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{{About|the dynamics of fluids confined in nanoscale structures|fluids containing nanoparticles|Nanofluid}}
 
'''Nanofluidics''' is the study of the behavior, manipulation, and control of [[fluid]]s that are confined to structures of [[nanometer]] (typically 1-100&nbsp;nm) characteristic dimensions (1&nbsp;nm = 10<sup>−9</sup> m). Fluids confined in these structures exhibit physical behaviors not observed in larger structures, such as those of [[Microfluidics|micrometer]] dimensions and above, because the characteristic physical scaling lengths of the fluid, (''e.g.'' [[Debye length]], [[hydrodynamic radius]]) very closely coincide with the dimensions of the [[nanostructure]] itself.[[Image:NCAM.png|frame||right|Schematic diagram of one particular realization of nanofluidics in a nanocapillary array membrane, or NCAM.  The NCAM is composed of a large number of parallel nanocapillaries, each of which have a pore radius, ''a/2'', which is approximately the same size as the Debye length, ''κ<sup>-1</sup>''.  The electrical double layer is characterized by a counter-ion distribution, ''N'', which is largest at the pore wall and decays toward the center of the pore.]]
 
When structures approach the size regime corresponding to molecular scaling lengths, new physical constraints are placed on the behavior of the fluid.  For example, these physical constraints induce regions of the fluid to exhibit new properties not observed in bulk, ''e.g.'' vastly increased [[viscosity]] near the pore wall; they may effect changes in [[thermodynamic]] properties and may also alter the [[chemical reactivity]] of species at the fluid-solid [[Interface (chemistry)|interface]].  A particularly relevant and useful example is displayed by [[electrolyte]] solutions confined in [[nanopore]]s that contain [[surface charge]]s, ''i.e.'' at electrified interfaces, as shown in the nanocapillary array membrane (NCAM) in the accompanying figure.
 
All electrified interfaces induce an organized charge distribution near the surface known as the [[electrical double layer]].  In pores of nanometer dimensions the electrical double layer may completely span the width of the nanopore, resulting in dramatic changes in the composition of the fluid and the related properties of fluid motion in the structure. For example, the drastically enhanced [[Surface area to volume ratio|surface-to-volume ratio]] of the pore results in a preponderance of counter-ions (''i.e.'' [[ion]]s charged oppositely to the static wall charges) over co-ions (possessing the same sign as the wall charges), in many cases to the near-complete exclusion of co-ions, such that only one ionic species exists in the pore.  This can be used for manipulation of species with selective polarity along the pore length to achieve unusual fluidic manipulation schemes not possible in [[Microfluidics|micrometer]] and larger structures.
 
== Theory ==
In 1965, Rice and Whitehead published the seminal contribution to the theory of the transport of electrolyte solutions in long (ideally infinite) nanometer-diameter capillaries.<ref>Rice, C. L.; Whitehead, R. ''Journal of Physical Chemistry'' 1965, '''69''', 4017-4024.</ref>
Briefly, the [[Electric potential|potential]], ''ϕ'', at a radial distance, ''r'', is given by the [[Poisson-Boltzmann equation]],
<br /><math>\frac{1}{r}\frac{d}{dr}\left (r \frac{d\phi}{dr} \right )= \kappa^2 \phi \  </math><br />
where ''κ'' is the inverse [[Debye length]],
<br /><math>\kappa = \sqrt{\frac{8\pi n e^2}{\epsilon k T}} </math><br />
determined by the ion [[number density]], ''n'', the [[dielectric constant]], ''ε'',  the [[Boltzmann constant]], ''k'', and the temperature, ''T''.  Knowing the potential, ''φ(r)'', the [[charge density]] can then be recovered from the [[Poisson equation]], whose solution may be expressed as a modified [[Bessel function]] of the first kind, ''I<sub>0</sub>'', and scaled to the capillary radius, ''a''. An equation of motion under combined pressure and [[Electrohydrodynamics|electrically-driven]] flow can then be written,
<br /><math>\frac{1}{r} \frac{d}{dr} \left (r \frac{d v_z}{dr} \right )= \frac{1}{\eta} \frac{dp}{dz} - \frac{F_z}{\eta}</math><br />
where ''η'' is the viscosity, ''dp/dz'' is the pressure gradient, and ''F<sub>z</sub>'' is the body force driven by the action of the applied [[electric field]], ''E<sub>z</sub>'', on the net charge density in the double layer.
When there is no applied pressure, the radial distribution of the velocity is given by,
<br /><math>v_z\left (r \right) = \frac{\epsilon \phi_0}{4 \pi \eta} E_z \left [ 1 - \frac {I_0 \left ( \kappa r \right )} {I_0 \left ( \kappa a \right )} \right ]</math><br />
From the equation above, it follows that fluid flow in nanocapillaries is governed by the ''κa'' product, that is, the relative sizes of the [[Debye length]] and the pore radius.
By adjusting these two parameters and the surface charge density of the nanopores, fluid flow can be manipulated as desired.
 
