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Carbon Nanotubes (CNTs)
The Good

                                             The Bad

& the Ugly
        Malcolm Mackley, Anson Ma, Kat Yearsley
    Department of Chemical Engineering and Biotechnology
The Carbon Family
Graphite    Graphene   Diamond          CNT




                                     Carbon Black




                                 2
CNTs; “The Good”
    Super potential properties
     Stiffness
                   CNT        1000 GPa
                     (steel    210 GPa)

     Electrical Conductivity
                     CNT     106 10 S /m
                                   7

                     (Copper 6 107 S /m)

     Thermal Conductivity
                  CNT         3500 W/m
K
                    (Copper    385 W/m
K)                               3
CNTs; “The Bad”
          health risk
              University of Cambridge
             Health and Safety Office
                      HSD060C
                      July 2009


Carbon nanotubes and other insoluble fibrous
nanoparticles that have the potential to become
airborne should be handled under HEPA‡
filtered local exhaust ventilation (LEV).


      ‡ High Efficiency Particulate Air (HEPA)


                                                 4
CNTs; “The Ugly”
  Dispersion




                   5
Dispersion matrix
• Epoxy resin*
  10Pas or 1 Pas SWNT, MWNT

• UV curing acrylic precursor*

• Thermoplastic Polypropylene (PP)
  Nanocyl (Compounding required)

• Agarose/water*
  Carboxyl Methyl Cellulose (CMC )“surfactant” required

• Fuming Sulphuric acid (LCP form)
  Matteo Pasquali ( Rice University, Houston Texas)
                                   * Personal involvement
                                                6
Dispersion devices

   Batch Stirred vessel; design, scale, feed
    protocol*.
   High shear mixer*.
   Ultra sound mixer; Biorupter, Nanorupter*.
   Compounding device (Nanocyl)
   Twin screw extruder (Nanocyl)

                        * Personal involvement
                                                 7
Best method of Mixing ?
   Simple shear

   Extension

   Stretch and Fold or Mixed flow
   “Vibration”



                                     8
MWCNT vs Carbon Black (CB)




0.25 wt% CNT in epoxy             0.25 wt% CB in epoxy




                   Kat Yearsley
                                             9
Optical Observation of
Untreated Multi-Walled CNT
          The Linkam, Cambridge Shear System CSS




                                             10
Microstructure
• Optical Microscope combined with shear cell

• Isotropic CB vs. Anisotropic CNTs

                                           Images Recorded


                           100
        Shear Rate (s-1)




                           10


                           0.5

                                 15 mins         10 s 10 s
                                                  11
0.25% CB in epoxy




                    12
0.25% CNTs




             13
CB after low shear:    CNT after low shear:
Aggregation            Aggregation




Flow                   Flow


CB after high shear:   CNT after high shear:
Disaggregation         Disaggregation & alignment




Flow                   Flow            14
The “Zoo” of CNT Microstructure
                 0 s-1    1 s-1   10 s-1   100 s-1   1000 s-1

I. Untreated
    SWNT



II. Treated
   SWNT




III. Untreated
     MWNT




 IV. Treated
   MWNT


   All at 0.05 wt% conc                       15
Steady Shear (SS) Experiments
                             CB                                     CNT
       1000
     1000                                       1000

        100
      100                                       100              0.4%
                  4%    4%                             0.3%
 η η      10   2%                        η
 (Pa.s)10                                        10 0%0%1%1%2%2%4%4%
Pa.s)          3%                      (Pa.s)            0.2%
               1%
        1 1     2%                                1
                  0%
                   0%                                          0%
      0.10.1                                 0.1
         0.10.1     1 1       10 10       100 0.1
                                        100                    1         10     100
                     Shear Rate (/s)
                   Shear Rate (/s)                            Shear Rate (/s)



                                                                 16
Aggregation/orientation model , Paco Chinesta
      Diffusion equation

      ∂        dρ  ∂            ∂ψ (ρ, n )        ∂ψ (ρ, n )      ∂ 2ψ (ρ, n )
    − ψ (ρ, n )  +     Dr ( n )             − 3vn            + Dn              =0
     ∂ρ        dt  ∂ρ             ∂ρ                ∂n                ∂n 2


       Where
       n is population from n = 0 to n = 1
.
               βα = vd vc         vn = v c − vd               Dn = vd n + vc (1 − n )
                                             ,


                                         Destruction rate due to shear        creation rate
      Constitutive equation


             σ = − p I + 2η D + 2ηN p a : D


                                                                         17
(a) 0.25% CNT                              (b) 0.1% CNT
   1000                                       1000




