Presentation 17102014

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    Literature review on the study ofchanges in pore size distributionof clay upon loading

    Jun Kang ChowSupervisor: Prof. YH Wang

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    Interpret the changes in poresize distribution of clay

    during the loading processes.

    Preconsolidation

    SEM MIP

    Loading

    Freeze drying

    Washing

    Adjust properties

    Direct observation(from SEM)

    Measurement (from MIP)+

    Current stage of research(Wang, Y.H. & Xu, D., 2007; Wang, Y.H. & Yu, C.Y.,

    (unpublished)) Sample : Speswhite

    kaolin

    Mechanical responses of kaolinite claydepend on cluster-to-cluster interactions

    rather than particle-to-particle interactions

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    Samples obtained before andafter loading for MIP test arenot identical .Freeze-drying process mayalter the pore sizedistribution of clayspecimens.

    Preconsolidation

    SEM MIP

    Loading

    Freeze drying

    Washing

    Adjust properties

    Results of MIP test show thatlarger pores reduce in size after

    loading.

    This does not guarantee thepores involved are inter-aggregated pores .

    PROBLEMS ?

    Current stage of research(Wang, Y.H. & Xu, D., 2007)

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    ~ 0.42 m (pore C of pH 4 spec.)~ 0.18 m (pore B of spec. withsalt)

    ~ 1.22 m (pore D of spec. withsalt)

    ~ 0.42 m (pore B of pH 7.8spec.)

    Existence of smaller/larger Types B, C and D pores than thesizes indicated.SEM image shows that particles that form aggregatedassociations can be unevenly arranged, creating larger intra-

    aggregates pores .

    Result of MIP test(Wang, Y.H. & Xu, D., 2007)

    Figure is taken from Wang, Y.H. and Xu, D.(2007)

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    We are unable to observe

    the loading process.

    We are unable to visualize

    how the arrangement of clayfabric is altered due toloading.

    To search the suitable method thatallows the visualization of changes

    in clay fabric arrangement upon

    loading

    HOW?

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    Methods to study pore sizedistribution of clay

    Directobservation

    Measurementtechnique

    Scanning ElectronMicroscope (SEM)EnvironmentalScanning ElectronMicroscope (ESEM)X-ray computedtopography (CTscanning)

    Mercury IntrusionPorosimetry (MIP)Nitrogen sorptionmethod

    Non-polar liquiddesorptionWater-desorption

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    Systematic errors due to:Inappropriate pore model (assuming cylindrical pore model)Variation in surface tension and contact angle

    Measurement of pore size distribution of clay (Lawrence, G.P., 1977; Westermack, S., 2000)

    Mercury intrusionporosimetry

    Nitrogen sorption Non-polar liquiddesorption

    Water desorption

    Measure poresize of ~ 3 nm 200 mMeasure thepressure requiredto force mercuryinto poresErrors due to:distribution ofpore volume andpore collapse

    Carried out atlow temperature(~ -196 C)Able todetermine rangeof pore size ~ 0.3- 300 nm

    Interactionsbetween non-polar liquidsand claysurfaces are

    weakEquilibriumtimes are long

    Most fine-textured soilsshrink andparticlerearrangement

    takes placeStresses onpore wallsduring anincrease insuction cause a

    reduction inpore size

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    A pore system cannot be adequatelycharacterised by the use of only onemethod.Combine both methods to measure thepore size distribution of clay. (Sills, I.D. etal. 1973a, 1974)

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    Technology available

    At this T, only a modest gas pressure isrequired to stabilize water (achieve saturation)

    Method

    Focus

    Type of samples

    Sample Size

    Preparation

    Resolution

    Workingtemperature

    SEM

    Morphology ofmaterials

    Dry samples(Absence of water)

    ~ few mm indiameter

    Freeze-drying &coating of samples

    are required

    ~

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    An electron beam is emittedtowards a conductive sample inhigh vacuum conditions .

    Secondary electrons are releasedfrom the sample, collected bydetector and amplified to producean image.

    The conductive coating of sample(gold) improves the image quality.

    The vacuum ensures the effectiveoperation of the electron gun.

    Working principle of SEM

    (Absence ofwater)

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    Working principle of ESEM When electrons are emitted, theyhave to travel through the ga s .

    Secondary electrons (with lowenergies) have a high collisioncross-section with the gas

    molecules.Ionizing collisions lead to thegeneration of addition daughterelectrons a cascadeamplification . At the same time, positive ions arealso produced.

    These ions drift down towards thesample compensate the chargebuild-up at the surface of insulators.

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    ESEM Quanta 250 FEI NanoCharacterization

    Metals & alloys,magnetic &superconductingmaterials

    Ceramics, composites,plasticsFilms/coatingsGeological materials

    mineralsSoft materials polymers, gels,tissues, plant

    Particle, porousmaterials fibers

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    Application of ESEM Journal Description

    Montes-H, G. et al.(2005) To study the swelling-shrinkage behavior of compactedbentonite submitted to hydration/dehydration conditions

    Vaunat, J. et al. (2007) To study the residual shear strength of a plastic clay(Boom clay) under high suction

    Zhang, G. et al. (2004) To study how Fe oxides alter the soil structure of a

    highly weathered oil alluviumSelvam, A. &Barkdoll, B. (2005)

    To observe changes in clay fabric using ESEM &correlate it to the permeability changes occurring in clay

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    One Sample

    Preparation Stage:WashingAdjusting

    PropertiesPreconsolidation

    Loading

    ESEM

    Varyloading

    Many Samples

    Preconsolidation

    SEM MIP

    Loading

    Freeze drying

    Washing

    Adjust properties

    Future work/Challenge:

    Design of cellDigital imageanalysis