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SCHIRTEC - Technical Information
Transcript of SCHIRTEC - Technical Information
Lighting Protection Theory
THE LIGHTNING PHENOMENON
Lightning is the phenomenon which accompanies the discharge of atmospheric charges from cloud to cloud or from cloud to earth. As lightning seeks the
path of the least resistance, it naturally tends to follow the shortest way between cloud and earth, such as buildings or towering projections. As illustrated
positive electrical charges gather in the clouds and negative charges gather in the ground. When the attraction between these two charges are strong
enough they come together in the form of lightning.
Lightning arrester equipment, properly manufactured and installed, dissipates the charges. In temperate climates a large majority of lightning is negative downwards lightning, as the negatively-charged cloud-base discharges to the ground.
The most important parameters are the following :
Amplitude
Rise time
Decay time
Current variation rate (di/dt)
Polarity
Charge
Specific energy
Number of strikes per discharge.
The first three parameters are independent in terms of statistics .
The expected effects of the characteristic lightning parameters are as follows:
Optical effects
Acoustical effects
Electro-chemical effects
Thermal effects
Electro-dynamic effects
Electro-magnetic radiation
LIGHTNING PROTECTION
Lightning Protection system are seperated two parts ;
External Lightning Protection System (LPS) and Internal Lightning Protection System.
External Lightning Protection System - LPS
External LPS is designed for protection of structures opposite to the direct lightning strokes.
For external LPS the following three different methods are used,
Air Rod
Mesh Method
Early Streamer Emission Lightning Rods
The protection level must be calculated before one of the above mentioned methods can be chosen. (IEC 62305- 1 - 1 and standarts of Europe)
LIGHTNING PROTECTION THEORY
Requirements for the the safety of people staying at work, home etc., made it necessary that special tasks were assigned to design engineers to take care
about the quality of lightning protection system on every higher building. The main function of the lightning protection system installed on the existing
building is to capture a lightning strike and then conduct the discharge current safely to the ground. Taking the fact into consideration that there are up to
100 lightning discharges to the ground every second throughout the world, it is always possible that a lightning strike hits the place which is particulary
close and important to you. The lightning protection system exists to intercept an atmospheric discharge in order to safely convey its current to the ground.
Lightning is formed as a result of processes occurring in the storm clouds. When air masses, ice crystals, water vapour drift and interact, then electrical
charges are generated. There are two types of storms (depending on the way how they are formed):
heat storms-formed as a result of strong heating and drifting upwards of the bottom air masses.
frontal storms-caused by the impact of a front of cold air on a warm moist air mass which is lifted above the advancing cold front.
In a typical storm cloud, the positive charges are concentrated in the upper part, whereas the negative charges build up at the base of the cloud. A further
charge growth causes an escalation of the electric field intensity until it exceeds the critical value. A cloud-to-ground discharge proceeds towards the
ground (small upward discharge can also be initiated from elevated ground points and this kind of discharge is called a ground-to-cloud discharge) or
towards the neighbouring cloud, which is called cloud-to-cloud discharge. Sound and visual effects of a lightning discharge are preceded by an invisible
initiated process. A high negative cloud potential (of the order of 108 V) is conveyed towards the ground by the downward leader, with the relatively small
decline of potential in its channel. When one of the upward leaders comes into contact with the downward leader, a conductive path of ionized air is created
allowing a powerful current to flow equalizing the potential difference between the cloud and the ground. In general, lightning installations are divided into:
conventional and active ones.
Conventional lightning protection system
Conventional lightning systems are based on the protection of a structure by making an installation of horizontal or vertical air terminals which are
connected to the earth with the help of downconductors. By means of the procedure described below, it is possible to decide according to the chosen
protection level whether the lightning protection is required or not. On the ground of our observations and experiences gained in this field, we recommend to
install the lightning protection on the structure regardless of the existance of a strike hazard level.
The selection of the protection level allows to minimize the risk of damage to people as well as complex and sophisticated equipment and structures. The
higher the efficiency of a lightning conductor is, the lower the risk of damages caused by lightning strikes will become. A protection level selection depends
on the kind of building, its structure and value.
