“nanotechnology a new way of looking at paper ......interesting materials are formed by nature •...

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Phil Jones Director Technical Marketing & New Ventures Source B Gibson 2002 “NANOTECHNOLOGY A New Way of Looking at Paper Coating Pigments and Coating Structures” “NANOTECHNOLOGY A New Way of Looking at Paper Coating Pigments and Coating Structures”

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  • Phil JonesDirector Technical Marketing & New Ventures

    Source B Gibson2002

    “NANOTECHNOLOGYA New Way of Looking

    at Paper CoatingPigments and

    Coating Structures”

    “NANOTECHNOLOGYA New Way of Looking

    at Paper CoatingPigments and

    Coating Structures”

  • Interesting materials are Formed by Nature

    • Deposits of white kaolin lie close to the surface

    • They were valuable enough to be dug out by hand

    Source: Ries 1914

  • 100

    Year

    1950

    Impa

    ct o

    n So

    ciet

    y

    1970 1990 2010 2030 2050 2070

    Nanotechnology,“The Next Industrial Revolution”

    Dr. R. Siegel,

    0

    Solid State Technology

    Biotechnology

    Nanotechnology

    Source: ten Wold 1998

    Nanotechnology 1 to 100 nm

  • Why Nanotechnology?

    • Less space, faster, less material, and less energy

    • Novel properties and phenomena• Most efficient length scale for

    manufacturing• Intersection of living/non-living

    Source: G McCarty 2003

  • Areas of Nano-technology• Thermal Barriers• Gas / Vapour Barriers• Optical (Vis/UV) Barriers• Information Recording Layers• Molecular Sieves• Absorption/desorption materials• High Hardness Tools• Nano-composite Cements

  • Assembly:Colloid Chemistry

    Atoms

    nanoparticles layers

    nanostructures

    Dispersions andcoatings

    assembly

    “building blocks”

    High surfacearea materials

    Functionalnanodevices

    Consolidated materials

    synthesis

    Source: Siegel 1999

  • Bio-mimetic Processes Leveraging Bio-Technology:Photonics : Meta-Materials

    Source: Belcher et al 1999

    Source: Busch & John 2000

    Light interacts with features similar in size with its wavelength

    Photonics Developing New Materials to interact with Light in PreciseWays

    Source Sambles 2001

    InverseOpal

  • Self -cleaning Surfaces:

    The Lotus LeafEffect

  • Paper Markets

    • Advertising– Magazine– Catalogue– Inserts

    • Information– Computer output;– ink-jet, EP– Digital Photography

    • Packaging– Point of Sale advertising

    © Hannah Jones 2001

  • Suprastar

    Coated Paper Surfaces

    Capim DG

    Carbital 95

    Opti-Gloss

    Higher SurfacePorosity

    Higher SurfacePorosity

    Slower Setting

    Slower Setting

  • Source: R Wygant 1999

    The Way That Light Interacts with the Surface Determines Appearance

    Atomic ForceMicroscopyImage ofPaper Surface

    Specular, Diffuse, Angular variation

  • suminagashi

  • The way that light interacts with the surface determines appearance

    • Specular• Diffuse• Angular variation

    Source: Quinteros 1999

  • Gloss vs Surface Roughness

    0102030405060708090

    100

    0 0.1 0.2 0.3 0.4 0.5 0.6

    Roughness micron

    Tapp

    i Glo

    ss

    20deg45deg60deg75deg85deg

    Source D I Lee, 1986 Tappi Coating Conference

    0.1 micron = 100 nm

  • clay +10 pphSBR latex

    Prepared cryogenicallyfor SEM

    Wetstate

    In order to bind, latex particles need to form a film

  • clay +10 pphSBR latex

    Prepared cryogenicallyfor SEM

    Wetstate

    Air-drystate

    In order to bind, latex particles need to form a film

  • 90

    80

    70

    60

    50

    40

    Drying Time

    75

    oG

    loss

    or

    Ref

    l ect

    a nce

    Ro

    75o Gloss

    Ro

    Source Lepoutre 1985

  • 75

    oG

    los s

    or

    Re f

    lect

    a nce

    Ro

    Solids volume % Concentration

    100

    90

    80

    70

    60

    50

    40

    3040 50 60 70 80 90 100

    Ro

    75o Wet Gloss

    GlossFreeze Dried

    FCC

    SCC

    Source Lepoutre 1985

  • Fundamentals of Print GlossInk Setting and Levelling

    Ink Setting

    • Fast Setting allows less levelling and hence lower ink gloss

    • Fast Setting is given by– Large pores

    – High pore volume

    – Low tortuosityblocky pigment platey pigment

    ‘ink bottle’ pore pore junction

    0100200300400500600700800

    0 30 60 90 120 150 180 210

    Time after Printing ( Seconds )

