5.3.4 - Earth-fault loop impedance values
The over-riding requirement is that sufficient
fault current must flow in the event of an earth fault to
ensure that the protective device cuts off the supply before
dangerous shock can occur. For normal 240 V systems, there
are two levels of maximum disconnection time. These are:
For socket outlet circuits where equipment
could be tightly grasped: 0.4 s
For fixed equipment where contact is unlikely
to be so good: 5 s
The maximum disconnection time of 5 s also
applies to feeders and sub-mains.
It must be appreciated that the longest
disconnection times for protective devices, leading to the
longest shock times and the greatest danger, will be associated
with the lowest levels of fault current, and not, as is
commonly believed, the highest levels.
Where the voltage is other than 240 V,
[Table 41A] gives a range of disconnection times for socket
outlet circuits, of which the lowest is 0.1 s for voltages
exceeding 400 V.
In general, the requirement is that if
a fault of negligible impedance occurs between a phase and
earth, the earth-fault loop impedance must not be greater
than the value calculated from..
|
Zs < |
Uo |
|
|
Ia |
|
|
|
where |
Zs = |
the earth fault loop impedance (Ohms) |
|
Uo = |
the system voltage to earth(V) |
|
Ia
= |
the current causing automatic disconnection |
|
(operation of the protective
device) in the required time [A]). |
The earth fault loop values
shown in [Tables
5.1, 5.2 and 5.4] depend on the supply voltage and assume,
as shown in the Tables, a value of 240 V. Whilst it would
appear that 240 V is likely to be the value of the supply
voltage in Great Britain for the foreseeable future, it
is not impossible that different values may apply. In such
a case, the tabulated value for earth fault loop impedance
should be modified using the formula:-
|
Zs =
|
Zt x |
U |
|
|
|
U240 |
|
|
|
|
where |
Zs =
|
is the earth fault loop
impedance required for safety |
|
Zt
=
|
is the tabulated
value of earth fault loop impedance |
|
U =
|
is the actual supply
voltage |
|
U240 =
|
is the supply voltage
assumed in the Table. |
As an alternative to this calculation,
a whole series of maximum values of earth fault loop impedance
is given in
{Table 5.1} (from [Table 41B]) for disconnection within
0.4 s. The reader should not think that these values are
produced in some mysterious way - all are easily verified
using the characteristic curves {Figs
3.13 to 3.19}.
For example, consider a 20 A HRC fuse to
BS88 used in a 240 V system. The fuse characteristic is
shown in {Fig
3.15}, and indicates that disconnection in 0.4 s requires
a current of about 130 A. It is difficult (if not impossible)
to be precise about this value of current, because it is
between the 100 A and 150 A current graduations.
Using these values,
|
|
|
Zs = |
Uo
|
=
|
240
|
Ohms = 1.84 Ohms |
|
Ia
|
|
130
|
|
Reference to {Table
5.1} shows that the stated value is 1.8 Oh,s, the discrepancy
being due to the difficulty in reading the current with
accuracy. {Tables
5.1 and 5.2} give maximum earth-fault loop impedance
values for fuses and for miniature circuit breakers to give
a minimum disconnection time of 0.4 s in the event of a
zero impedance fault from phase to earth.
The reason for the inclusion of fixed equipment
as well as distribution circuits in
{Table 5.2} will become apparent later in this sub-section.
Table 5.1 - Maximum
earth-fault loop impedance for 240 V socket
---------------- outlet
circuits protected by fuses |
Fuse rating (A)
|
Maximum earth-fault loop impedance
(Ohms)
|
-
|
Cartridge
BS 88
|
Cartridge BS 1361
|
Semi-enclosed BS3036
|
5
|
-
|
10.9
|
10.0
|
6
|
8.89
|
-
|
-
|
10
|
5.33
|
-
|
-
|
15
|
-
|
3.43
|
2.67
|
20
|
1.85
|
1.78
|
1.85
|
30
|
-
|
1.20
|
1.14
|
32
|
1.09
|
-
|
-
|
40
|
0.86
|
-
|
-
|
45
|
-
|
0.60
|
0.62
|
Table 5.2 - Maximum
earth-fault loop impedance for 240 V circuits
-----------------protected
by miniature circuit breakers to give compliance
---------------- with 0.4
s disconnection time |
-
|
Maximum earth-fault loop impedance
(Ohms)
|
Device rating (A)
|
MCB
type 1
|
MCB
type 2
|
MCB
type 3
and type C
|
MCB
type B
|
MCB
type D
|
5
|
12.00
|
6.86
|
4.80
|
-
|
2.40
|
6
|
10.00
|
5.71
|
4.00
|
8.00
|
2.00
|
10
|
6.00
|
3.43
|
2.40
|
4.80
|
1.20
|
15
|
4.00
|
2.29
|
1.60
|
-
|
0.80
|
16
|
3.75
|
2.14
|
1.50
|
3.00
|
0.75
|
20
|
3.00
|
1.71
|
1.20
|
2.40
|
0.60
|
25
|
2.40
|
1.37
|
0.96
|
1.92
|
0.48
|
30
|
2.00
|
1.14
|
0.80
|
-
|
0.40
|
32
|
1.88
|
1.07
|
0.75
|
1.50
|
0.38
|
40
|
1.5
|
0.86
|
0.60
|
1.20
|
0.30
|
The severity of the electric shock received
when there is a phase to earth fault (indirect contact)
depends entirely on the impedance of the circuit protective
conductor. We saw in {3.4.3}
and {Fig
3.8} how the volt drop across the protective conductor
is applied to the person receiving the shock. Since this
volt drop is equal to fault current times protective conductor
impedance, if the protective conductor has a lower impedance
the shock voltage will he less. Thus it can be sustained
for a longer period without extreme danger.