== Fabrication ==
Nanostructures can be fabricated as single cylindrical channels, nanoslits, or nanochannel arrays from materials such as silicon, glass, polymers (e.g. [[Poly(methyl methacrylate)|PMMA]], [[Polydimethylsiloxane|PDMS]], PCTE) and synthetic vesicles.<ref>Karlsson, M.; Davidson, M.; Karlsson, R.; Karlsson, A.; Bergenholtz, J.; Konkoli, Z.; Jesorka, A.; Lobovkina, T.; Hurtig, J.; Voinova, M.; Orwar, O. ''Annu. Rev. Phys. Chem.'' 2004, '''55''', 613-649.</ref>
Standard [[photolithography]], bulk or surface micromachining, replication techniques (embossing, printing, casting and injection molding), and nuclear track or chemical etching,<ref>Lichtenberg, J.; Baltes, H. In ''Advanced Micro & Nanosystems'', 2004; Vol. 1, pp 319-355., 4</ref><ref>Mijatovic, D.; Eijkel, J. C. T.; van den Berg, A. ''Lab on a Chip'' 2005, '''5''', 492-500.</ref>
are commonly used to fabricate structures which exhibit characteristic nanofluidic behavior.
 
== Applications ==
Because of the small size of the fluidic conduits, nanofluidic structures are naturally applied in situations demanding that samples be handled in exceedingly small quantities, including Coulter counting,<ref>Saleh, O. A.; Sohn, L. L. ''Review of Scientific Instruments'' 2001, '''72''', 4449-4451.</ref>
analytical separations and determinations of biomolecules, such as proteins and DNA,<ref>Han, C.; Jonas, O. T.; Robert, H. A.; Stephen, Y. C. ''Applied Physics Letters'' 2002, '''81''', 3058-3060.</ref>
and facile handling of mass-limited samples.  One of the more promising areas of nanofluidics is its potential for integration into microfluidic systems, i.e. [[µTAS|MicroTotal Analytical Systems]] or [[Lab-on-a-chip]] structures.  For instance, NCAMs, when incorporated into microfluidic devices, can reproducibly perform digital switching, allowing transfer of fluid from one microfluidic channel to another,<ref name="Cannon">Cannon, J. D.; Kuo, T.-C.; Bohn, P. W.; Sweedler, J. V. ''Analytical Chemistry'' 2003, '''75''', 2224-2230.</ref><ref>Pardon G, Gatty HK, Stemme G, van der Wijngaart W, Roxhed N. Pt-Al(2)O(3) dual layer atomic layer deposition coating in high aspect ratio nanopores. Nanotechnology. 2012 Dec 4;24(1):015602–2. http://dx.doi.org/10.1088/0957-4484/24/1/015602</ref>
selectivity separate and transfer analytes by size and mass,<ref name="Cannon">Cannon, J. D.; Kuo, T.-C.; Bohn, P. W.; Sweedler, J. V. Analytical Chemistry 2003, 75, 2224-2230.</ref><ref>Ramirez, P.; Mafe, S.; Alcaraz, A.; Cervera, J. ''Journal of Physical Chemistry B'' 2003, '''107''', 13178-13187.</ref><ref>Kohli, P.; Harrell, C. C.; Cao, Z.; Gasparac, R.; Tan, W.; Martin, C. R. ''Science'' 2004, '''305''', 984-986.</ref><ref>Jirage, K. B.; Hulteen, J. C.; Martin, C. R. ''Analytical Chemistry'' 1999, '''71''' 4913-4918.</ref><ref>Kuo, T. C.; Sloan, L. A.; Sweedler, J. V.; Bohn, P. W. ''Langmuir'' 2001, '''17''', 6298-6303.</ref>
mix reactants efficiently,<ref>Tzu-C. Kuo, Kim, H.K.; Cannon, D.M. Jr.; Shannon, M.A.; Sweedler, J.V.; Bohn, P.W. ''Angewandte Chemie International Edition'' 2004, '''43''', 1862-1865.</ref>