A List of the effectiveness of lightning conductor with corresponding protection levels follows below.
Protectio
n Level
Effectiveness of lightning conductor E
I 0,98
II 0,95
III 0,90
IV 0,80
The Zones of protection can be determined by the "Cone of Protection" and "Rolling Sphere" methods.
The "Cone of Protection" rule consists of placing the protected structure in the zone of protection of high vertical air terminal.
Angle α for the protection level 0.95 is a 45º "Rolling Sphere" rule, which involves rolling imaginary shperes over the structure. The outer structure contour
is described by spheres. Points between the sphere and the structure indicate the protected areas. The areas touched by the sphere are deemed to require
protection. Depending on a protection level for a structure, the different values of sphere radius have to be considered.
AIR ROD
Before a Lightning Strike hits, lonization leads to an increase of the electric field around the top of the rod and the lightning current is lead from the rod to
the ground. According to table 1, the protected area connects the level of protection according to the protective angle, the length of the rod, the height of the
rod above the surface to be protected. Air Rods are used for the mesh method and stretched technique.
This is done by connecting the Air Rods to the down conductors, while the building is covered by a mesh with down conductors. In this system the
protection stage result the distance of down conductors fixings are determined according to these distances conductors are fixed.
In the Roof system of Mesh Metod, Specially Air Terminals are used on conductors crossing points on firing roofs. On f i re resistant roofs (metal roofs
etc ...) It is not needed to use air terminals (IEC 62305)
Mesh Method Details
Protection Levels According to Height and α Angles
AIR ROD AND MESH METHOD PROCESSING CRITERIA ACCORDING TO PROTECTION LEVEL
Protection
Level
Air Rod Height (m) cage (m) Down conductor
distance (m)
20 30 45 60
I α angles 25 * * * 5x5 10
II 35 25 * * 10x10 15
III 45 35 25 * 15x15 20
IV 55 45 35 25 20x20 25
Surge Protection Theory
Overvoltage definition
Overvoltage is any voltage, whose peak value exceeds the appropriate peak value of the highest operating voltage in the LV power system. Overvoltage is
usually an accidental phenomenon, which differs in time history and the place of its occurrence. Its parameters are defined by its cause (lightning stroke,
switching in heavy-current network and so on) and also by electrical character of the circuit (wave resistance, ending impedance, discharge ability and so
on). In the past few years the range of current and voltage courses for different uses has been standardized. These courses enable implementation of
testing on equipment and constructive elements under the same conditions. In the following text the most important parameters of the most used
standardized courses will be defined (according to EN 61 643-11, IEC 60-1 and CSN 34 5640).
Peak value (amplitude) Umax,Imax
peak value is the maximal value of voltage or current
which is achieved by monitored impulse course
Front of impulse
a part of voltage or current impulse before the peak
value
Front time of current impulse T1
1,25multiple of the time interval between moments, when
actual current value rise from 10% to 90% of the peak value
Front time of voltage impulse T1
1,67multiple of the time interval between moments, when actual
voltage value rise from 30% to 90% of the peak value
Tail of impulse
a part of voltage or current impulse after the peak value
Time to half-value T2 the time interval between virtual beginning of impulse and the
moment, when observed course reduces to 50% of its peak value
Note: The virtual beginning is an intersection of time axis and bisector, which goes through points, where actual value of
the front of impulse at first time reaches partly given lower value and partly given higher value …in detail see the following two figures.
Standardized testing current impulse
two basic types of testing current impulses are used during SPD tests:
Testing impulse of lightning current Iimp(10/350) – it is used for simulation of lightning current (so-called test by lightning current)
Testing current impulse Imax(8/20) – it is used for simulation of indirect effect of lightning and switching overvoltages. Arrester must discharge
cca 17,5x higher charge during test by the testing impulse of lightning current Iimp(10/350), than during testing by the current impulse Imax(8/20) with the
same amplitude. Also resulting in a different construction of the lightning current arresters tested by the lightning current impulse Iimp(10/350) and
surge arresters tested by the current impulse Imax(8/20).
