How Molecular Weight and Branching of Polymers Influences Laser - - PowerPoint PPT Presentation

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How Molecular Weight and Branching of Polymers Influences Laser - - PowerPoint PPT Presentation

How Molecular Weight and Branching of Polymers Influences Laser Sintering Techniques Dr. Bernd Tartsch Malvern Instruments GmbH Rigipsstr. 19, D-71083 Herrenberg Tel: +49-7032-97 770, Fax: +49-7032-97 854 E-Mail: bernd.tartsch@malvern.com,


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SLIDE 1

How Molecular Weight and Branching of Polymers Influences Laser Sintering Techniques

  • Dr. Bernd Tartsch

Malvern Instruments GmbH

  • Rigipsstr. 19, D-71083 Herrenberg

Tel: +49-7032-97 770, Fax: +49-7032-97 854 E-Mail: bernd.tartsch@malvern.com, www.malvern.de

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SLIDE 2

Selective Laser sintering process

Quelle: Wikipedia, Materialgeeza

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SLIDE 3

Laser sintering applications

› Prototyping › Functional tests/build in tests › Small serial production › Interpenetrating parts

Quelle: NW Rapid Manufacturing Quelle: Ebyton Technology Quelle: Rapid Pro

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SLIDE 4

Materials for laser sintering

› Polyamide (modified)

  • high mechanical load capacity
  • temperature resistent (>150 °C)
  • resistent against bases, solvents, etc.

› filled with glass beads or mineral fibers › Other thermoplastic elastomers › Ceramics › Metals

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SLIDE 5
  • 1. Challenge: Adding the next layer of material

› Particle size determines smallest structure size (0,1 mm) › Particle size distribution and shape influences „flow“ of

particles

› Best properties: regular, equi-axed, non-porous particles

Laser diffraction for particle size and size distribution Automated optical particle size characterization system adds shape information

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SLIDE 6
  • 2. Challenge: Recycling of unused material

› Branching of polymer › Degradation of polymer Triple detection size exclusion chromatography

What do we need as an analytical tool?

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SLIDE 7

Why can‘t we use conventional GPC with RI?

Potential branching destroys the relation between molecular weight and retention volume (hydrodynamic radius).

400,000

Elutionsvolumen (mL) Log (Molekulargewicht)

100,000 10,000 Mn, Mw, Mz Mw/Mn

RI-Signalintensität

Ci 400,000

Elutionsvolumen (mL) Log (Molekulargewicht)

100,000 10,000 Mn, Mw, Mz Mw/Mn

RI-Signalintensität

Ci

same Mw different radius

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SLIDE 8

Absolute Molecular Weight by Rayleigh Light Scattering

Rayleigh ratio I/I0 at angle  Weight average molecular weight Scattering function R/R0 (0...1) Concentration Optical constant

  • 2. Virial coefficient

Refractive index of solvent Laser wavelength Avogadro number Refractive index increment R Mw P c K A2 n0 0 NA dn/dc

2 4 2 2

2        dc dn N n K

A

Laser Scattered light at angle  Incident laser intensity

 I0 I

Sample cell

c 2A P M 1 R Kc

2 θ w θ

 

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SLIDE 9

Angular Dependence

Laser Laser 90° 7° Laser Laser 90° 7°

small molecules

radius < 15 nm Pθ = 1 for all θ

large molecules

radius > 15 nm

Pθ = 1 for θ = 0°

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SLIDE 10

Molecular Weight Measurements

25 50 75 100 125 150 175 200 225 Refractive Index (mv) 5 10 15 20 25 Right Angle Light Scattering (mv) 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 Retention Volume (mL) 25 50 75 100 125 150 175 200 225 Refractive Index (mv) 10 20 30 40 50 Right Angle Light Scattering (mv) 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 Retention Volume (mL)

5 times used new PA Mw = 36.200 g/mol PDI = 1,23 Mw = 88.300 g/mol PDI = 1,31

Chromatographic conditions: Eluent: HFIP, 0.05 M K-acetate Columns: 2x I-MBHMW Flow rate: 0,5 ml/min Temperature: 45 °C

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SLIDE 11

What do we need for branching? Zimm-Stockmayer-Theory

M

         (lin) R (br) R g

2 G 2 G

   

 

/ 1

(lin) (br) g

M

        

Light Scattering Viscometer

R ]M [

3 h

 

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SLIDE 12

Rg determination by Rayleigh Light Scattering

Sin2 (/2) Rθ/KC

Intercept = Mw Slope ≈ 0 for Rg < 15 nm => No Rg Slope = Rg 30o 45o 60o 90o 120o 135o 150o

Small molecules < 1/20 laser wavelength

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SLIDE 13

Rh or IV determination using the 4-Capillary Differential Viscometer

Wheatstone bridge concept Max Haney, 1983

IV C DP IP DP sp     2 4  IP

+ -

DP

  • +

GPC IN OUT

Solvent Sample

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SLIDE 14

Calculating the number of branches

  • 1. star branching

2 / 1 2 / 1

9 4 7 1

                

n n

B B g

   

                               1 2 2 ln 2 2 1 6

2 / 1 2 / 1 2 / 1 2 / 1 2 / 1 n n n n n n n

B B B B B B B g

2

2 3 f f g  

  • 2. trifunctional random – monodisperse in molecular weight
  • 3. trifunctional random – polydisperse in molecular weight

Bn ... number of branches f ... number of arms

  • B. H. Zimm, W. H. Stockmayer,,
  • J. Chem. Phys 17, 1301 (1949).
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SLIDE 15

Mark-Houwink-Plot or Branching View

Quelle: Wikipedia, Materialgeeza

Log M Log IV

branched species Linear species g

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SLIDE 16

Mark-Houiwnk-Plot of new and used PA

new 1x used 2x used 5x used

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SLIDE 17

Numeric Results

Samples Mw PDI Branches new 36.200 1,23 Linear reference 1x used 52.400 1,28 1,18 2x used 65.700 1,27 1,43 5x used 88.300 1,31 1,89

 Now the the data can be related with the behaviour

in the laser sintering process and the amount of material that can be mixed with new material can be determined

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SLIDE 18

Summary

› GPC with triple detection provides a tool to determine

the amount of material that can be recycled in a laser sintering process

› Static Light Scattering is necessary in order to

determine the absolute Mw of the branched polymers

› Viscosity detection is necessary in order to measure

branching of the polymers

› In this case, the laser sintering process leads to a

increase in molecular weight due to formation of branched structures.

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SLIDE 19

Thank you for your attention