and separate fluids with disparate characteristics.<ref name="Cannon">Cannon, J. D.; Kuo, T.-C.; Bohn, P. W.; Sweedler, J. V. Analytical Chemistry 2003, 75, 2224-2230.</ref><ref>Fa, K.; Tulock, J. J.; Sweedler, J. V.; Bohn, P. W. ''Journal of the American Chemical Society'' 2005, '''127''', 13928-13933.</ref>
In addition, there is a natural analogy between the fluid handling capabilities of nanofluidic structures and the ability of electronic components to control the flow of electrons and holes. This analogy has been used to realize active electronic functions such as rectification<ref>Cervera, J.; Schiedt, B.; Neumann, R.; Mafe, S.; Ramirez, P., Ionic conduction, rectification, and selectivity in single conical nanopores.'' Journal of Chemical Physics'' 2006, '''124''', 104706.</ref><ref>Guan, W.; Fan, R.; Reed, M.; "Field-effect reconfigurable nanofluidic ionic diodes." ''Nature Communications'',2, 506, (2011). http://dx.doi.org/10.1038/ncomms1514</ref>
and field-effect<ref>Karnik, R.; Castelino, K.; Majumdar, A., Field-effect control of protein transport in a nanofluidic transistor circuit. ''Applied Physics Letters'' 2006, '''88''', 123114.</ref><ref>Karnik, R.; Fan, R.; Yue, M.; Li, D.Y.; Yang, P.D.; Majumdar, A., Electrostatic control of ions and molecules in nanofluidic transistors. ''NanoLetters'' 2005, '''5''', 943-948.</ref><ref>Pardon G, van der Wijngaart W. Modeling and simulation of electrostatically gated nanochannels. Advances in Colloid and Interface Science. 2013 Nov;199-200C:78–94. http://dx.doi.org/10.1016/j.cis.2013.06.006</ref>
and bipolar [[transistor]]<ref>Daiguji, H.; Yang, P.D.; Majumdar, A., Ion transport in nanofluidic channels. ''NanoLetters'' 2004, '''4''', 137-142.</ref><ref>Ivan Vlassiouk and Zuzanna S. Siwy, Nanofluidic Diode. ''Nano Letters'' 2007, '''7''', 552-556</ref>
action with ionic currents. Application of nanofluidics is also to Nano-optics for producing tuneable microlens array<ref>Liquid micro-lens array activated by selective electrowetting on lithium niobate substrates
S. Grilli, L. Miccio, V. Vespini, A. Finizio, S. De Nicola, and P. Ferraro
Optics Express 16, 8084-8093 (2008).  http://dx.doi.org/10.1364/OE.16.008084</ref><ref>P. Ferraro, L. Miccio, S. Grilli, A. Finizio, S. De Nicola, and V. Vespini, "Manipulating Thin Liquid Films for Tunable Microlens Arrays," Optics & Photonics News 19, 34-34 (2008) http://www.opticsinfobase.org/abstract.cfm?URI=OPN-19-12-34</ref>
 
Nanofluidics have had a significant impact in [[biotechnology]], [[medicine]] and clinical diagnostics with the development of [[lab-on-a-chip]] devices for [[PCR]] and related techniques.<ref name= Herold2>{{cite book |author= Herold, KE; Rasooly, A (editor)| year=2009 |title=Lab-on-a-Chip Technology: Biomolecular Separation and Analysis | publisher=Caister Academic Press | isbn= 978-1-904455-47-9}}</ref>
 
Because the science of nanofluidics is still in its infancy, we can expect rapid development of new applications in the coming years.
 
