1963 Volume 32 Issue 5 Pages 301-309
This paper deals with the electric potential of human body measured by varying the kind of frictionable materials on which and with which one walks (carpets and foot-wear) and the manner and duration of walking in room air of 23°_??_25°C and 45_??_55% R. H. Any combination of the above factors gives the potential change approximately in the form vbw{1-exp(-t/τbw)}. The saturation potential vbw up to 3 kV is related linearly with the time constant τbw as
vbw=[vbw](1-τbw/[τbw]),
where [vbw] and [τbw] are constants.
Depending upon the rubbing being hard or light, the coordinate system seems to be ([vbw], 0) or (0, [τbw]). This phenomenon can be explained in terms of an equivalent circuit consisting of the internal resistance R that participates in the phenomenon and the load impedance R"C calculated from electric constants of the materials. From this equivalent circuit, [vbw] and [τbw] are obtained as _??_vbw and _??_τbw, respectively. Anti-static treatments such as application of surfactants and blending with rayon on carpet and conductive foot-wear are effective in lowering [vbw].
The maximum potential of our body of 3 kV by walking with highly insulated foot-wear, the full capacity of the body of 90 pF in standing on one leg and the rubbing area of 150cm2 give the charge density of 5.4esu/cm2 which is of the order of corona density of 8.4esu/cm2 on a parallel-plate condenser, suggesting that the corona discharge between carpet and foot-wear is responsible for such high density of charge in our body. When we reflect upon the fact that, for a highly insulated human. body of the capacity of 110 pF in standing on both legs to experience electric shock on the finger tip, body potential of at least 5 kV is needed, there. will be no such danger provided the room air temper-ature and humidity are not lower than the values used in this experiment. If otherwise, any foot-wear such as leather-soled shoes may conduct the generated charge to raise the body potential above the danger mark.