Abstract
The particles encountered in plastics and paints display a wide range of physical and chemical characteristics. Many of these characteristics affect both the way that the particles process during plastic or paint manufacture as well as the impact they have on the end-use properties of the plastic or paint. In this chapter, we make a broad, high-level survey of the various analytical techniques used to characterize particles, including their appearance, size distribution, elemental composition, bulk properties, and surface properties, to make the reader aware of what analytical options are available and what these options can reveal.
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Notes
- 1.
A mil is one-thousandth of an inch.
- 2.
It is remarkable that we can visually distinguish particle size differences of 30 nm. By contrast, most people are unable to visually detect the size difference of a colored billiard ball (57 mm) and the white cue ball (63.5 mm)—a difference that is over two million times greater. One can even more easily detect different colloidal gold particle sizes of the similar magnitude as the difference in TiO2 particle size, since the wavelength of light most strongly scattered by a colloidal gold particle is quite sensitive to particle size. This remarkable achievement is possible because these particle sizes are matched to visible light, and because we are capable of discerning subtle changes in color (as discussed in Chapter 5, we can distinguish roughly 10 million colors).
- 3.
For simplicity we will refer in this section to the adsorbing species as molecules, but atomic gases, such as helium, argon or krypton, absorb onto surfaces in the same way.
- 4.
The exceptions are resin particles in paints, which are organic and so are low surface energy materials.
- 5.
Following the practice of the last section, we will refer here to the interacting species as molecules, but such species can be atoms as well.
- 6.
The surface energy of a liquid is sometimes referred to as its surface tension.
- 7.
This should not be confused with the surface coverage in Eq. 2. Equation 2, on the one hand, and Eqs. 8, 9, and 11, on the other, use the symbol θ in a very different way.
- 8.
Properly speaking, we must specify the materials on both sides of a surface when discussing surface area. In situations of interest to us, the surface interface with a liquid or solid is air (or gas), and the subscripts for the symbols for liquid and solid surface energies will include the letter “g”—e.g., γlg and γsg.
- 9.
This should not be confused with the constant c in the gas adsorption equations.
- 10.
We might expect that all water would evolve at 100 °C—the boiling point of liquid water. While the end product is the same in all cases (gaseous water molecules), the starting point is different. The vaporization process—and the temperature at which it occurs—is dependent on how strongly a molecule is attached to its neighboring molecules. When the neighboring molecules are like molecules, as they are in liquid water, this process occurs at 100 °C. In other materials, the atomic environment surrounding the water molecules is different, and so, too, is the water evolution temperature.
- 11.
Light does not merely reflect from particles that are of similar size to the wavelength of light, but instead scatters from them (see Chapter 3).
- 12.
The ability of a magnetic lens to spread out an electron beam is far greater than the ability of a glass lens to spread out a light beam.
- 13.
There are still positively and negatively charged sites on the surface at the IEP, but these charges balance to give a net charge of zero. This situation is equivalent to the concept of zwitterions for discrete molecules.
- 14.
Pigmentary TiO2 particles made by the chloride process invariably have some alumina on their surfaces, which shifts the IEP to a higher value than for pure rutile (IEP = 5.2).
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Diebold, M., Backer, S.D., Niedenzu, P.M., Hester, B.R., Vanhecke, F.A.C. (2022). The Physical Properties of Small Particles. In: Pigments, Extenders, and Particles in Surface Coatings and Plastics. Springer, Cham. https://doi.org/10.1007/978-3-030-99083-1_2
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