== Challenges ==
There are a variety of challenges associated with the flow of liquids through [[carbon nanotube]]s and nanopipes. A common occurrence is channel blocking due to large macromolecules in the liquid. Also, any insoluble debris in the liquid can easily clog the tube. A solution for this researchers are hoping to find is a low friction coating or channel materials that help reduce the blocking of the tubes. Also, due to the large size of polymers, including biologically relevant molecules such as DNA often fold ''in vivo''. This causes blockage because typical DNA molecules from a virus have lengths of approx. 100-200 kilobases and will form a random coil of the radius some 700&nbsp;nm in aqueous solution at 20%. This is also several times greater than the pore diameter of even large carbon pipes and 2 orders of magnitude the diameter of a single walled carbon nanotube.
 
== See also ==
* [[Nanomechanics]]
* [[Nanotechnology]]
* [[Microfluidics]]
* [[Nanofluidic circuitry]]
 
== References ==
{{reflist}}
 
[[Category:Nanotechnology]]
[[Category:Fluid dynamics]]
[[Category:Analytical chemistry]]
[[Category:Surface chemistry]]
[[Category:Materials science]]
 
[[ja:流体素子]]

Revision as of 07:33, 23 January 2014

29 yr old Orthopaedic Surgeon Grippo from Saint-Paul, spends time with interests including model railways, top property developers in singapore developers in singapore and dolls. Finished a cruise ship experience that included passing by Runic Stones and Church.

Nanofluidics is the study of the behavior, manipulation, and control of fluids that are confined to structures of nanometer (typically 1-100 nm) characteristic dimensions (1 nm = 10−9 m). Fluids confined in these structures exhibit physical behaviors not observed in larger structures, such as those of micrometer dimensions and above, because the characteristic physical scaling lengths of the fluid, (e.g. Debye length, hydrodynamic radius) very closely coincide with the dimensions of the nanostructure itself.

Schematic diagram of one particular realization of nanofluidics in a nanocapillary array membrane, or NCAM. The NCAM is composed of a large number of parallel nanocapillaries, each of which have a pore radius, a/2, which is approximately the same size as the Debye length, κ-1. The electrical double layer is characterized by a counter-ion distribution, N, which is largest at the pore wall and decays toward the center of the pore.

When structures approach the size regime corresponding to molecular scaling lengths, new physical constraints are placed on the behavior of the fluid. For example, these physical constraints induce regions of the fluid to exhibit new properties not observed in bulk, e.g. vastly increased viscosity near the pore wall; they may effect changes in thermodynamic properties and may also alter the chemical reactivity of species at the fluid-solid interface. A particularly relevant and useful example is displayed by electrolyte solutions confined in nanopores that contain surface charges, i.e. at electrified interfaces, as shown in the nanocapillary array membrane (NCAM) in the accompanying figure.

All electrified interfaces induce an organized charge distribution near the surface known as the electrical double layer. In pores of nanometer dimensions the electrical double layer may completely span the width of the nanopore, resulting in dramatic changes in the composition of the fluid and the related properties of fluid motion in the structure. For example, the drastically enhanced surface-to-volume ratio of the pore results in a preponderance of counter-ions (i.e. ions charged oppositely to the static wall charges) over co-ions (possessing the same sign as the wall charges), in many cases to the near-complete exclusion of co-ions, such that only one ionic species exists in the pore. This can be used for manipulation of species with selective polarity along the pore length to achieve unusual fluidic manipulation schemes not possible in micrometer and larger structures.

Theory

In 1965, Rice and Whitehead published the seminal contribution to the theory of the transport of electrolyte solutions in long (ideally infinite) nanometer-diameter capillaries.[1] Briefly, the potential, ϕ, at a radial distance, r, is given by the Poisson-Boltzmann equation,
1rddr(rdϕdr)=κ2ϕ
where κ is the inverse Debye length,
κ=8πne2ϵkT
determined by the ion number density, n, the dielectric constant, ε, the Boltzmann constant, k, and the temperature, T. Knowing the potential, φ(r), the charge density can then be recovered from the Poisson equation, whose solution may be expressed as a modified Bessel function of the first kind, I0, and scaled to the capillary radius, a. An equation of motion under combined pressure and electrically-driven flow can then be written,
1rddr(rdvzdr)=1ηdpdz−Fzη
where η is the viscosity, dp/dz is the pressure gradient, and Fz is the body force driven by the action of the applied electric field, Ez, on the net charge density in the double layer. When there is no applied pressure, the radial distribution of the velocity is given by,
vz(r)=ϵϕ04πηEz[1−I0(κr)I0(κa)]
From the equation above, it follows that fluid flow in nanocapillaries is governed by the κa product, that is, the relative sizes of the Debye length and the pore radius. By adjusting these two parameters and the surface charge density of the nanopores, fluid flow can be manipulated as desired.