Course and parameters of lightning voltages and currents
In the chart shown below there are typical courses and parameters of lightning impulse voltages and currents, which occur in conductive parts of
landscape, building constructions and metal lines in consequence of lightning stroke (taking in account influences caused by galvanic, inductive or
capacitive coupling).The typical values of lightning impulse voltages and currents, which occur in conductive parts of landscape, building constructions and
metal lines.
Testing current impulse in the waveform of 10/350μs is most often used for simulation of currents infiltrating into power lines and electric equipment
in consequence of galvanic coupling. In case of inductive and capacitive coupling the voltage and current impulses are considera-bly shorter. The
examination of interfering lightning effects in relation to inductive surges (currents) in consequence of inductive coupling is most often carried out by
the testing current impulses in the waveform of 8/20μs. The examination of lightning effects in relation to interfering surges (currents) in
consequence of capacitive coupling is similarly carried out by the testing voltage impulses in the waveform of 1,2/50μs.
Kinds of surge couplings
Generally
Disturbing energies (e.g. voltages, currents, fields) can infiltrate into the building by ways of different couplings whereas cabling and its layout
represent an important part here.
Galvanic coupling
During near and direct lightning strokes into the lightning conductors of buildings, the overvoltage shows in consequences of a galvanic coupling. The
galvanic coupling is given by a different size of ground potentials along the building (earth electrodes, protective connection etc.)
Capacitive coupling
There is always a capacitive coupling (parasitic capac-ity) between the source of interference and the receiver. The higher the front rate of rise of the
disturbing voltage impulse (du/dt) is, the stronger its interference effect is.
Inductive coupling
There is always an inductive coupling (magnetic field) between the source of interference and the receiver. The higher the front rate of rise of the
disturbing current impulse (di/dt) activating the magnetic field is, the higher the interference effect is.
Types of overvoltage
Direct Lightning Stroke
A lightning stroke is an electric discharge between an electrically charged cloud and earth surface (earth lightning), between two or more clouds and each
other or between parts of one cloud (cloud lightning). Just a small percentage of strokes happens be tween the surface and the clouds. The lightning
strokes originate in the „storm cells“, which stretch average out up to few kilometers. Every storm cell is active for up to 30 minutes and generates from two
to three lightning strokes per minute. The storm cell often reaches the height of over 10 kilometres, whereas the bottom visible part of the clouds is
usually at the height of one to two kilometres. In the centre of the storm cell there exists a strong rising air flow, which causes separation of positive and
negative charges. The positive charge is usu-ally binded on the frazils at the top of the storm cell, while negative charge is usually binded on water drops at
the bottom of the cell. Nearby the earth the cell is charged with positive charge which is usually caused by discharge especially from forest. Beyond the
storm cells originating from the summer heat there are storm cells originating from the frontal cloudiness as a result of big air masses movement. The
storm frequency depends on the season. In summer months (July–August) there are on average 5 times more storms than in winter months
(December–February). The environmental heating up supports the storm creation. In autumn warm water near the seacoast gives the necessary energy
for the storm creation. According to IEC 1312-1:1995 and IEC 62305 it is possible to describe lightning charges by five basic parameters.
Total impoulse lightning charge Qf max.300 C
THe first stroke charge Qs max.100 C
The first stroke peak current Iimp max.200 kA
Specific energy the first stroke current W/R max.10 MJ/Ω
Rate of rise of the current di/dt max.200 kA/μs
General distribution of lightning current when an object is thunderstruck
Protection system of LV power system composited of lightning current arresters and surge arresters SPD must be able to discharge lightning currents
or their substantial parts without their damage. It is generally recommended to come out from the ohmic resistance of the building earthing, pipeline,
power distribution system and so on for the purposes of establishing current distribution going through SPD in case of direct lightning stroke into a
building protected by the outside lightning system. The following figure shows a typical example of lightning current distribution in an object hit by
direct lightning stroke.