  ηa 100                                     ηa 100
[Pa.s]                                     [Pa.s]




     10                                         10
           0.1          1             10              0.1          1             10
                  Shear rate [s -1]                                        -1
                                                              Shear rate [s ]

                 (c) 0.05% CNT                              (d) 0.025% CNT
    100                                        100




  ηa 10                                      ηa 10
[Pa.s]                                     [Pa.s]




      1                                           1
           0.1          1             10              0.1           1            10
                  Shear rate [s -1]                          Shear rate [s -1]



                                                                18
CNT Fibre makers


   Pasqualli Group Rice University Houston
   Windle team     Cambridge University




                                   19
Rice University Houston.;
Anson Ma and Matteo Pasquali, Oct 2010




                                         20
TRUE SOLUTIONS OF SWNTs
            1 min                               10 min           60 min




     CNTs dissolve spontaneously
      in chlorosulfonic acid
Davis, Pasquali, et al, Nature Nanotech, 4, 830, 2009
                                                            21
Pasquali et al, US Patent Application under review (2009)
BEHAVIOR AT HIGH CONCENTRATION

                             12% vol SWNT in chlorosulfonic, CROSS POLARS

                 co
                  hi ntra
                   nc
                    gh t
                      e
                       er ion
  ISOTROPIC
CONCENTRATED




                   LIQUID
                 CRYSTALLINE
    analyzer
                     -60
                   -45OOOO
                      -75
                    -30O                                                50 µm
                    0O
                    -15
     polarizer                  Davis, Pasquai, et al, Nature Nanotech, 4, 830, 2009
                                                                22
SPINNING NEAT SWNT FIBERS




Ericson, Pasquali, Smalley, et al., Science, 305, 1447 (2004)
Smalley, Pasquali, et al., US Patent 7,125,502 (2006)
Davis, Pasquali, et al., Nature Nanotech., (2009)
Pasquali et al., patent application under review              23
TYPICAL ACID-SPUN SWNT FIBER



                                                          Ø=37±3µm




                                                            Ø=50±2µm




Sub-optimal mesostructure (bundles), affect transport
Excellent macrostructure                            24
                       Wang, Pasquali, Smalley, et al., Chem. Mater., 17, 6361 (2005)
SPINNING FROM CHLOROSULFONIC ACID
   7 WT% SWNT in chlorosulfonic              7 wt% SWNT in    7 wt% SWNT in
   acid, coagulated in 96% H2SO4             chlorosulfonic   chlorosulfonic
           13 µm                             acid: Solvent    acid, coagulated in
                                             evaporation      dichloromethane




                          30 µ m                  100 µm                              100 µm




                   1 µm                    1 µm                                1 µm



                                   • Smooth, compact fibers
                                       via slow coagulation
                                   • Coagulants: dichloromethane,
                                       chloroform, ether, sulfuric acid (96%)
                                                                       25
                                    Davis, Pasquali, et al, Nature Nanotech, 4, 830, 2009
Carbon Nanotube Fibres and
their Composites

   Alan Windle
       And
      Team

                             acromolecular
                             aterials
                             ab


                 New Museums Site, Pembroke Street
                 Cambridge, CB23QZ, UK
Fibre spinning in furnace
                       H2
                            Ethanol or Hexane
                            Ferrocene 2%
                            Thiophene 0.3%




                                 Nanotube
      1100 - 1300`°C




                                 Smoke

                                                            Its elastic!
                                                            an aerogel
                                  Ya-Li Li, Ian Kinloch and Alan Windle,
                                    Science, 304, p 276, 9 April 2004

                                                27
Department of Materials, Cambridge,


                                         Injection system


                                         Reactor


                                        Gas exchange valve




Fibre collection
                                           28
Continuous wind up with
            drawing (10 - 50 m/min)




n.b. 20m/min at 0.05 tex is only 1mg/min or ~ 1g/day
                                          29
The knot test; (Get Knotted)


                      Tensile strength not
                      degraded by presence
                      of a knot.

                      c.f. For carbon fibre
                      with a knot, strength
                      can be only 10 % of
                      unknotted sample


                               30
Wide angle X-ray of fibre
          ESRF synchrotron source Grenoble




                                 002




   Winding rate = 20 m/min                  Winding rate = 30 m/min

Very good orientation of CNTs, graphitic component
                  Unoriented
                                                       31
but an unoriented component (particles ?)
Carbon nanotube fibre properties

Physical:           Specific Gravity 0.5 – 1.1
                    (Diameter 10 micron)

Mechanical:         Strength            0.5 - 2.3 GPa/SG

                    Stiffness           20 – 80 GPa/SG


Thermal:            Conductivity      50 – 1000 Wm -1K-1


Electrical:          Conductivity        8 x 105 S/m
       (no influence of sample length, but only 1/60 of
copper or 1/8 on a unit mass basis). Mix of metallic and
                                             32
Carbon nanotube fibres



Carbon fibre           Polymer fibres

             Carbon
           A new sort
           Nanotube
            of stuff ?
             Fibres


               Yarns

                                 33
Conclusions

•CNTs (still) have exciting potential.
•Handle with care.
•Dispersion still a challenging problem.

