TN system - Earth-fault current calculation

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Three methods of calculation are commonly used:
  • The method of impedances, based on the trigonometric addition of the system resistances and inductive reactances
  • The method of composition
  • The conventional method, based on an assumed voltage drop and the use of prepared tables

Methods of determining levels of short-circuit current

In TN-earthed systems, a short-circuit to earth will, in principle, always provide sufficient current to operate an overcurrent device.
The source and supply mains impedances are much lower than those of the installation circuits, so that any restriction in the magnitude of earth-fault currents will be mainly caused by the installation conductors (long flexible leads to appliances greatly increase the “fault-loop” impedance, with a corresponding reduction of short-circuit current).

The most recent IEC recommendations for indirect-contact protection on TN earthing systems only relates maximum allowable tripping times to the nominal system voltage.(see Figure F12

The reasoning behind these recommendations is that, for TN systems, the current which must flow in order to raise the potential of an exposed conductive part to 50 V or more is so high that one of two possibilities will occur:

  • Either the fault path will blow itself clear, practically instantaneously, or
  • The conductor will weld itself into a solid fault and provide adequate current to operate overcurrent devices

To ensure correct operation of overcurrent devices in the latter case, a reasonably accurate assessment of short-circuit earth-fault current levels must be determined at the design stage of a project.

A rigorous analysis requires the use of phase-sequence-component techniques applied to every circuit in turn. The principle is straightforward, but the amount of computation is not considered justifiable, especially since the zero-phase-sequence impedances are extremely difficult to determine with any reasonable degree of accuracy in an average LV installation.

Other simpler methods of adequate accuracy are preferred. Three practical methods are:

  • The “method of impedances”, based on the summation of all the impedances (positive-phase-sequence only) around the fault loop, for each circuit
  • The “method of composition”, which is an estimation of short-circuit current at the remote end of a loop, when the short-circuit current level at the near end of the loop is known
  • The “conventional method” of calculating the minimum levels of earth-fault currents, together with the use of tables of values for obtaining rapid results

These methods are only reliable for the case in which the cables that make up the earth-fault-current loop are in close proximity (to each other) and not separated by ferro-magnetic materials.

Method of impedances

For calculations, modern practice is to use software agreed by National Authorities, and based on the method of impedances, such as Ecodial-3. National Authorities generally also publish Guides, which include typical values, conductor lengths, etc.

This method summates the positive-sequence impedances of each item (cable, PE conductor, transformer, etc.) included in the earth-fault loop circuit from which the short-circuit earth-fault current is calculated, using the formula:
[math]\displaystyle{ I=\frac{Uo}{\sqrt{\left ( \sum R \right )^2 + \left ( \sum X \right )^2 }} }[/math] 
where
(ΣR) 2 = (the sum of all resistances in the loop)2 at the design stage of a project.
and (ΣX) 2 = (the sum of all inductive reactances in the loop)2
and Uo = nominal system phase-to-neutral voltage.
The application of the method is not always easy, because it supposes a knowledge of all parameter values and characteristics of the elements in the loop. In many cases, a national guide can supply typical values for estimation purposes.

Method of composition

This method permits the determination of the short-circuit current at the end of a loop from the known value of short-circuit at the sending end, by means of the approximate formula:
[math]\displaystyle{ Isc=I\frac{Uo}{U+Zs\ Isc} }[/math]
where
Isc = upstream short-circuit current
I = end-of-loop short-circuit current
Uo = nominal system phase voltage
Zs = impedance of loop
Note: In this method the individual impedances are added arithmetically(1) as opposed to the previous “method of impedances” procedure.

(1) This results in a calculated current value which is less than that it would actually flow. If the overcurrent settings are based on this calculated value, then operation of the relay, or fuse, is assured.

Conventional method

The maximum length of any circuit of a TN-earthed installation is: [math]\displaystyle{ \frac{0.8\ Uo\ Sph}{\rho \left ( 1+m \right )Ia} }[/math]

This method is generally considered to be sufficiently accurate to fix the upper limit of cable lengths.

Principle The principle bases the short-circuit current calculation on the assumption that the voltage at the origin of the circuit concerned (i.e. at the point at which the circuit protective device is located) remains at 80% or more of the nominal phase to neutral voltage. The 80% value is used, together with the circuit loop impedance, to compute the short-circuit current.