Socket outlet circuits can therefore have
a disconnection time of up to 5 s provided that the circuit
protective conductor impedance's are no higher than shown
in {Table 5.3} for various types of protection.
The reasoning behind this set of requirements
becomes clearer if we take an example. {Table 5.3} shows
that a 40 A cartridge fuse to BS 88 must have an associated
protective conductor impedance of no more than 0.29 Ohms
if it is to comply. Now look at the time/current characteristic
for the fuse {Fig
3.15} from which we can see that the current for operation
in 5 s is about 170 A. The maximum volt drop across the
conductor (the shock voltage) is thus 170 x 0.29 or 49.3
V.
Table 5.3 - Maximum
impedance of circuit protective conductors to
---------------- allow
5 s disconnection time for socket outlets |
-
|
Maximum impedance of circuit protective
conductor
|
Rating (A)
|
Fuse BS 88
|
Fuse BS 1361
|
Fuse BS 3036
|
MCB type 1
|
MCB type 2
|
MCB type 3 & C
|
MCB type B
|
MCB type D
|
5
|
-
|
3.25
|
3.25
|
2.50
|
1.43
|
1.00
|
-
|
0.50
|
6
|
2.48
|
-
|
-
|
2.08
|
1.19
|
0.83
|
1.67
|
0.42
|
10
|
1.48
|
-
|
-
|
1.25
|
0.71
|
0.50
|
1.00
|
0.25
|
15
|
-
|
0.96
|
0.96
|
0.83
|
0.48
|
0.33
|
-
|
-
|
16
|
0.83
|
-
|
-
|
0.78
|
0.45
|
0.31
|
0.63
|
0.16
|
20
|
0.55
|
0.55
|
0.63
|
0.63
|
0.36
|
0.25
|
0.50
|
0.12
|
25
|
0.43
|
-
|
-
|
-
|
-
|
-
|
-
|
0.10
|
30
|
-
|
0.36
|
0.43
|
0.42
|
0.24
|
0.17
|
-
|
-
|
32
|
0.34
|
-
|
-
|
0.39
|
0.22
|
0.16
|
0.31
|
0.08
|
40
|
0.26
|
-
|
-
|
0.31
|
0.18
|
0.13
|
0.25
|
0.06
|
45
|
-
|
0.18
|
0.24
|
0.28
|
0.16
|
0.11
|
0.22
|
0.06
|
Table 5.4 - Maximum
earth-fault loop impedance for 240 V fixed
---------------- equipment
distribution circuits protected by fuses |
-
|
Maximum earth-fault loop impedance
|
Device rating
(A)
|
Cartridge
BS 88
|
Cartridge
BS 1361
|
Semi-enclosed
BS 3036
|
5
|
-
|
17.1
|
-
|
6
|
14.1
|
-
|
-
|
10
|
7.74
|
-
|
-
|
15
|
-
|
5.22
|
5.58
|
16
|
4.36
|
-
|
-
|
20
|
3.04
|
2.93
|
4.00
|
30
|
-
|
1.92
|
2.76
|
32
|
1.92
|
-
|
-
|
40
|
1.41
|
-
|
-
|
45
|
-
|
1.00
|
1.66
|
50
|
1.09
|
-
|
-
|
Application of the same reasoning
to all the figures gives shock voltages of less than 50
V. This limitation on the impedance of the CPC is of particular
importance in TT systems where it is likely that the resistance
of the earth electrode to the general mass of earth will
be high.
The breaking time of 5 s also applies to
fixed equipment, so the earth-fault loop impedance values
can be higher for these circuits, as well as for distribution
circuits. For fuses, the maximum values of earth-fault loop
impedance for fixed equipment are given in {Table 5.4}.
No separate values are given for miniature
circuit breakers. Examination of the time/current characteristics
{Figs
3.16 to 3.19} will reveal that there is no change at
all in the current causing operation between 0.4 s and 5
s in all cases except the Type 1. Here, the vertical characteristic
breaks off at 4 s, but this makes little difference to the
protection. In this case, the values given in {Table
5.2} can be used for fixed equipment as well as for
socket outlet circuits. An alternative is to calculate the
loop impedance as described above.