       Next generation
   Composite reinforcement ?
       “Carbon Fibre” ?
                               34
The problem!           Polymers - CNTs




Molecular dynamics simulations of entangled polymers (or maybe CNTs?)
    Prof Aleksei Likhtman (University of Reading)
                                                   35

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CNT Nantes- 2011

  • 1. Carbon Nanotubes (CNTs) The Good The Bad & the Ugly Malcolm Mackley, Anson Ma, Kat Yearsley Department of Chemical Engineering and Biotechnology
  • 2. The Carbon Family Graphite Graphene Diamond CNT Carbon Black 2
  • 3. CNTs; “The Good” Super potential properties Stiffness CNT 1000 GPa (steel 210 GPa) Electrical Conductivity CNT 106 10 S /m 7 (Copper 6 107 S /m) Thermal Conductivity CNT 3500 W/m K (Copper 385 W/m K) 3
  • 4. CNTs; “The Bad” health risk University of Cambridge Health and Safety Office HSD060C July 2009 Carbon nanotubes and other insoluble fibrous nanoparticles that have the potential to become airborne should be handled under HEPA‡ filtered local exhaust ventilation (LEV). ‡ High Efficiency Particulate Air (HEPA) 4
  • 5. CNTs; “The Ugly” Dispersion 5
  • 6. Dispersion matrix • Epoxy resin* 10Pas or 1 Pas SWNT, MWNT • UV curing acrylic precursor* • Thermoplastic Polypropylene (PP) Nanocyl (Compounding required) • Agarose/water* Carboxyl Methyl Cellulose (CMC )“surfactant” required • Fuming Sulphuric acid (LCP form) Matteo Pasquali ( Rice University, Houston Texas) * Personal involvement 6
  • 7. Dispersion devices  Batch Stirred vessel; design, scale, feed protocol*.  High shear mixer*.  Ultra sound mixer; Biorupter, Nanorupter*.  Compounding device (Nanocyl)  Twin screw extruder (Nanocyl) * Personal involvement 7
  • 8. Best method of Mixing ?  Simple shear  Extension  Stretch and Fold or Mixed flow  “Vibration” 8
  • 9. MWCNT vs Carbon Black (CB) 0.25 wt% CNT in epoxy 0.25 wt% CB in epoxy Kat Yearsley 9
  • 10. Optical Observation of Untreated Multi-Walled CNT The Linkam, Cambridge Shear System CSS 10
  • 11. Microstructure • Optical Microscope combined with shear cell • Isotropic CB vs. Anisotropic CNTs Images Recorded 100 Shear Rate (s-1) 10 0.5 15 mins 10 s 10 s 11
  • 12. 0.25% CB in epoxy 12
  • 14. CB after low shear: CNT after low shear: Aggregation Aggregation Flow Flow CB after high shear: CNT after high shear: Disaggregation Disaggregation & alignment Flow Flow 14
  • 15. The “Zoo” of CNT Microstructure 0 s-1 1 s-1 10 s-1 100 s-1 1000 s-1 I. Untreated SWNT II. Treated SWNT III. Untreated MWNT IV. Treated MWNT All at 0.05 wt% conc 15
  • 16. Steady Shear (SS) Experiments CB CNT 1000 1000 1000 100 100 100 0.4% 4% 4% 0.3% η η 10 2% η (Pa.s)10 10 0%0%1%1%2%2%4%4% Pa.s) 3% (Pa.s) 0.2% 1% 1 1 2% 1 0% 0% 0% 0.10.1 0.1 0.10.1 1 1 10 10 100 0.1 100 1 10 100 Shear Rate (/s) Shear Rate (/s) Shear Rate (/s) 16
  • 17. Aggregation/orientation model , Paco Chinesta Diffusion equation ∂  dρ  ∂  ∂ψ (ρ, n )  ∂ψ (ρ, n ) ∂ 2ψ (ρ, n ) − ψ (ρ, n )  +  Dr ( n )  − 3vn + Dn =0 ∂ρ  dt  ∂ρ  ∂ρ  ∂n ∂n 2 Where n is population from n = 0 to n = 1 . βα = vd vc vn = v c − vd Dn = vd n + vc (1 − n ) , Destruction rate due to shear creation rate Constitutive equation σ = − p I + 2η D + 2ηN p a : D 17
  • 18. (a) 0.25% CNT (b) 0.1% CNT 1000 1000 ηa 100 ηa 100 [Pa.s] [Pa.s] 10 10 0.1 1 10 0.1 1 10 Shear rate [s -1] -1 Shear rate [s ] (c) 0.05% CNT (d) 0.025% CNT 100 100 ηa 10 ηa 10 [Pa.s] [Pa.s] 1 1 0.1 1 10 0.1 1 10 Shear rate [s -1] Shear rate [s -1] 18
