24 Structural, Nanomechanical, and Nanotribological Characterization 1471
is not strictly controlled in terms of location of contact, it is difficult to distinguish
adifference between the topmost layer of the hair, and the portionswhich have been
mechanically damaged. However, this indifference between these regions (which
generally occur on the surface away from scale edges, and near scale edges, respec-
tively)may also be due tothe fact that physicalwear does not affect surfacepotential
in insulating samples, as discussed previously.
24.8.2 Effect of External Voltage and Humidity on Surface Potential
Samples were mounted in conductivesilver paint and an external power supply was
used to develop charge [56]. To determine environmental effects on surface charge,
relative humidity was controlled and varied.
To study the effects of external voltage and humidity, virgin, virgin treated,
chemically damaged, chemically damaged treated (1 cycle), and chemically dam-
aged treated (3 cycles) were studied at an external voltage of 0, 1, and 2V at
50% and 10% relative humidities. Representative AFM images for chemically dam-
aged and chemically damaged treated (1 cycle of conditioner) hair samples are
shown in Fig. 24.83a. It should be noted that the contrast seen around cuticle
scale edges is likely a result of the topography effect [56]. A key point shown
by these images is the existence of areas of trapped charge in the low humid-
ity samples. This is not seen in the samples measured in ambient. These areas
of trapped charge are seen as bright areas on the sample in the “averaged sur-
face potential” images. In other words, there is more contrast in the averaged sur-
face potential maps under low humidity (neglecting any contrast seen around the
scale edge) than is seen for the same samples under ambient humidity. It is im-
portant to clarify that the ‘bright areas’ are only in reference to the increase in
contrast in the surface potential map (averaged surface potential) away from the
scale edges. This is only considered for the “0 V” samples, where added external
charge does not affect the surface potential of the sample. This observation indi-
cates that water vapor in the air contributes significantly to the mobility of sur-
face charges on the hair. This result has been previously reported for macro stud-
ies on surface charge of hair [41, 57, 60]. Trapped charges are most pronounced
in the untreated samples. This suggests that conditioner treatment has a similar ef-
fect as water vapor. Even under very low humidity conditions, conditioner treat-
ment increases the mobility of surface charges, dissipating trapped charges. Fig-
ure 24.83b shows bar charts of the average surface potential change. Error bars
indicate +/- one standard deviation. It can be observed in these figures that all
samples exhibit very similar values in the 50% relative humidity scenario. This
again indicates that the water vapor in the air plays a significant role on the sur-
face charge of the hair, and also on the mobility of charge. For the 50% case it is
shown that the potential changes nearly 1V for every 1V change in applied poten-
tial. However, this is not the case for the 10% relative humidity situation. In this
case, a higher 0–1V value indicates more charge mobility and the ability to dissi-
pate charge, whereas a lower value indicates less charge mobility. This being the