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8/19/2019 EARTHING DESIGNE
1/17
EARTHING AND
CONSIDERATIONS FOR ITS
DESIGNPresenter : Dr. J. K. Arora
•
An earthing system is the total set of measures usedto connect an electrically conductive part of the
power system to earth.
• A well-designed earthing system ensures correct operation
of protective devices on occurrence of earth faults orlightening strikes, safety of equipment and personnel and
prevents build-up of electrostatic charges or occurrence of
dangerous induced voltages on equipments and structures.
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ROLES OF EARTHING SYSTEM
i) Correct operation of the electric network, leading
to good power quality through:• Low zero sequence impedance for return of
unbalanced fraction of three-phase ac
• Rapid and unambiguous identification of fault
conditions for efficient relay and fuse coordination
ii) To ensure electrical safety for exposed humans
and animals by:
• Fast identification of faults, leading to reducedfault duration
• Limiting touch and step voltages and resulting
body currents to safe values
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iii) To protect against lightning by:
• Limiting potential differences across electrical
insulation on stricken equipment• Providing low-impedance paths for dissipation
of stroke current energy
iv) Providing low-impedance paths for dissipation
of stroke current energy
EARTH ELECTRODEA conductor or group of bare conductors in
intimate contact with, and providing an electrical
connection to earth
Simple Electrode or combination of simple electrodes
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Figure 1. Current dissipation through soil fromlong vertical rod electrode
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IMPORTANT PARAMETERS
Efficacy of an earth electrode determined from
i) earth resistance of the electrodeii) the dangerous voltages namely maximum value of
step voltage and touch voltage
iii) transferred potential
Earth resistance - A function of i) Soil resistivity, ii)electrode geometry defined by shape, dimensions
and layout of earth conductors forming the
electrode, iii) its depth of burial, and pattern of
current dissipation in earth around the electrodeDangerous voltages depend on aforementioned factors
and magnitude of current that flows between grid
electrode and the surrounding soil
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Earth Electrodes & Earth Resistance
• Metallic rods buried vertically into earth orhorizontal bars or strips or a combination of both
• Earth resistance not due to conductors but due to
flow of current across the soil• Current flow between earth electrode near fault
to ground electrodes towards sources of current
• Current flow assumed to be flowing acrosshemispheres of increasing surface areas
• Resistivity of conductor a few micro-ohm-m,that of soil a few ohm-m to hundreds of ohm-m
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• Resistance of conductors of ground electrode is
negligible
• Resistivity of mass of soil important; at a distancewhich is about 5-10 times the extent of electrode, cross-
sectional area of current path is so large that additional
resistance of soil beyond it is very small
• Size of electrode is important; ground resistanceinversely related to size. Same material concentrated in
a small volume has larger ground resistance than when
spread over a larger area
• If soil is rocky or sandy, good option to encase the
conductors in cement concrete for good contact w soil
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PRINCIPAL DESIGN DATAi) resistivity of the soil, ii) size and shape of the
area over which grid electrode is to beinstalled, iii) magnitude of single line to earth
fault current and grid current.
Besides these, the other data needed is i)material of earth conductors and type of joints,
ii) duration of fault current, iii) special
considerations of corrosion and minimum size
of earth conductors if any, iv) shock duration,
v) resistivity of gravel layer and its depth, and
vi) type of fencing/boundary wall.