  • 19. CNT Fibre makers  Pasqualli Group Rice University Houston  Windle team Cambridge University 19
  • 20. Rice University Houston.; Anson Ma and Matteo Pasquali, Oct 2010 20
  • 21. TRUE SOLUTIONS OF SWNTs 1 min 10 min 60 min CNTs dissolve spontaneously in chlorosulfonic acid Davis, Pasquali, et al, Nature Nanotech, 4, 830, 2009 21 Pasquali et al, US Patent Application under review (2009)
  • 22. BEHAVIOR AT HIGH CONCENTRATION 12% vol SWNT in chlorosulfonic, CROSS POLARS co hi ntra nc gh t e er ion ISOTROPIC CONCENTRATED LIQUID CRYSTALLINE analyzer -60 -45OOOO -75 -30O 50 µm 0O -15 polarizer Davis, Pasquai, et al, Nature Nanotech, 4, 830, 2009 22
  • 23. SPINNING NEAT SWNT FIBERS Ericson, Pasquali, Smalley, et al., Science, 305, 1447 (2004) Smalley, Pasquali, et al., US Patent 7,125,502 (2006) Davis, Pasquali, et al., Nature Nanotech., (2009) Pasquali et al., patent application under review 23
  • 24. TYPICAL ACID-SPUN SWNT FIBER Ø=37±3µm Ø=50±2µm Sub-optimal mesostructure (bundles), affect transport Excellent macrostructure 24 Wang, Pasquali, Smalley, et al., Chem. Mater., 17, 6361 (2005)
  • 25. SPINNING FROM CHLOROSULFONIC ACID 7 WT% SWNT in chlorosulfonic 7 wt% SWNT in 7 wt% SWNT in acid, coagulated in 96% H2SO4 chlorosulfonic chlorosulfonic 13 µm acid: Solvent acid, coagulated in evaporation dichloromethane 30 µ m 100 µm 100 µm 1 µm 1 µm 1 µm • Smooth, compact fibers via slow coagulation • Coagulants: dichloromethane, chloroform, ether, sulfuric acid (96%) 25 Davis, Pasquali, et al, Nature Nanotech, 4, 830, 2009
  • 26. Carbon Nanotube Fibres and their Composites Alan Windle And Team acromolecular aterials ab New Museums Site, Pembroke Street Cambridge, CB23QZ, UK
  • 27. Fibre spinning in furnace H2 Ethanol or Hexane Ferrocene 2% Thiophene 0.3% Nanotube 1100 - 1300`°C Smoke Its elastic! an aerogel Ya-Li Li, Ian Kinloch and Alan Windle, Science, 304, p 276, 9 April 2004 27
  • 28. Department of Materials, Cambridge, Injection system Reactor Gas exchange valve Fibre collection 28
  • 29. Continuous wind up with drawing (10 - 50 m/min) n.b. 20m/min at 0.05 tex is only 1mg/min or ~ 1g/day 29
  • 30. The knot test; (Get Knotted) Tensile strength not degraded by presence of a knot. c.f. For carbon fibre with a knot, strength can be only 10 % of unknotted sample 30
  • 31. Wide angle X-ray of fibre ESRF synchrotron source Grenoble 002 Winding rate = 20 m/min Winding rate = 30 m/min Very good orientation of CNTs, graphitic component Unoriented 31 but an unoriented component (particles ?)
  • 32. Carbon nanotube fibre properties Physical: Specific Gravity 0.5 – 1.1 (Diameter 10 micron) Mechanical: Strength 0.5 - 2.3 GPa/SG Stiffness 20 – 80 GPa/SG Thermal: Conductivity 50 – 1000 Wm -1K-1 Electrical: Conductivity 8 x 105 S/m (no influence of sample length, but only 1/60 of copper or 1/8 on a unit mass basis). Mix of metallic and 32
  • 33. Carbon nanotube fibres Carbon fibre Polymer fibres Carbon A new sort Nanotube of stuff ? Fibres Yarns 33
  • 34. Conclusions •CNTs (still) have exciting potential. •Handle with care. •Dispersion still a challenging problem. Next generation Composite reinforcement ? “Carbon Fibre” ? 34
  • 35. The problem! Polymers - CNTs Molecular dynamics simulations of entangled polymers (or maybe CNTs?) Prof Aleksei Likhtman (University of Reading) 35

