Introduction to Nanoscience and Nanotechnology. Chris Binns
Чтение книги онлайн.

Читать онлайн книгу Introduction to Nanoscience and Nanotechnology - Chris Binns страница 24

Название: Introduction to Nanoscience and Nanotechnology

Автор: Chris Binns

Издательство: John Wiley & Sons Limited

Жанр: Отраслевые издания

Серия:

isbn: 9781119172253

isbn:

СКАЧАТЬ A Bohr magneton (1μB) is the magnetic moment of a single free electron produced by its intrinsic angular momentum (spin).

      4 4 The high magnetization was first observed in Fe67Co33 alloys, but the magnetically soft variant Fe50Co50 that is used commercially was patented in 1929 by G. W. Elmer.

      5 5 Bacterium that infects the lungs of cystic fibrosis sufferers and causes inflammation and breathing problems.

      6 6 You should find that your estimate is much larger than the critical size (~100 nm) for a single‐domain particle given in the text. The reason is that the exchange energy in a domain boundary can be reduced by a large factor by spreading it over a number of atomic layers. That is, instead of having an abrupt 180ª reversal of the magnetization across a single atomic plane, the magnetization rotates a fraction of 180° across each plane. This brings the critical size down to ~100 nm.

      In the previous chapter, the special properties of matter at nanoscale dimensions were presented and how this novel behavior could be exploited in technologies as diverse as advanced engineering materials and health care. This chapter is about nanoparticles and the environment, which encompasses naturally occurring nanoparticles and environmental applications of nanotechnology. Sections 2.12.7 discuss naturally occurring nanoparticles, both in our immediate environment, that is, the Earth's crust, oceans and atmosphere and out into deep space, where nanoparticles with their unique properties have helped shape the observable Universe. Section 2.7 describes the use of nanoparticles in addressing environmental issues via two important examples, that is, removing toxins from groundwater and recycling plastics.

      The particles in the Earth's atmosphere have an important influence on the climate, but also have a poorly understood effect on life and our health. Improving our understanding of the effect of airborne nanoparticles is becoming increasingly important in a world where nanotechnology is poised to become a major activity. Clearly, the amount of manufactured nanoparticles will increase, so it is wise to be aware of how they interact with life and with the environment. It is important to emphasize, however, that manufactured nanoparticles are normally bound up in some material and the number of “loose” particles produced by nanotechnology will not necessarily become significant compared to those produced by the natural processes described below. In this chapter, the discussion is extended to encompass nanoparticles that are generated by existing human activities not directly involving nanotechnology, such as power generation, transport, etc. Obviously, these are not naturally occurring in the normal sense of the phrase, but they are a component of a pre‐nanotechnology background of nanoparticles in which we live. The effect of naturally occurring nanoparticles on the environment is an enormous multidisciplinary subject and a rigorous discussion is well beyond the scope of this book. It is an important hot topic, however, as it encompasses climate change and nanoparticles are implicated in many of the feedback mechanisms involved in the Gaia hypothesis that treats the Earth as a living organism. The aim of this chapter is to describe, in general terms, where the nanoparticles come from and, as in the previous chapter, emphasize the special nature of particles belonging to the nanoworld (<100 nm – Figure I.1).

image

      Source: (a) US Geological Survey. (b) Reproduced with permission from the government of British Columbia. (d) Reproduced with the permission of the Spanish Society for Microbiology from D. Schüler [1]. (e) NASA.

      It is easy to show [2] that for large (micron‐sized or more) particles with a diameter d and a density ρp, their terminal velocity due to gravity in a still gas with a density ρg is:

      (2.1)equation

      where η is the viscosity of the gas (η = 1.81 × 10−5 Pa s for air at Standard Conditions) and g is the acceleration due to gravity. For 1 μm diameter particles with a typical density (1000–5000 kg/m3), this gives ~0.1 mm/s. The equation, however is only valid for relatively large particles. In its derivation, it is assumed that the gas velocity at the particle surface is zero, which is invalid for very small particles whose size is less than the mean‐free path of the gas molecules. To put it crudely, very small particles “slip” through the gaps between the gas molecules and fall faster than predicted by the equation. As the particles get smaller, an increasing slip correction factor needs to be applied and this can get to be a factor of 10 or more. Even so, the fact that the terminal velocity decreases as d2 ensures that small particles do drop more slowly. Applying the slip correction factor to 10 nm diameter СКАЧАТЬ