Fabrication

Nanostructures can be fabricated as single cylindrical channels, nanoslits, or nanochannel arrays from materials such as silicon, glass, polymers (e.g. PMMA, PDMS, PCTE) and synthetic vesicles.[2] Standard photolithography, bulk or surface micromachining, replication techniques (embossing, printing, casting and injection molding), and nuclear track or chemical etching,[3][4] are commonly used to fabricate structures which exhibit characteristic nanofluidic behavior.

Applications

Because of the small size of the fluidic conduits, nanofluidic structures are naturally applied in situations demanding that samples be handled in exceedingly small quantities, including Coulter counting,[5] analytical separations and determinations of biomolecules, such as proteins and DNA,[6] and facile handling of mass-limited samples. One of the more promising areas of nanofluidics is its potential for integration into microfluidic systems, i.e. MicroTotal Analytical Systems or Lab-on-a-chip structures. For instance, NCAMs, when incorporated into microfluidic devices, can reproducibly perform digital switching, allowing transfer of fluid from one microfluidic channel to another,[7][8] selectivity separate and transfer analytes by size and mass,[7][9][10][11][12] mix reactants efficiently,[13] and separate fluids with disparate characteristics.[7][14] In addition, there is a natural analogy between the fluid handling capabilities of nanofluidic structures and the ability of electronic components to control the flow of electrons and holes. This analogy has been used to realize active electronic functions such as rectification[15][16] and field-effect[17][18][19] and bipolar transistor[20][21] action with ionic currents. Application of nanofluidics is also to Nano-optics for producing tuneable microlens array[22][23]

Nanofluidics have had a significant impact in biotechnology, medicine and clinical diagnostics with the development of lab-on-a-chip devices for PCR and related techniques.[24]

Because the science of nanofluidics is still in its infancy, we can expect rapid development of new applications in the coming years.

Challenges

There are a variety of challenges associated with the flow of liquids through carbon nanotubes and nanopipes. A common occurrence is channel blocking due to large macromolecules in the liquid. Also, any insoluble debris in the liquid can easily clog the tube. A solution for this researchers are hoping to find is a low friction coating or channel materials that help reduce the blocking of the tubes. Also, due to the large size of polymers, including biologically relevant molecules such as DNA often fold in vivo. This causes blockage because typical DNA molecules from a virus have lengths of approx. 100-200 kilobases and will form a random coil of the radius some 700 nm in aqueous solution at 20%. This is also several times greater than the pore diameter of even large carbon pipes and 2 orders of magnitude the diameter of a single walled carbon nanotube.

See also

References

43 year old Petroleum Engineer Harry from Deep River, usually spends time with hobbies and interests like renting movies, property developers in singapore new condominium and vehicle racing. Constantly enjoys going to destinations like Camino Real de Tierra Adentro.

