peru 3d character xmt 2012

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    3D Characterization, Analysis and

    Simulation of Multiphase Particulate

    Systems in Mineral Processing Using X-ray Computed Tomography

    J.D. Miller

    Chair and Ivor Thomas Distinguished Professor

    Department of Metallurgical EngineeringCollege of Mines and Earth Sciences

    University of Utah

    Lima, Peru, October 2012

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    Development of X-ray Tomography

    Instrumentation Development Year Resolution

    Milli Scanner Translate/Rotate, 1st - 6th

    generation, Medical field

    1971- ~ 1 mm

    Micro Scanner Algorithm,

    Microfocus X-ray source

    Cone Beam Geometry

    1984

    1995- ~10 mm

    HR Micro

    Scanner

    Improved detector,

    Advanced X-ray optics

    2000s ~1 mm

    Nano Scanner Monochromatic source,

    Higher photon flux

    2010s ~50 nm

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    X-Ray Tube

    Imaging

    Detector

    X-Ray Beam

    Specimen

    Positioning

    Stage

    Cone Beam MicroCT - Installed 2000

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    Early Applications of X-ray

    Tomography in Mineral Processing

    1987 Sedimentation and Flocculation Somasundaran et al.

    Powder Technology

    1990 Applications in Mineral Processing Miller, Lin, Cortes

    Miner. Process. &Extrac. Metal. Review

    1991 Coal Washability Lin et al.

    Coal Preparation

    1996 Swirl Flow in ASH Flotation Das and Miller,IJMP

    1996 Cone Beam Microtomography for

    3D Mineral Liberation Analysis

    Lin and Miller,

    IJMP

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    Research Group at the University of Utah,~2008

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    Multiphase Particulate Systems

    X-ray Computed Tomography (CT)

    The analysis of individual particles

    with spatial resolution in 3D has been

    difficult. Only recently have we beenable to spatially resolve particle size,

    shape, and composition in 3D using x-

    ray tomography.

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    Projection

    3D View

    Slice

    Views

    Conventional

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    Phase Differentiation by X-Ray CT

    Mineral

    Name

    Formula Mass Density

    (g/cm3)m (cm

    -1)

    Quartz

    Calcite

    MagnetiteRutile

    SiO2CaCO3

    Fe3O4TiO2

    2.65

    2.71

    5.204.25

    0.448

    0.530

    1.6200.955

    2.3

    8.3

    .E

    bZam

    i

    ii ZfZ8.38.3

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    Particle Properties

    Geometric Features - Size,Shape, Surface Area

    Density, Porosity, DamageCompositionExposure,

    Texture, Liberation

    Pore Network Structures

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    High Resolution XMT-Installed 2009

    Source Detector

    Sample Stage

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    High Resolution X-ray Micro CT

    Analysis of packed particle beds containing

    as many as 60,000 particles can be

    accomplished in less than 3 hours withspecial software to establish the 3D

    characteristics of each particle in the

    sample population. Such data corresponds

    to 1 Gbyte of tomographic information.

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    Particle Separation (Watershed)Rougher Feed (45x25 mm)

    HRXMT Watershed Segmentation

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    Critical Factors in the Development of High

    Resolution X-ray Tomography Systems

    X-ray Source / Optics

    Detector Sensitivity

    Computer Capacity

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    Mineral Processing Applications

    Comminution

    Exposure/Liberation

    Heap Leaching

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    Comminution

    Damage of Particles in Specified Size ClassFraction of particles with cracks

    Crack density

    Specific crack surface area Grain Boundary Fracture

    Increased liberation

    Loss of interfacial area

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    Damage-Isolation of Crack Surfaces

    (Copper Ore , 2.00x0.85 mm)

    Green

    surface Pink

    cracks + pores

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    Percent of Damaged Particles (4.75x2.00 mm) for

    Different Crushing Methods (voxel resolution = 40 mm)Crushing

    Method

    Extent of Damage

    (% of Particles Cracked)

