anchor is found to move as a single rigid block bounded by planar rupture surfaces; the rupture surfaces emerging from the anchor edges are seen to make approximately an angle <|> with the vertical. The vertical uplift capacity of a group of two and an infinite number of multiple interfering rigid rough strip anchors embedded horizontally in sand at shallow depths has been examined. At collapse, it is specified that all the anchors in the group are loaded to failure simultaneously exactly at the same magnitude of the failure load. For different clear spacing (S) between the anchors, the magnitude of the efficiency factor (£Y) is determined. On account of interference, the magnitude of 4y is found to reduce continuously with a decrease in the spacing between the anchors. For all values of X and §, the magnitude of ^y for the multiple anchors case is found to be always smaller than that for the two anchors case. In contrast to a group of footings under compression, the magnitude of ^v for a group of anchors is found to decrease invariably with an increase in $ for a given value of S/B. For S > 2c/tan<j) , the uplift resistance of anchors in the group becomes equal to that of an isolated anchor, and no interference is seen to exist; where d is the depth of anchor. By examining the nodal velocity patterns, it was noted that in the event of collapse, a wedge of soil mass just above the anchors and encompassed within linear rupture surfaces moves vertically upward almost as a single rigid unit with the velocity same as that of the anchor plate itself. On this basis, a closed form solution of the problem has been developed. The results from the closed form solution for the group of two anchors as well as for multiple anchors are found to provide an excellent comparison with the rigorous upper bound numerical solution especially for the value of § greater than or equal to about 35°. For all the problems taken in this study, it has been seen that an upper bound limit analysis in combination with finite elements and linear programming is a very useful numerical tool for determining the magnitudes of collapse loads.

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