Page 37 - Science at the nanoscale
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RPS: PSP0007 - Science-at-Nanoscale
                             7:14
                   June 9, 2009
                                                                      2.4. Motion at the Nanoscale
                               From the Gaussian relation in (2.15), we can define the charac-
                             teristic 2D diffusion length as:
                                                              1
                                                               /
                                                   x rms = (4Dt) 2
                                                                                  (2.17)
                               If we go back to the example in the previous section of the iron
                             nanoparticle of 1 nm radius falling through water with terminal
                                            −1
                             velocity of 1 pms
                                              , the corresponding Brownian diffusion length
                                       1/2
                             x rms = 2D
                                          is about 9 µm, which is the characteristic distance
                             displaced every second due to Brownian motion. This value is
                             much larger than 1 pm, and hence Brownian diffusive motion is
                             dominant for the 1 nm particle.
                               If however the iron particle radius was 1 µm, its diffusion length
                             is now 0.3 µm, which is almost comparable to its terminal velocity
                                    −1
                                      . Hence both diffusive motion and viscosity of the fluid
                             of 1 µms
                             need to be taken into account in describing the particle’s motion.
                             In general, Newton’s law of motion in such cases in the presence
                             of an external force F ext and taking into account the Brownian dif-
                             fusive force F(t) and viscosity η of the fluid can be written in 1D
                             as:
                                                                          2
                                                                     3


                                                          dx
                                                                         d x
                                                                 4πR ρ
                                                                                  (2.18)
                                                             =
                                       F ext + F(t) − (6πηR)
                                                                           2
                                                          dt
                                                                   3
                                                                         dt
                               This so-called Langevin equationLangevin equation is a stochastic
                             differential equation in which two force terms have been added
                             to Newton’s second law: One term represents a frictional force
                             due to viscosity, the other a random force F(t) associated with the
                             thermal motion of the fluid molecules. Since friction opposes mo-
                             tion, the first additional force is proportional to the particle’s ve-  27  ch02
                             locity (dx/dt) and is oppositely directed. This equation needs to be
                             solved to describe the complete motion of a nanosized-object in a
                             fluid.
                             2.4  MOTION AT THE NANOSCALE
                             It has been often hypothesised that in the not-too-distant-future,
                             micron-sized medical nanorobots will be able to navigate through
                             our bloodstream to destroy harmful viruses and cancerous cells
                             (see Figure 2.4).  This is reminiscent of the 1966 science fic-
                             tion film Fantastic Voyage written by Harry Kleiner, which was
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