    Oxide Copper

    Ore

    Sulfide Copper

    Ore

    Feed 14 20

    Jaw 14 23

    Low HPGR 37 51

    Medium HPGR 44 69

    High HPGR 79 84

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    Nano CT Image-Copper Sulfide Ore(0.15x0.038 mm, voxel resolution = 130 nm)

    Crack width = 0.29 mm

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    Grain Boundary Fracture

    Conservation of interfacial area after crushing is

    indicative of trans-granular random breakage. On

    the other hand, if interfacial area is diminished

    after breakage some degree of preferential grain

    boundary fracture has occurred. For completeliberation of all grains after crushing the

    interfacial area goes to zero. Thus the interfacial

    area criterion is an important metric to assess the

    significance of preferential grain boundaryfracture for different breakage conditions.

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    Volume : 8.24 mm3

    Interfacial Area :

    0.2522 mm2/mm3

    Grain Boundary Fracture

    Compression

    +500 mm 500x350 mm 350x250 mm 250x180 mm 180x125 mm

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    Specific Interfacial Area Ratio vs Energy

    Dissipation Rate

    0.5

    0.6

    0.7

    0.8

    0.9

    1.0

    0.0E+00 2.0E-05 4.0E-05 6.0E-05 8.0E-05

    Power (W)

    S

    pecificinterfacia

    larearatio

    (mm

    2/mm

    3)

    Energy Dissipation Rate (W)

    Garcia, Lin, Miller, Minerals Engineering 22 (2009) 236

    243

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    Mineral Processing Applications

    Comminution

    Exposure/Liberation

    Heap Leaching

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    Liberation Limited Grade/Recovery Curves

    0

    10

    20

    30

    40

    50

    60

    70

    80

    90

    100

    0 10 20 30 40 50 60 70 80 90 100

    Recovery (%)

    Grade(%)

    Complete Liberation

    NoLiberation

    Increased

    Liberation

    (Each Particle of Uniform Composition, Grade =20%)

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    Liberation Limited Grade/Recovery Curves

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    Texture Analysis and Flotation Kinetics

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    Mineral Processing Applications

    Comminution

    Exposure/Liberation

    Heap Leaching

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    Heap Leaching

    Zaldvar, Chile

    LeachSoution

    HostRock

    Copper

    Mineral

    Optimization of the Heap

    Leaching recoveries requires abetter understanding of the

    variables involved (exposure,

    permeability, kinetics, etc.)

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    Heap Leaching Research

    Mineral

    Exposure

    Rate of

    Chemical

    Reactions

    Fluid Flow in

    Packed

    Particle Beds

    PSD

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    Mineral Exposure Analysis

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    Exposure vs Particle Size

    Miller et al. Int. J. Miner. Process. 72 (2003) 331340

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    Predicted Copper Recovery from Exposure Analysis

    vs. Results from 1.5 m Column Experiments

    Miller et al. Int. J. Miner. Process. 72 (2003) 331

    340

    Ch i Hi h D i Mi l G i

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    Changes in High Density Mineral Grains

    Lin, Garcia, J.D. Miller Symposium, 2005

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    Leaching - Column Tests

    Input

    Output

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    CT Analysis of Packed Column

    Si l ti f Fl Th h P k d C l

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    Simulation of Flow Through Packed Column

    Using Lattice Boltzmann Model

    Before Column Leaching (full column)

    Sim lation of Flo Thro gh Packed Col mn

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    Simulation of Flow Through Packed Column

    Using Lattice Boltzmann Model

    After Column Leaching (full column)

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    Summary

    Advanced instrumentation and accompanying

    software for x-ray tomography analysis haveallowed for a more complete description of

    multiphase particulate systems so important to

    achieve significant improvements in mineral

    processing technology.

    As a consequence, appropriate education and

    training of young scientists and engineers in this

    area is necessary in order to prepare current studentswith advanced skills for future development and

    applications in our profession.