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406                                                   13 Nanoaerosol

            13.4.2 Adhesion Efficiency and Nanoaerosol Thermal
                   Rebound


            In conventional filtration theory, the adhesion efficiency is assumed unity (η ad ≡ 1).
            However, it is not certain for nanoaerosol particles. Conventional filtration theory
            (in Sect. 6.5) indicates that nanoaerosol particle filtration efficiency increases
            inversely with particle size. Base on this hypothesis, filtration efficiency of nano-
            aerosol particles can reach 100 % for a properly designed filter. In reality, however,
            there should be a critical size from which filtration efficiency drops with the
            decrease of particle diameter (see Fig. 13.4). Otherwise, gas molecules, which are
            indeed extremely small particles, should be captured by filters resulting in no
            separation of aerosol particles and the carrier gas. Knowledge of this critical size is
            important to the design of effective nanoaerosol filters.
              When an aerosol particle impacts on a filtration surface, there is an interfacial
            adhesion force attempting to hold them together. When the adhesion force is strong
            enough to offset the outgoing momentum at the end of impact, the particle is
            captured by the filtration surface. It has been well accepted that aerosol particles
            always stick on the surface in contact. However, this may not be true for nano-
            aerosol particles because the impact between a solid nanoparticle and a solid surface
            is most likely elastic because of the small contact area, high speed, and unique
            properties of nanoaerosol [10]. As a result, nanoparticles may rebound from the
            filtration surface.
              Most researchers (e.g., [60]) assume that the thermal speed of nanoaerosol
            particles follow the Maxwell–Boltzmann distribution, which is described in
            Eq. (13.18).

                                           m            mv im
                                                3=2       2
                                       2
                             f ðv im Þ¼ 4pv       exp                   ð13:18Þ
                                       im
                                          2pkT          2kT


            Fig. 13.4 Filtration efficiency
            vs aerosol particle diameter
            (not in scale)
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