A New Approach to Measuring ERIC in Deinked Papers David Vahey, - - PowerPoint PPT Presentation

a new approach to measuring eric in deinked papers
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A New Approach to Measuring ERIC in Deinked Papers David Vahey, - - PowerPoint PPT Presentation

A New Approach to Measuring ERIC in Deinked Papers David Vahey, J.Y. Zhu and Carl Houtman USDA, Forest Products Laboratory Madison, WI Effective Residual Ink Conc. (ERIC) 950 nm Ink Assumption: At Absorbance 950 nm any absorbance is


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SLIDE 1

A New Approach to Measuring ERIC in Deinked Papers

David Vahey, J.Y. Zhu and Carl Houtman USDA, Forest Products Laboratory Madison, WI

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SLIDE 2

Effective Residual Ink Conc. (ERIC)

200 400 600 800 1000 1200 Wavelength (nm) Absorbance

Paper (x100) Ink

950 nm

Assumption: At 950 nm any absorbance is due to ink

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SLIDE 3

ERIC Uses Near Infrared (950 nm) to Emphasize Ink Absorbers

= Visible Light = Near Infrared (NIR) Ink Dye Lignin NIR Absorption depends mostly on ink concentration

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SLIDE 4

ERIC Measurement

Ro R∞

Single sheet

  • ver a black

cavity Stack of similar sheets

Reflectance at 950 nm using d/0º

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SLIDE 5

Advantages of ERIC Measurement

  • Rapid, commercially available
  • Suitable precision for control actions
  • An improvement over brightness

measurement

– More sensitive to ink – Less sensitive to dyes and lignin

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SLIDE 6

Disadvantages of ERIC Measurement

  • When Ro and R∞ are close, the errors increase
  • Some samples exhibit such low reproducibility

that results become meaningless

  • Sample must be repositioned to take the two

measurements

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SLIDE 7

Goals of the Study

  • Explore the sources of inconsistency in

ERIC measurements

  • Determine the impact of using a different

wavelength and/or geometry (e.g. 750 nm with a UV/Vis spectrophotometer)

  • Develop a preliminary error analysis
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SLIDE 8

Light-Paper Interaction Theory

A* T = % Transmission R = % Reflection A = % Absorption I = 100%, Incident Illumination Conservation of Energy→ 100% = R + T + A

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SLIDE 9

Approximate ERIC calculation

⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ − − × ≈ ) ( 1 100 (ppm) ERIC

2

m kg w T R

w = Basis Weight R = Reflectance fraction T = Transmittance fraction

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SLIDE 10

Standard ERIC Measurement Approach

A* R0 Single Sheet R∞ Thick Stack T = 0 T>0

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SLIDE 11

Kubelka-Munk Theory

I J

x In differential form: dI = -(K+S) I dx + S J dx dJ = -S I dx + (K+S) J dx Gain from scattering I Loss

  • f

J

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SLIDE 12

a bit of mathematics….

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SLIDE 13

Standard ERIC calculations

( )

∞ ∞

− × = R R S ERIC 2 1 100

2

( )

⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − =

∞ ∞ ∞ ∞

R R R R R w R S

2

1 1 ln 1

Problem: ERIC→∞ as Ro/R∞→1

w = basis weight, in kg/m2

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SLIDE 14

ERIC Measurement Problem with Opaque Papers

A* R0 Single Sheet R0/R∞ ≈ 1-R0T2 Thick Stack T ≈ 0

*

~R0T2 ~R0T

R∞

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SLIDE 15

High Opacity Paper

  • With opacity > 97%, Ro and R∞ are very

close, thus the estimate of S is very poor.

  • One possible solution is to use an estimated

value for Savg (near 50 m2/kg for TMP).

  • Another is to base ERIC on R and T

measurements instead of Ro and R∞.

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SLIDE 16

The R and T Method for ERIC

* T = Transmission R = Reflection I = 1, Incident Illumination ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − + − − + − ⋅ − − =

− 2 2 2 2 1 2 2 2 2 2 2

4 ) 1 ( 2 1 sinh 4 ) 1 ( ) 1 ( x 100 R R T T R R T w T R ERIC

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SLIDE 17

Experimental Setup for ERIC by the R and T method

Lamp Chopper Aperture Paper Aperture Moveable Detector for Transmission (T) and Reflection (R) Lens T R Amplifier Oscilloscope

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SLIDE 18

Experimental Samples

  • TMP: 65 g/m2 handsheets from pulp samples with

varying degrees of residual ink.

  • Kraft: 65 g/m2 handsheets from pulp samples with

residual ink from laser printing.

  • Newsprint: 50 g/m2 page from a directory.
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SLIDE 19

Summary of Results

ERIC, by method Opacity Sample 792 693 558 702 96.1 TMP 2 1238 1100 939 1106 98.7 TMP 3 602 504 417 519 94.6 TMP 1 158 149 189 83.2 Kraft 140 127 181 81.7 News Commercial SavgR∞ R0R∞ RT

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SLIDE 20

ERIC Results by Three Different Methods

News Kraft Trial 1 Trial 2 Trial 3 280 560 840 1120 1400 20 40 60 80 100

  • ERIC (ppm)

Opacity ERIC RT RoR sR sR :Technidyne

Sample

Opacity (%)

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SLIDE 21

Typical ERIC values

  • ERIC ≈ 1000 ppm, for newsprint at the start
  • f deinking
  • ERIC ≈ 200-300 ppm for commercial

recycled newsprint

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SLIDE 22

ERIC Error Analysis

200 400 600 800 1000 1200 10 100

RT R0R sR S 50 40 Data

ERIC (ppm) ERIC COV (%)

  • 6

20

  • 40

70

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SLIDE 23

Conclusions

  • ERIC values greater than 800 ppm are prone to

errors with standard RoR∞ method.

  • Use of an estimated scattering coefficient S make

comparisons between different papers difficult.

  • ERIC measurement using R and T

– Requires no assumptions about S. – Becomes increasingly accurate at high ERIC