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RESISTIVITY OF SOIL
• Soil resistivity measurement is Wenner four-
probe method• Dependent on moisture content of soil, seasonal
variation near surface, but constant in deeper soil
• Earth formed from layers of different materials• Soil modification may work mostly for simple
electrodes. For a grid laid in concrete slab of say
1:3 cement:sand ratio (av. Resistivity 150 Ω-m) ,
grid at most acts like a plate electrode
• Based on interpretation of measurements,
uniform or two-layer soil model may be adopted
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i) Earth resistance R G (Ω) of the electrode in
uniform soil of resistivity ρ Ω-m, for a grid electrode
of area = A m2 is approximated by Laurent’s formula
above
ii) Increase in length of horizontally buried earthconductors by placing them closely has little affect
on earth resistance
iii) ‘ A’ is whole of contiguous area of gridiv) Substations with low resistances are not an
indication of safe design, nor is a substation with a
high resistance necessarily an indication of an unsafe
desi n
A4R
G
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EARTH FAULT CURRENT AND
GRID CURRENT
• Only faults that cause fault current to flow intoearth to be considered
• It determines magnitudes of EPR, step voltage
and touch voltage• For a single line to earth fault
)]XXX( j)R R R R 3/[( 021021f I0 = E
If = 3 I0
Standardized values of current such as 65 kA, or 40 kA, or
31.5 kAbased on three-phase current breaking capacity of
circuit breakers
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Electrode Conductor • must be able to carry the current which is to flow into
soil for the required duration of time• inefficient joint will have its own resistance causing
heating and damage at the joint
• Corrosion is dependant on presence of moisture andsalts in the soil; is a function of soil resistivity
• Use of Mild Steel avoids galvanic action with other
underground utilities, which are mostly of steel
• Area of MS conductor in mm2, tf seconds, and I amps3
f c10tKIA
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Table II. Corrosion allowance for steel earth conductors
S.
No.
Resisti
vity
(Ω– m)
Class (corrosive)
of soil%
Thickness
mil mm
1 Up to
25
Corrosive &
Severely Corrosive
30 180 4.5
0
2 > 25 <
100
Mildly &
Moderately
Corrosive
15 90 2.2
5
3 > 100 Very Mildly
Corrosive
10 30 0.7
5
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DURATION OF FAULT CURRENT AND
SHOCK DURATION
• fault duration tf for should be the maximum possiblefault clearing time including back up
• 1 second for stations using solid state or digital relaysand 3-second for stations using electromagnetic relays
• operating time of protective relays and circuit breaker isused as shock duration ts for personnel safety againstshock
• ts
taken 0.5 s for stations using digital relays and 1 s forstations using electromagnetic relays
• appropriate value applicable keeping in view the relayand circuit breaker operating times to br chosen
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RESISTIVITY OF GRAVEL LAYER AND
ITS DEPTH
• Gravel of resistivity s & thickness hs spread overareas of swyd for several reasons; one of which isincrease in earth resistance of foot and themaximum permissible values of E
step
and Etouch• Resistance modification factor is
• Instead of gravel concrete slab
09.0h2
)1(09.0
Cs
s
s
At some stations a slab of cement concrete is being tried
below gravel to prevent growth of weeds/grass. Resistivity
of gravel is important to calculate Cs.
Alternate
expressions for Cs available
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FENCING/BOUNDARY WALL
Touch voltage maximum near fence. Conductor spacing
may have to be reduced to make it safe
Touch voltage maximum between fence and a point 1
meter away outside itin area without gravel
Alternately, boundary wall topped with fence may be
considered
SOFTWARE IN EARTHING DESIGNMany formulas currently in use obtained empirically from
computer simulation results
Several limitations on use of formulas
When the conductors are unequally spaced or when thesoil model is two-la er or more use of software mandator
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132 kVSystem bus
132/33 kV transformers 132/33 kV transformers
33 kV lines
33 kV substation
11 kV line
System generator
Three-phase fault level on 132 kV bus is 31.5 kASingle line to earth fault on 33 kV bus at the distrib. s/s,
fault current = 1819 A. This current returns to the grid
station through earth, the grid current is thus 1819 A.
SLG fault on 11 kV bus at the distrib. s/s, fault current= 4617 A. No current returns to the grid station through
earth and the grid current is zero
SLG fault on 11 kV line very near to the distrib. s/s,
fault current = 2616.4 A. grid current = 2616.4 A