This coefficient takes account of all voltage drops upstream of the point considered. In LV cables, when all conductors of a 3-phase 4-wire circuit are in close proximity (which is the normal case), the inductive reactance internal to and between conductors is negligibly small compared to the cable resistance. This approximation is considered to be valid for cable sizes up to 120 mm2.
Above that size, the resistance value R is increased as follows:

Core size (mm2) Value of resistance
S = 150 mm2 R+15%
S = 185 mm2 R+20%
S = 240 mm2 R+25%

The maximum length of a circuit in a TN-earthed installation is given by the formula:
[math]\displaystyle{ Lmax=\frac{0.8\ Uo\ Sph}{\rho \left ( 1+m \right )Ia} }[/math] 
where:
Lmax = maximum length in metres
Uo = phase volts = 230 V for a 230/400 V system
ρ = resistivity at normal working temperature in ohm-mm2/metre
(= 22.5 10-3 for copper; = 36 10-3 for aluminium)
Ia = trip current setting for the instantaneous operation of a circuit-breaker, or
Ia = the current which assures operation of the protective fuse concerned, in the specified time.
[math]\displaystyle{ m=\frac{Sph}{SPE} }[/math]
Sph = cross-sectional area of the phase conductors of the circuit concerned in mm2
SPE = cross-sectional area of the protective conductor concerned in mm2.
(see Fig. F39)



FigF39.jpg

 



















Fig. F39: Calculation of L max. for a TN-earthed system, using the conventional method


Tables

The following tables give the length of circuit which must not be exceeded, in order that persons be protected against indirect contact hazards by protective devices

The following tables, applicable to TN systems, have been established according to the “conventional method” described above.
The tables give maximum circuit lengths, beyond which the ohmic resistance of the conductors will limit the magnitude of the short-circuit current to a level below that required to trip the circuit-breaker (or to blow the fuse) protecting the circuit, with sufficient rapidity to ensure safety against indirect contact.
Correction factor m
Figure F40 indicates the correction factor to apply to the values given in Figures F41 to F44, according to the ratio Sph/SPE, the type of circuit, and the conductor materials.

The tables take into account:

  • The type of protection: circuit-breakers or fuses
  • Operating-current settings
  • Cross-sectional area of phase conductors and protective conductors
  • Type of system earthing (see Fig.F45 )
  • Type of circuit-breaker (i.e. B, C or D)(1)

The tables may be used for 230/400 V systems.

Equivalent tables for protection by Compact and Multi 9 circuit-breakers (Merlin Gerin) are included in the relevant catalogues.



Circuit Conductor material m = Sph/SPE (or PEN)
m = 1 m = 2 m = 3 m = 4
3P + N or P + N Copper 1 0.67 0.50 0.40
Aluminium 0.62 0.42 0.31 0.25

Fig. F40: Correction factor to apply to the lengths given in tables F41 to F44 for TN systems


Circuits protected by general purpose circuit-breakers (Fig. F41)



Nominal cross-
sectional
area
of
conductors
Instantaneous or short-time-delayed tripping current Im (amperes)
mm2 50 63 80 100 125 160 200 250 320 400 500 560 630 700 800 875 1000 1120 1250 1600 2000 2500 3200 4000 5000 6300 8000 10000 12500
1.5 100 79 63 50 40 31 25 20 16 13 10 9 8 7 6 6 5 4 4                    
2.5 167 133 104 83 67 52 42 33 26 21 17 15 13 12 10 10 8 7 7 5 4                
4 267 212 167 133 107 83 67 53 42 33 27 24 21 19 17 15 13 12 11 8 7 5 4            
6 400 317 250 200 160 125 100 80 63 50 40 36 32 29 25 23 20 18 16 13 10 8 6 5 4        
10     417 333 267 208 167 133 104 83 67 60 53 48 42 38 33 30 27 21 17 13 10 8 7 5 4    
16         427 333 267 213 167 133 107 95 85 76 67 61 53 48 43 33 27 21 17 13 11 8 7 5 4
25             417 333 260 208 167 149 132 119 104 95 83 74 67 52 42 33 26 21 17 13 10 8 7
35               467 365 292 233 208 185 167 146 133 117 104 93 73 58 47 36 29 23 19 15 12 9
50                 495 396 317 283 251 226 198 181 158 141 127 99 79 63 49 40 32 25 20 16 13
70                       417 370 333 292 267 233 208 187 146 117 93 73 58 47 37 29 23 19
95                           452 396 362 317 283 263 198 158 127 99 79 63 50 40 32 25
120                               457 400 357 320 250 200 160 125 100 80 63 50 40 32
150                                 435 388 348 272 217 174 136 109 87 69 54 43 35
185                                   459 411 321 257 206 161 128 103 82 64 51 41
240                                       400 320 256 200 160 128 102 80 64 51

