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Download the book, free !! contact roman@gatech.edu, also available in paperback from Amazon
Download the book, free !! contact roman@gatech.edu, also available - - PowerPoint PPT Presentation
Download the book, free !! contact roman@gatech.edu, also available in paperback from Amazon 1 Renewable Bioproducts Institute (formerly IPST) Georgia Institute of Technology 50 10th St. N.W., Atlanta, Georgia, U.S.A. 2 In this talk, well
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Download the book, free !! contact roman@gatech.edu, also available in paperback from Amazon
Renewable Bioproducts Institute (formerly IPST) Georgia Institute of Technology 50 10th St. N.W., Atlanta, Georgia, U.S.A.
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Paper can be thought of a conglomeration of pine straw clumps on a millimeter scale , paper is thus inherently non-uniform . In cross section, paper is a stack of tubes, many are collapsed.
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Laser confocal shot, torn edge 40 X Same as left but lighting up a single layer Paper as a mass of fettucine ! Same paper but a different spot
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at 20% RH
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π»πππππππππ% πΊπ° = π»πππππππ (%π΅) Γ %π΅ Γ . ππ + π. ππ When conditioning samples takes too long , for intra-lab comparison of specs and reproducibility , use the correction:
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Variability increases when testing pieces on a smaller scale e.g. SCT vs RCT, or 15 mm wide strips vs 25 mm wide strips. Samples taken from Front or Back positions show greater CD variation than those near the Center
Load cell measures F
Cross head moves down distance βl
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Define tensile stiffness Sb , using values from the tensile test:
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F
Ξ
πΉππΈ,π·πΈ Γ π’ = ππππΈ,π·πΈ πππΈ,π·πΈ = βπππΈ,π·πΈ πππΈ,π·πΈ πππΈ,π·πΈ = βπΊ
ππΈ,π·πΈ
1) For both MD and CD orientation, where t is the sheet βcaliperβ*, tensile stiffness Sb: 2) Defining strain Ξ΅ : 3) Stress Ο, is Force/Area 4) Hookeβs law
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strength T (Page equation) and compression stress Ο (Shallhorn Gurnagul)
1 ππ = π ππ + π·π₯ 2π½πΉ
ππ’3
ππ π β 1
2
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~ Β± 12 % about Control Page and Seth experiments 1981
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Pin adhesion test
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So, D can be checked using Sb and t
βSandwichβ beam approximation:
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= C(ECT)3/4 {(EMDth2/2 x ECDth2/2)1/2}1/4 x Z1/2 = Cβ(ECT)3/4 (E x t) ΒΌ (h x Z)1/2
Usual simplified McKee equation
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ππ = πΉπ’ = ππ2 π’ = πΎ π’ π2 π’ = πΎπ2
Ο β density = Basis weight/caliper = Ξ²/t V2 β sound velocity squared aka βspecific stiffnessβ Tensile stiffness is related to specific stiffness:
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V2
A proposed βMcKeeβ equation for RCT: Buckling load for a cylinder: Model for RCT:
The data fit:
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Ultrasonic Tensile Stiffness Ξ²V2 (N/mm) x 103
CMT
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Bristow wheel emulating handwriting Applying a swath of aqueous ink Top printed side Bottom unprinted side
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βπ = π΄π
β β π΄π β π + ππ β β ππ β π + ππ β β ππ β π
ΞE = a1x1 + a2x2 + ...+ anxn + b
Underside show-through Tappi method colorimeter CIE L*a*b* values Show-though quantified as difference in unprinted and printed: Seek a regression predictive model of the form:
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Contact Angle Cobb water absorption Air permeability Surface roughness (stylus)
Hercules size (HST)
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ΞE = - 0.0312 x (HST) + 0.170 x (contact angle) + 2.60 x (angle rate) + 7.86 x (Cobb30/Ξ²) -10.3
β Compression and Tension strengths β Burst β Bending stiffness
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E is key Itβs the modulus, you see It is there, for you and me Itβs good for tension Nice for compression, And deserves, your attention !
Thank you for your Attention !! Questions, Comments, to: ο¨ Roman@gatech.edu