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NANOTECHNOLOGY- CARBON NANOTUBES




      Presented by- Nithya Nair
CONTENTS

   Nanotechnology
   Introduction to the topic
   History
   Why carbon nanotubes?
   Fundamentals for Hydrogen Storage
    i. Physisorption
    ii.Chemisorption
   Comparison table
   Synthesis
   Doping
   Conclusion
   References
NANOTECHNOLOGY

    Nanotechnology is the creation of useful/functional materials, devices
    and systems (of any useful size ) through control manipulation of matter
    on the 1-100nm length scale and the use of novel phenomena and
    properties which arise because of nanometer length scale.
Nanometer
   One billionth of a meter (10-9 m)
   Hydrogen atom 0.04nm
   Proteins 1-20nm


   Chemically reactivity differs .
   Improved mechanical properties
   Increased surface area
   New chemical formulation
Source: Silicon Valley Toxics Coalition
INTRODUCTION


Carbon nanotubes are extremely thin hollow cylinders made of carbon with pores that
can store gases by the phenomena of adsorption.

Various carbon nanotubes

Single walled nanotubes (SWNT) - diameter range of 0.4 to 3nm .

Multi walled nanotubes (MWNT) - several sheets, arranged concentrically in
increasingly larger diameters with diameters in the range of 1.4 to 100 nm.

Metal doped nanotubes - Obtained by doping of various metals to carbon nanotubes.
HISTORY

   After Kroto & Smalley discovered Fullerene, one of carbon allotropes (a
    cluster of 60 carbon atoms: C60) for the first time in 1985, Dr.Iijima, a
    researcher for this new material , in Japan discovered in 1991, a thin long
    straw-shaped carbon Nanotubes during TEM analysis of carbon clusters.
PROPERTIES


   A carbon atom in nanotube forms a hexagonal lattice of sp² bond with three
    other carbon atoms.

   As the inner diameters of the tubes are extremely thin down to about
    several nanometers, the tubes are called Nanotubes.

   Thermal conductivity (>3000 W/m-K),

   The elastic ability to extend ≈5.8% of its original length

   More appealing still is the disproportionately large surface area to volume
    that these materials possess , for this allows for a greater potential of
    interactions, both physical or chemical in nature
APPLICATIONS IN HYDROGEN STORAGE


 Depleting non- renewable source of energy prompting us to move to an
  energy resource which is abundantly available and which is eco- friendly as
  well.


 „Hydrogen‟ ,sought as future fuel because of high energy content than any
  other fuel, at least 3 times than gasoline.


 Advantage- clean fuel, byproduct only water.

 Disadvantage- low energy density by volume. So difficult to store and
  transport.
WHY CARBON NANOTUBES FOR H2 STORAGE


Available techniques for hydrogen storage-


   As cryogenic liquid


   As pressurized gas


   As physical combination with metal hydrides/complex hydrides on board
    production


   By reform of methanol


   Carbon nanotubes
HYDROGEN STORAGE FUNDAMENTALS

Physisorption

   Based on Vander Waal‟s interaction.


   Stem from intermolecular forces between atoms that result from instantaneous
    charge distribution in atoms & molecules when they approach each other.


   The interaction energy, also called the London Dispersion forces
   Adsorption on a flat carbon surface depends on the adsorption stereometry.


    An average value would be 4-5 kj mol⁻1.This represents a very weak
    interaction .Therefore, hydrogen is desorbed with increasing temperature, and a
    very little hydrogen adsorption is observed on carbon at elevated temperature.
Source:greener-industry.org.uk website
CHEMISORPTION


    If the π-bonding between the carbon atom were to be fully utilized, every
    carbon atom could be a site for chemisorptions of one hydrogen atom.


   Desorption results of nanotubes treated with chemisorbed
    hydrogen, however, can only be released at higher temperatures.


   Hydrogen storage in CNTs by chemical reaction, on the other hand , has
    largely been discounted as irreversible and thus technologically less relevant
TABLE 1.1 VARIOUS SAMPLES OF CARBON NANOTUBES AND
              THEIR HYDROGEN STORAGE CAPACITY [11],[14]
Sample         % Purity             H₂ (wt%)   T(K)       P(MPa)    Ref.
SWNTs          Assumed 100          5-10       133        0.04      (A.C. Dillon et al.,
                                                                    1997)
SWNTs          50                   4.2        300        10.1      (C. Liu et al,1999)

SWNTs          High                 8.25       80         7         (Y. Ye et al, 1999)