Editor's Notes

  1. CB and CNTs are both nanoscale structures of graphitic carbon, although they have very different shapes. CNTs have very large aspect ratios, whereas CB has a more compact conformation. CB has been used as an additive to polymers to improve their conductivity for many years whereas CNTs are only now starting to be produced in large quantities (tonnes/year). There is, however, much interest in producing polymer/CNT composites owing to the superior electrical conductivity properties of the CNTs. The purpose of this study was to make a direct comparison between the microstructures formed by these two different carbon structures and the effect on rheology and electrical conductivity. CNTs were grown by CVD in the Material Science Dept at Cambridge University, producing tubes which are larger than commercially available CNTs. CB was obtained from the Cabot company. Both CB and CNTs were suspended in UV-curing epoxy, a Newtonian fluid, using ultrasound.
  2. In an effort to understand the origin of the viscosity enhancement, optical microscopy combined with a Cambridge Shear System shear cell was performed on low concentration CB and CNT samples. The shear cell consists of two parallel quartz plates, the top of which is fixed whereas the bottom can rotate. The gap size was set at 0.5 mm and the sample was viewed 7.5 mm from the centre of the plates. CB and CNTs have very different structures: CB particles form isotropic, approximately spherical shapes whereas CNTs are long and thin and therefore anisotropic. There is therefore much more scope for particle alignment with shear for CNTs than CB and it was hoped that this would be observed. CB and CNT suspensions were subjected to the same shear rate profile as shown in this sketch. The samples were sheared at 0.5 reciprocal seconds for 15 mins. The shear rate was then increased to 10 s-1 and then 100 s-1 for 10 s each. Video was taken for the last 10 s of the 0.5 s-1 shear and the entire period of shear at 10 s-1 and 100 s-1.
  3. Consider first a 0.25 wt% suspension of CB: [start video], the dark regions are the CB and the light regions are the epoxy. After 15 mins at a relatively low shear rate, these large aggregates have been formed… As the shear rate is increased, these aggregates start to break up… and then are broken up even more when the shear rate is increased to 100 s-1 so that at the end of the experiment… they are considerable smaller than they were at the beginning of the video. The aggregate size correlates with the viscosity of the suspension: larger aggregates correspond to a higher viscosity.
  4. Repeating the experiment with a 0.25 wt% suspension of CNTs gives similar results, although the video is less clear. Once again, the dark regions correspond to the CNTs and the light regions the epoxy. After long times at low shear rates, large aggregates have been formed and these aggregates are broken down as the shear rate is increased.
  5. This image shows a [0.25 wt%] suspension of CB after a long time at low shear. As seen in the video, the CB particles have formed aggregates. These are relatively large compared to the CB particles themselves, and so there will be relatively large van der Waals forces between them. At higher concentrations, the aggregates will be larger, and so the interactions between them will be larger until ultimately an extensive “elastic network” will be formed, corresponding the low frequency plateau observed in G’. [click] This image shows a suspension of CB after a period of high shear. The aggregates have been broken down, corresponding to a reduction in the apparent viscosity of the sample. [click and pause] The shear thinning behaviour is clearly related to the size of CB aggregates, with viscosity enhancement at low shear rates being possibly due to interaction between the aggregates. [pause] [click] CNTs have a long, thin structure compared to the more isotropic CB particles. This may affect the way they behave in suspension [pause]. After long times at low shear rates, the CNTs also form aggregates. As well as the van der Waals forces holding the particles together, however, there is also entanglement of CNTs [point out]. [click and pause] [click] After shear at high shear rates, as with the CB suspension, the aggregates have broken down, and the smaller CNT structures have also aligned with the shear flow [click and pause].
  6. Steady Shear experiments were also performed and, once again, the behaviour is very similar between the CB and CNT suspensions, although a larger concentration of CB is required to get the same rheological response. Both systems show shear thinning behaviour with the amount of viscosity enhancement at low shear increasing with increasing filler concentration.