    Max

    Sep

    arat

    ion

    Forc

    e--

    ----

    ----

    ->

    Fastest SettingSlowest Setting

    FastSlow

    Ink Surface

    Source: J Preston 1999

  • • Characterization Techniques from micro-electronics Industry have improved knowledge of pigment structures– Atomic Force Microscopy– Field-Emission

    Scanning Electron-Microscopy– Mercury Porosimetry– Microcalorimetry

    Pigment StructurePigment Structure

    © Hannah Jones 1999

  • Minerals are Now Produced in Refineries: Selecting Shapes and Sizes

    • Major Kaolin Crude Sources– U K – Georgia– Brazil

    • Calcium Carbonates – Merchant Plants

    • Ground Calcium Carbonates– Satellite Plants

    • Ground Calcium Carbonates• Precipitated Calcium Carbonates

    • Delamination/Grinding (Cracking)• Particle Size Selection (Distillation)• Precipitation (Synthesis)• Aggregation (Polymerization)

  • A range of products is made from a kaolin feedstock

    • Finer particle size gives higher gloss

    • Fine blocky particles give lower ink gloss

    • Fine Platey particles give higher ink gloss

    • Delaminated made from coarse residues and is very platey

    0

    10

    20

    30

    40

    50

    60

    70

    80

    90

    100

    110EQUIVALENT SPERICAL DIAMETER, MICRONS

    WT

    % F

    INER

    TH

    AN

    FeedFine #1#1#2Delaminated

  • Fb

    Fg

    gFv

    ρ2

    ρ1

    s

    Rsρ2= density of solid

    Fb = Bouyancy Force

    Fg = Force due to Gravity

    S = velocity of particle

    g = gravitational constant

    ρ1= density of liquid

    Fnet = Fg- Fb = V( ρ2-ρ1)g

    Fnet = (4/3)πR3( ρ2-ρ1)g

    R = ( )9 ηs 2(ρ2-ρ1)g 1/2 Stokes’ Law

    η = viscosity of liquid

    s = terminal velocity of particleρ = density

    g2R2( ρ2-ρ1)9 ηS =

  • ESD: Equivalent Spherical Diameter

    C JPEJ 2000O

  • The TEM shadowing techniqueThe TEM shadowing techniqueFor a given shadow angle, particle thickness (t) is proportional to shadow length (l)

    Example TEM image

    Pt-C vapour coating

    Particle Shadow

    Source: J Husband 2002

  • 0.05

    0.4

    1

    1.6

    2.2

    60

    120

    180

    0

    20

    40

    60

    80

    100

    Nano-Mineral Sizes and Shapes

    0

    5

    10

    15

    20

    25

    30

    0 20 40 60 80 100 120 140 160 180 200 220Crystal Thickness Nanometers

    Num

    ber

    Mine C

    Mine AMine B

    Crystal Thickness

    Shape & Size Distribution

    Diametermicron Thickness

    nm

    Source: R Pruett 1997

    Source Golley & Dover 1989

  • Calculating disc diameter from esd and shape factor measurements

    d

    t

    SF = dt

    esdd = [2.356SF ]0.5**Jennings & ParslowSource J Husband 1997

  • Measurement of esd does not discriminate between delamination and transverse fracture

    3.0 µm1.5 µm

    SF = 20:1 SF = 10 : 1esd = 0.84 µm esd = 0.60 µm

    OR

    SF = 40 : 1

    esd = 0.60 µm

    3.0 µm

    Source J Husband 1997

  • Diameter

    1

    2

    3

    4

    5

    0 10 20 30 40 50 60

    Aspect Ratio (L/t)

    Dia

    met

    er (L

    , µm

    )

    t

    Thickness

    00.10.20.3

    0.40.50.6

    0 10 20 30 40 50 60

    Aspect Ratio (L/t)

    Thi

    ckne

    ss (t

    , µm

    )Disc Diameter and Thickness

    L

    1 1 µµm e.s.d. Discm e.s.d. Disc

    A given e.s.d. measured by SediGraphTM can refer to very different particles.