SWNTs          Purified             1.2        Ambient    4.8       (Smith Jr, Bittner,Shi,
                                                                    Jhonson, & Bockrath,
                                                                    2003)



SWNTs          90 vol%              0.63       298        -         (Ritschel et al., 2002)

SWNTs          Purified             6          77         0.2       (Pradhan et al., 2002)


SWNTs          Unpurified           0.93       295        0.1       (Nishimaya     et     al.,
                                                                    2002)
SWNTs          Unpurified           0.37       77         0.1       (Nishimaya     et     al.,
                                                                    2002)
MWNTs          Purified             0.25       ~300-700   Ambient   (Wu et al., 2000)

MWNTs          Unpurified           0.5        298        -         (Ritschel et al., 2002)

MWNTs          High                 5-7        300        1.0       (Y. Chen et al., 2001)

MWNTs          High, acid treated   13.8       300        1.0       (Y. Chen et al., 2001)

MWNTs          High                 0.7-0.8    300        7.0       (Badzian, Breval       &
                                                                    Piotrowski, 2001)
SYNTHESIS




                                                                               Source: B lue penguin report




Schematics of a laser ablation set-up, reproduced from B. I. Yakobson and R.E. Smalley, American Scientist 85, 324 (1997).
METAL DOPED CARBON NANOTUBES

   Metal doping provides additional binding energy state of hydrogen.
   Transition metals doped- V, Ti, Pt and Pd.
   Storage condition : 30 atm, 300K
   Enhanced hydrogen storage capacity on doping, the reversible hydrogen storage
    capacity of doped nanotubes.




                                                 April 2011 Journal of the American Chemical Society
CHALLENGES TO OVERCOME

   High accessible surface, large free pore volume & strong
    interactions- Three main demand for high hydrogen storage
    capacity.


   A more accurate & practical approach towards studying
    thermodynamics, Kinetics, Adsorption /Desorption of
    nanotubes.


   Mass production of carbon nanotubes with controlled
    microstructures at a reasonable cost.
REFERENCES

1. ZHANG, Ei- fei; LUI, Ji-ping; LU, Guang- shu. “Preparation of Isolated Single Wall
    Carbon Nanotubes With High Hydrogen Capacity.”[J],(The Chinese Journal Of
    Process Engineering),Vol.6, No.3, June 2006.
2. Baughman, Ray H.; Anvar A. Zakhidov, and Walt A. De Heer. "Carbon Nanotubes:
   The Route toward Applications." Science 297 (2002): 787-92.
3. Iijima,S., Nature(1991) 354, 56.
4. http://www.energy.gov
5. U.S. Department of Energy‟s Efficiency and Renewable Energy Website.
   https://www1.eere.energy.gov/hydrogenandfuelcells/storage/current_technology.
   html(2010).
6. KUNG Chaoi, “Carbon Nanotubes for Hydrogen Storage”. Nov. 2002.
7. Yunjin, “Hydrogen Storage using carbon Nanotubes.” Hefei University of
   Technology, China
8. DILLON, A.C.; GENNET, T.; GELLEMEN, J.L.; JONES, K.M.; PARILLS, P.A. and
   Heben, “Optimization of Single –Wall Nanotube Synthesis For Hydrogen Storage”.
   National Renewable Energy Laboratory.
10. NIKITIN, Anton; LI, Xialolin; ZHANG, Zhang; OGASAWARA, Hirohita; DAI, Hongjie &
   NILSSON, Anders. “Hydrogen Storage in Carbon Nanotubes through the Formation of
   Stable C-H Bonds” Nano Letters, 2008 Vol.8, No.1 (162-167) .
11. Dillon, A. C.; K. M. Jones; T. A. Bekkedahl; C. H. Kiang, D. S. Bethune, and M. J. Heben.
   "Storage of hydrogen in single-walled carbon nanotubes." Nature 386 (1997): 377-79.
12. Liu, C., Y. Y. Fan, M. Liu, H. T. Chong, H. M. Cheng, and M. S. Dresselhaus. "Hydrogen
   Storage in Single-Walled Carbon Nanotubes at Room Temperature." Science 286 (1999):
   1127-129.
13. “Chemical Activation Of Single Walled Carbon Nanotubes for Hydrogen Adsorption’’.
   SMITH, Milton R.; BIITTNER, Edward W.; SHI, Wei & BOCKRATH, C. Bradely.
14. Chen, Y. L., B. Liu, J. Wu, Y. Huang, H. Jiang, and K. C. Hwang. "Mechanics of hydrogen
   storage in carbon nanotubes." Journal of the Mechanics and Physics of Solids 56 (2008):
   3224-241.
15. http://www.nanowerk.com
16. http://www.ewels.info/science/publications/papers/2008.DopingChapter.pdf
An introduction to synthesis  & applications of carbon (2)

