Page 77 - Electrical Safety of Low Voltage Systems
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60 Chapter Four
FIGURE 4.17 The
earth potential V G
assumed by the
faulty ECP .
R BG is due to the presence of the floor, whose resistance in dry con-
ditions is at least 1 k . In the absence of floor (i.e., outdoor locations),
R BG can be calculated by considering the person’s feet as two circular
plates, of radius r = 0.1 m, in parallel on the soil. Each foot/plate has
a ground resistance approximately equal to
2
∼
R Foot = = 4 (4.22)
5r
where is the superficial soil resistivity in ohm meters ( · m). Thus,
the human body resistance-to-ground R BG equals 2 . The tendency of
international standards for low-voltage installations is not to consider
the resistance of footwear, by assuming the person, conservatively,
shoeless. The presence of shoe resistance in series to the body, in fact,
would limit the body current’s circulation, benefiting the person’s
safety.
Let us assume a person standing in an area sufficiently far from the
electrodetobeconsideredatzeropotential.Inthisworst-casescenario,
be the person exposed to indirect contact by touching a faulted ECP.
Assume the ECP leaks the ground current I, so that the person’s hand
is subject to the potential V ST = V G (Fig. 4.18).
The prospective (or source) touch voltage V ST is defined as the po-
tential difference between the faulted ECP (i.e., the dryer of Fig. 4.18)
and the earth occupied by the person, at a distance of1mfromthe
ECP, 12 when the ECP is not being touched by the person.
In reality, the person touching the enclosure is not subject to the
potential difference V ST but to the touch voltage V T , which is ≤V ST .A
voltage divider, in fact, takes place between the body resistance R B
and the person resistance-to-ground R BG (Fig. 4.19).
In low-voltage systems, V T is defined as the voltage differential
which a person, 13 standing at1mfromthe grounded ECP, may be
subject to, between both hands and both feet. 14
Upon the human touch of the faulted ECP, the natural presence of
R BG causes an “elevation” of the electric potential in correspondence