Fig. F41:  Maximum circuit lengths (in metres) for different sizes of copper conductor and instantaneous-tripping-current settings for general-purpose circuit-breakers in 230/400 V TN system with m = 1


Circuits protected by Compact or Multi 9 circuit-breakers for industrial or domestic use (Fig. F42 to Fig. F44)



Sph Rated current (A)
mm2 1
2  3 4  6 10 16  20 25 32 40  50 63 80 100 125
1.5 1200 600 400  300  200 120 75 60 48 37 30 24 19 15 12 10
2.5   1000 666 500  333 200 125 100  80 62 50 40 32  25 20 16
4      1066  800 533 320 200 160 128 100 80 64 51  40 32  26
6       1200 800  480 300 240 192 150 120 96 76 60  48 38 
10              800 500 400  320 250 200 160 127 100  80  64
16                  800 640 512 400  320  256  203 160 128 102
25                        800 625 500 400 317 250 200 160
35                             875 700  560 444  350 280 224 
50                                 760  603 475 380 304

Fig. F42:  Maximum circuit lengths (in meters) for different sizes of copper conductor and rated currents for type B (1) circuit-breakers in a 230/400 V single-phase or three-phase TN system with m = 1



Sph Rated current (A)
mm2 1
2  3 4  6 10 16  20 25 32 40  50 63 80 100 125
1.5 600 300 200 150 100 60 37 30 24 18 15 12 9 7 6 5
2.5   500 333 250 167 100 62 50  40 31  25 20 16  12 10
4      533 400  267 160 100 80 64  50 40 32  25  20 16  13 
6       600 400  240 150 120 96 75 60 48  38 30  24  19 
10           677 400 250 200  160 125 100 80 63  50  40  32 
16                 640 400 320 256 200  160  128 101 80 64  51 
25                    625 500 400 312 250 200 159  125 100 80 
35                      875  700 560 437 350  280 222  175 140 112 
50                          760 594 475 380  301  237 190 152 

Fig. F43:  Maximum circuit lengths (in metres) for different sizes of copper conductor and rated currents for type C (1) circuit-breakers in a 230/400 V single-phase or three-phase TN system with m = 1

(1) For the definition of type B and C circuit-breakers refer to chapter H

 

Sph Rated current (A)
mm2 1
2  3 4  6 10 16  20 25 32 40  50 63 80 100 125
1.5 429 214 143 107 71 43  27 21 17 13 11 9 5 3
2.5 714 357 238 179  119 71  45  36  29 22  18  14 11  7 6
4   571 381  286  190 114  71  80 46 36  29  23  18  14 11 9
6   857 571 429 286 171  107  120  69  54  43  34  27  21  17 14
10       952 714 476 284  179  200  114  89  71  57  45  36  29 23
16                762 457  286  320 183 143  114  91  73  57  46 37
25                714 446 500 286  223  179  143  113  89  71 57
35                   625 700 400 313  250  200  159  125  80 100
50                      848 543 424 339 271  215  170  136 109

Fig. F44: Maximum circuit lengths (in metres) for different sizes of copper conductor and rated currents for type D (1) circuit-breakers in a 230/400 V single-phase or three-phase TN system with m = 1

(1) For the definition of type D circuit-breaker refer to chapter H

Example
A 3-phase 4-wire (230/400 V) installation is TN-C earthed. A circuit is protected by a type B circuit-breaker rated at 63 A, and consists of an aluminium cored cable with 50 mm2 phase conductors and a neutral conductor (PEN) of 25 mm2.
What is the maximum length of circuit, below which protection of persons against indirect-contact hazards is assured by the instantaneous magnetic tripping relay of the circuit-breaker?
Figure F42 gives, for 50 mm2 and a 63 A type B circuit-breaker, 603 metres, to which must be applied a factor of 0.42 (Figure F40 for [math]\displaystyle{ m=\frac{Sph}{SPE}=2 }[/math]).
The maximum length of circuit is therefore:
603 x 0.42 = 253 metres.

Particular case where one or more exposed conductive part(s) is (are) earthed to a separate earth electrode

Protection must be provided against indirect contact by a RCD at the origin of any circuit supplying an appliance or group of appliances, the exposed conductive parts of which are connected to an independent earth electrode.
The sensitivity of the RCD must be adapted to the earth electrode resistance (RA2 in Figure F45). See specifications applicable to TT system.



FigF45.jpg

 













Fig. F45: Separate earth electrode


ru:Система TN: защита от косвенного прикосновения zh:TN系统间接接触防护

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