ja:流体素子

  1. ↑ Rice, C. L.; Whitehead, R. Journal of Physical Chemistry 1965, 69, 4017-4024.
  2. ↑ Karlsson, M.; Davidson, M.; Karlsson, R.; Karlsson, A.; Bergenholtz, J.; Konkoli, Z.; Jesorka, A.; Lobovkina, T.; Hurtig, J.; Voinova, M.; Orwar, O. Annu. Rev. Phys. Chem. 2004, 55, 613-649.
  3. ↑ Lichtenberg, J.; Baltes, H. In Advanced Micro & Nanosystems, 2004; Vol. 1, pp 319-355., 4
  4. ↑ Mijatovic, D.; Eijkel, J. C. T.; van den Berg, A. Lab on a Chip 2005, 5, 492-500.
  5. ↑ Saleh, O. A.; Sohn, L. L. Review of Scientific Instruments 2001, 72, 4449-4451.
  6. ↑ Han, C.; Jonas, O. T.; Robert, H. A.; Stephen, Y. C. Applied Physics Letters 2002, 81, 3058-3060.
  7. ↑ 7.0 7.1 7.2 Cannon, J. D.; Kuo, T.-C.; Bohn, P. W.; Sweedler, J. V. Analytical Chemistry 2003, 75, 2224-2230. Cite error: Invalid <ref> tag; name "Cannon" defined multiple times with different content
  8. ↑ Pardon G, Gatty HK, Stemme G, van der Wijngaart W, Roxhed N. Pt-Al(2)O(3) dual layer atomic layer deposition coating in high aspect ratio nanopores. Nanotechnology. 2012 Dec 4;24(1):015602–2. http://dx.doi.org/10.1088/0957-4484/24/1/015602
  9. ↑ Ramirez, P.; Mafe, S.; Alcaraz, A.; Cervera, J. Journal of Physical Chemistry B 2003, 107, 13178-13187.
  10. ↑ Kohli, P.; Harrell, C. C.; Cao, Z.; Gasparac, R.; Tan, W.; Martin, C. R. Science 2004, 305, 984-986.
  11. ↑ Jirage, K. B.; Hulteen, J. C.; Martin, C. R. Analytical Chemistry 1999, 71 4913-4918.
  12. ↑ Kuo, T. C.; Sloan, L. A.; Sweedler, J. V.; Bohn, P. W. Langmuir 2001, 17, 6298-6303.
  13. ↑ Tzu-C. Kuo, Kim, H.K.; Cannon, D.M. Jr.; Shannon, M.A.; Sweedler, J.V.; Bohn, P.W. Angewandte Chemie International Edition 2004, 43, 1862-1865.
  14. ↑ Fa, K.; Tulock, J. J.; Sweedler, J. V.; Bohn, P. W. Journal of the American Chemical Society 2005, 127, 13928-13933.
  15. ↑ Cervera, J.; Schiedt, B.; Neumann, R.; Mafe, S.; Ramirez, P., Ionic conduction, rectification, and selectivity in single conical nanopores. Journal of Chemical Physics 2006, 124, 104706.
  16. ↑ Guan, W.; Fan, R.; Reed, M.; "Field-effect reconfigurable nanofluidic ionic diodes." Nature Communications,2, 506, (2011). http://dx.doi.org/10.1038/ncomms1514
  17. ↑ Karnik, R.; Castelino, K.; Majumdar, A., Field-effect control of protein transport in a nanofluidic transistor circuit. Applied Physics Letters 2006, 88, 123114.
  18. ↑ Karnik, R.; Fan, R.; Yue, M.; Li, D.Y.; Yang, P.D.; Majumdar, A., Electrostatic control of ions and molecules in nanofluidic transistors. NanoLetters 2005, 5, 943-948.
  19. ↑ Pardon G, van der Wijngaart W. Modeling and simulation of electrostatically gated nanochannels. Advances in Colloid and Interface Science. 2013 Nov;199-200C:78–94. http://dx.doi.org/10.1016/j.cis.2013.06.006
  20. ↑ Daiguji, H.; Yang, P.D.; Majumdar, A., Ion transport in nanofluidic channels. NanoLetters 2004, 4, 137-142.
  21. ↑ Ivan Vlassiouk and Zuzanna S. Siwy, Nanofluidic Diode. Nano Letters 2007, 7, 552-556
  22. ↑ Liquid micro-lens array activated by selective electrowetting on lithium niobate substrates S. Grilli, L. Miccio, V. Vespini, A. Finizio, S. De Nicola, and P. Ferraro Optics Express 16, 8084-8093 (2008). http://dx.doi.org/10.1364/OE.16.008084
  23. ↑ P. Ferraro, L. Miccio, S. Grilli, A. Finizio, S. De Nicola, and V. Vespini, "Manipulating Thin Liquid Films for Tunable Microlens Arrays," Optics & Photonics News 19, 34-34 (2008) http://www.opticsinfobase.org/abstract.cfm?URI=OPN-19-12-34
  24. ↑ 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

    My blog: http://www.primaboinca.com/view_profile.php?userid=5889534
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