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An introduction to synthesis & applications of carbon (2)

  • 1. NANOTECHNOLOGY- CARBON NANOTUBES Presented by- Nithya Nair
  • 2. CONTENTS  Nanotechnology  Introduction to the topic  History  Why carbon nanotubes?  Fundamentals for Hydrogen Storage i. Physisorption ii.Chemisorption  Comparison table  Synthesis  Doping  Conclusion  References
  • 3. NANOTECHNOLOGY Nanotechnology is the creation of useful/functional materials, devices and systems (of any useful size ) through control manipulation of matter on the 1-100nm length scale and the use of novel phenomena and properties which arise because of nanometer length scale. Nanometer  One billionth of a meter (10-9 m)  Hydrogen atom 0.04nm  Proteins 1-20nm  Chemically reactivity differs .  Improved mechanical properties  Increased surface area  New chemical formulation
  • 4. Source: Silicon Valley Toxics Coalition
  • 5. INTRODUCTION Carbon nanotubes are extremely thin hollow cylinders made of carbon with pores that can store gases by the phenomena of adsorption. Various carbon nanotubes Single walled nanotubes (SWNT) - diameter range of 0.4 to 3nm . Multi walled nanotubes (MWNT) - several sheets, arranged concentrically in increasingly larger diameters with diameters in the range of 1.4 to 100 nm. Metal doped nanotubes - Obtained by doping of various metals to carbon nanotubes.
  • 6. HISTORY  After Kroto & Smalley discovered Fullerene, one of carbon allotropes (a cluster of 60 carbon atoms: C60) for the first time in 1985, Dr.Iijima, a researcher for this new material , in Japan discovered in 1991, a thin long straw-shaped carbon Nanotubes during TEM analysis of carbon clusters.
  • 7. PROPERTIES  A carbon atom in nanotube forms a hexagonal lattice of sp² bond with three other carbon atoms.  As the inner diameters of the tubes are extremely thin down to about several nanometers, the tubes are called Nanotubes.  Thermal conductivity (>3000 W/m-K),  The elastic ability to extend ≈5.8% of its original length  More appealing still is the disproportionately large surface area to volume that these materials possess , for this allows for a greater potential of interactions, both physical or chemical in nature
  • 8. APPLICATIONS IN HYDROGEN STORAGE  Depleting non- renewable source of energy prompting us to move to an energy resource which is abundantly available and which is eco- friendly as well.  „Hydrogen‟ ,sought as future fuel because of high energy content than any other fuel, at least 3 times than gasoline.  Advantage- clean fuel, byproduct only water.  Disadvantage- low energy density by volume. So difficult to store and transport.
  • 9. WHY CARBON NANOTUBES FOR H2 STORAGE Available techniques for hydrogen storage-  As cryogenic liquid  As pressurized gas  As physical combination with metal hydrides/complex hydrides on board production  By reform of methanol  Carbon nanotubes
  • 10. HYDROGEN STORAGE FUNDAMENTALS Physisorption  Based on Vander Waal‟s interaction.  Stem from intermolecular forces between atoms that result from instantaneous charge distribution in atoms & molecules when they approach each other.  The interaction energy, also called the London Dispersion forces  Adsorption on a flat carbon surface depends on the adsorption stereometry.  An average value would be 4-5 kj mol⁻1.This represents a very weak interaction .Therefore, hydrogen is desorbed with increasing temperature, and a very little hydrogen adsorption is observed on carbon at elevated temperature.
  • 12. CHEMISORPTION  If the π-bonding between the carbon atom were to be fully utilized, every carbon atom could be a site for chemisorptions of one hydrogen atom.  Desorption results of nanotubes treated with chemisorbed hydrogen, however, can only be released at higher temperatures.  Hydrogen storage in CNTs by chemical reaction, on the other hand , has largely been discounted as irreversible and thus technologically less relevant