    Source J Husband 1997

  • % < 2 μ

    Mean ESD μ

    ShapeFactor

    Diameterμ

    Thickness nm

    Ultra-FineGlossing

    98 0.2 5 0.29 58

    Ultra-FinePlatey

    98 0.2 45 0.89 19

    #2 Clay 80 0.4 10 0.82 82

    Delaminated 80 0.55 30 1.96 65

    Capim DG 90 0.51 12 1.15 96

    Contour1500

    90 0.5 60 2.52 42

    Hyperplatey 50 2.0 100 13.0 130

    Sedigraph measurements are not the whole story

  • 40

    45

    50

    55

    4 5 6 7 8Coat weight gsm

    Cal

    ende

    red

    glos

    sSuper Platey60:1

    Standard delaminated30:1

    +8units

    Super Platey Clay in 30# offset formulation

    Source: Husband: 1999

  • 0.5

    0.75

    1

    1.25

    4 5 6 7 8Coat weight gsm

    Park

    er P

    rint S

    urf S

    moo

    thne

    ss,

    µm

    Super Platey60:1

    Standard delaminated30:1

    1.8 gsm

    Super Platey Clay in 30# offset formulation

    Source: Husband: 1999

  • Effect of particle shape on mechanical properties : tensile index of kaolin / GCC (C90) blends

    High shape factor clays increase tensile strength in blends with GCC. 20pph XP increases tensile by 0.55 Nmg-1 cf. 20 pph Alphalux. This is the same as 5 pph latex (see next slide).

    R2 = 0.8522

    R2 = 0.9581

    0.001.002.003.004.005.006.007.008.00

    0 20 40 60 80 100% kaolin

    Tens

    ile s

    tren

    gth

    M P

    a Fine platey

    Fine blocky

    12 pph latex, 0.3 pph CMC. Coatings made on plastic film, peeled off and tensile strength measured. Average of 13-18 measurements / sample.

  • • Self Assembly of building blocks– Optical performance– Ink interactions– Blister Resistance– Dot Shape– Water uptake in Ink-jet– Thermal Barrier for EP

    Selection of Shapes and Sizes Building Functional Performance

    Selection of Shapes and Sizes Building Functional Performance

  • Particles and Pores of similar size as wavelength of light

    Light of Similar Wavelength as objectLight of Similar Wavelength as object

    Light of Similar Wavelength as PoreLight of Similar Wavelength as Pore

    Light is diffracted and scattered by

    small objects

  • Control of Pore Size and Volume

    Blending enables a wide range of pores structures to be developed enabling balance between optics, print snap and blister resistance and dewatering to be changed

    Blending enables a wide range of pores structures to be developed enabling balance between optics, print snap and blister resistance and dewatering to be changed

    0

    20

    40

    60

    80

    100

    120

    140

    160

    0 10 20 30 40 50 60 70

    Pore Volume cc/kg

    BlendsUK ClayUS ClayBraz ClayGCCPCC

    Bubble Size refers to relative Pore Density

  • Brightness and Print Gloss with Pigment Blends

    70

    71

    72

    73

    74

    75

    76

    50 55 60 65 70 75 80Print Gloss 75°

    Shee

    t Brig

    htne

    ss IS

    O

    StandardBlends

    EngineeredBlends

    OptimisedSolutions

    HelicoaterTM Data, 1000m/min, Latex/CMC FormulationData refers to PCC/GCC + US/Brazilian/UK kaolins

    Standard Clay-Carbonate blends trade brightness and print gloss.Certain, but not all, Engineered pigment blends offer step changes in

    brightness while maintaining high print gloss.

    Standard Clay-Carbonate blends trade brightness and print gloss.Certain, but not all, Engineered pigment blends offer step changes in

    brightness while maintaining high print gloss.

    Optimised Solutions

    Opti-Print PCC

  • Brightness v Opacity with Pigment Blends

    70

    71

    72

    73

    74

    75

    76

    83.5 84.5 85.5 86.5 87.5Opacity

    B'n

    ess

    Kaolins

    Carbonates

    Standard Blends

    Engineered Blends

    Optimised Solutions

    Optimised Solutions

  • 0

    0.2

    0.4

    0.6

    0.8

    1

    0 0.1 0.2 0.3Filler volume fraction

    Rel

    ativ

    e Pe

    rmea

    bilit

    y (P

    /Po)

    SpheresCylindersPlates A.R. 30 Plates A.R. 100

    Platy Minerals as a Barrier MaterialCussler et al. J. Membrane Sci. 231, 1-12

  • Barrier Formulation (3- European Project)• RC-latex used in existing Imerys benchmarking experiment

    •50% solids•final coatweight: 10-12 gsm

    0

    50

    100

    150

    200

    250

    Paper latex only latex + filler

    MVT

    R (g

    /m2d

    ay)

  • Pore Structure the Drive