  • 13. TABLE 1.1 VARIOUS SAMPLES OF CARBON NANOTUBES AND THEIR HYDROGEN STORAGE CAPACITY [11],[14] Sample % Purity H₂ (wt%) T(K) P(MPa) Ref. SWNTs Assumed 100 5-10 133 0.04 (A.C. Dillon et al., 1997) SWNTs 50 4.2 300 10.1 (C. Liu et al,1999) SWNTs High 8.25 80 7 (Y. Ye et al, 1999) SWNTs Purified 1.2 Ambient 4.8 (Smith Jr, Bittner,Shi, Jhonson, & Bockrath, 2003) SWNTs 90 vol% 0.63 298 - (Ritschel et al., 2002) SWNTs Purified 6 77 0.2 (Pradhan et al., 2002) SWNTs Unpurified 0.93 295 0.1 (Nishimaya et al., 2002) SWNTs Unpurified 0.37 77 0.1 (Nishimaya et al., 2002) MWNTs Purified 0.25 ~300-700 Ambient (Wu et al., 2000) MWNTs Unpurified 0.5 298 - (Ritschel et al., 2002) MWNTs High 5-7 300 1.0 (Y. Chen et al., 2001) MWNTs High, acid treated 13.8 300 1.0 (Y. Chen et al., 2001) MWNTs High 0.7-0.8 300 7.0 (Badzian, Breval & Piotrowski, 2001)
  • 14. SYNTHESIS Source: B lue penguin report Schematics of a laser ablation set-up, reproduced from B. I. Yakobson and R.E. Smalley, American Scientist 85, 324 (1997).
  • 15. METAL DOPED CARBON NANOTUBES  Metal doping provides additional binding energy state of hydrogen.  Transition metals doped- V, Ti, Pt and Pd.  Storage condition : 30 atm, 300K  Enhanced hydrogen storage capacity on doping, the reversible hydrogen storage capacity of doped nanotubes. April 2011 Journal of the American Chemical Society
  • 16. CHALLENGES TO OVERCOME  High accessible surface, large free pore volume & strong interactions- Three main demand for high hydrogen storage capacity.  A more accurate & practical approach towards studying thermodynamics, Kinetics, Adsorption /Desorption of nanotubes.  Mass production of carbon nanotubes with controlled microstructures at a reasonable cost.
  • 17. REFERENCES 1. ZHANG, Ei- fei; LUI, Ji-ping; LU, Guang- shu. “Preparation of Isolated Single Wall Carbon Nanotubes With High Hydrogen Capacity.”[J],(The Chinese Journal Of Process Engineering),Vol.6, No.3, June 2006. 2. Baughman, Ray H.; Anvar A. Zakhidov, and Walt A. De Heer. "Carbon Nanotubes: The Route toward Applications." Science 297 (2002): 787-92. 3. Iijima,S., Nature(1991) 354, 56. 4. http://www.energy.gov 5. U.S. Department of Energy‟s Efficiency and Renewable Energy Website. https://www1.eere.energy.gov/hydrogenandfuelcells/storage/current_technology. html(2010). 6. KUNG Chaoi, “Carbon Nanotubes for Hydrogen Storage”. Nov. 2002. 7. Yunjin, “Hydrogen Storage using carbon Nanotubes.” Hefei University of Technology, China 8. DILLON, A.C.; GENNET, T.; GELLEMEN, J.L.; JONES, K.M.; PARILLS, P.A. and Heben, “Optimization of Single –Wall Nanotube Synthesis For Hydrogen Storage”. National Renewable Energy Laboratory.
  • 18. 10. NIKITIN, Anton; LI, Xialolin; ZHANG, Zhang; OGASAWARA, Hirohita; DAI, Hongjie & NILSSON, Anders. “Hydrogen Storage in Carbon Nanotubes through the Formation of Stable C-H Bonds” Nano Letters, 2008 Vol.8, No.1 (162-167) . 11. Dillon, A. C.; K. M. Jones; T. A. Bekkedahl; C. H. Kiang, D. S. Bethune, and M. J. Heben. "Storage of hydrogen in single-walled carbon nanotubes." Nature 386 (1997): 377-79. 12. Liu, C., Y. Y. Fan, M. Liu, H. T. Chong, H. M. Cheng, and M. S. Dresselhaus. "Hydrogen Storage in Single-Walled Carbon Nanotubes at Room Temperature." Science 286 (1999): 1127-129. 13. “Chemical Activation Of Single Walled Carbon Nanotubes for Hydrogen Adsorption’’. SMITH, Milton R.; BIITTNER, Edward W.; SHI, Wei & BOCKRATH, C. Bradely. 14. Chen, Y. L., B. Liu, J. Wu, Y. Huang, H. Jiang, and K. C. Hwang. "Mechanics of hydrogen storage in carbon nanotubes." Journal of the Mechanics and Physics of Solids 56 (2008): 3224-241. 15. http://www.nanowerk.com 16. http://www.ewels.info/science/publications/papers/2008.DopingChapter.pdf