Where an individual evaluation is not possible, it can be assumed that:
50% of the total lightning current Iimp=200kA (10/350)…. IS1= 100kA (10/350) enters the earth termination system of the LPS
(lightning protection system) of the structure considered
50% of Iimp=200kA (10/350)…. IS2= 100kA (10/350) is distributed among the services entering the structure (external conductive
parts, el.power, communication lines, etc.) The value of the current flowing in each service Ii is given by IS/n, where n is the number of the above
mentioned services (see the above figure). For evaluating the current Iv in individual conductors in unscreened cables, the cable current Iiis divided by
m, the number of conductors, i.e. Iv = Ii /m.
For shielded cables, the current will flow along the shield. Requirement on dimensioning of protective system SPD in the most usual connection of the
building and LV power system (TNC - system 230/400V/50Hz) results from this reasoning: For maximum lightning current size Iimp = 200kA (10/350) it
is enough to dimension the protective cascade of each phase conductor entering the object on cca 4% Iimp, that is on cca 8kA (10/350) in most cases.
Distribution of protected area into the lightning protection zones
The standard IEC 13 12-1 and IEC 62 305 defines the lightning protection zones LPZ from the respect of the direct even indirect lightning
effect. These zones are characteristic thanks to fundamental breaks of the electromagnetic conditions in their limited zones.
LPZ OA
Zone where items are subject to direct lightning strokes, and therefore may have to carry up to the full lightning current; the
unattenuated electromagnetic field occurs here.
LPZ OB Zone where items are not subject to direct lightning strokes, but the unattenuated electromagnetic field occurs
LPZ OCZone where items are not subject to direct lightning strokes and where currents on all conductive parts within this zone are further
reduced compared with zones 0B. In this zone the electromagnetic field may also be attenuated depending on the screening measures
LPZ 1Zone where items are not subject to direct lightning strokes and where currents on all conductive parts within this zone are further
reduced compared with zones 0B. In this zone the electromagnetic field may also be attenuated depending on the screening measures
LPZ 2
Zone where items are not subject to direct lightning strokes and where currents on all conductive parts within this zone are further
reduced compared with zones 0B. In this zone the electromagnetic field may also be attenuated depending on the screening measures
If a further reduction of conducted currents and/or elec-tromagnetic field is required, subsequent zones shall be introduced. The requirement for those
zones shall be selected according to the required environmental zones of the system to be protected. In general, the higher the number of the zones, the
lower the electromagnetic environment parameters. At the boundary of the individual zones, bonding of all metal penetrations shall be provided and
screening measures might by installed.
Note: Bonding at the boundary between LPZ 0A, LPZ 0B and LPZ 1 is defined in IEC 13 12-1 and IEC 62 305. The electromagnetic fields
inside a structure are influenced by opening windows, by currents on metal conductors (e.g. bonding bars, cable shields and tubes), and by cable routing.
The following figure shows an example for dividing a structure into several zones.
There all electric power and signal lines enter the protected volume (LPZ 1) at one point,
and are bonded to bonding bar 1 at the boundary of LPZ 0A, LPZ 0B and LPZ 1. In
addition, the lines are bonded to the internal bonding bar 2 at the boundary of LPZ 1 and
LPZ 2.
Furthermore, the outer shield 1 of the structure is bonded to bonding bar 1 and the inner
shield 2 to bonding bar 2. Where cables pass from one LPZ to another, the bonding must
be executed at each boundary. LPZ 2 is constructed in such a way that partial lightning
currents are not transferred into this volume and cannot pass through it.
The above described segmentation of the protected ob-ject into protection zones gives
possibilities of active protection of the LV power system thanks to insertion of the
protective SPDs (usually at the zone boundary LPZ 0→1and LPZ 1→2) and other
protective SPDs at the zone boundary LPZ 2→3. Standardly it is recommended to insert
so-called 1ststage protection – surge arrester class I tested by lightning current
Iimp(10/350) at the zone boundary LPZ 0→1. It is recommended to insert 2nd stage
protection - surge arrester class II tested by testing impulse Imax(8/20) at the boundary
zone LPZ 1→2. At the boundary of LPZ 2→3 and subsequently along the consequential
circuit there is also recommended to shoulder after every cca 10m by socalled 3rd
stage protection class III also tested by testing impulse Imax(8/20) or UOC. For extra
important protected equipment it is recommended to secure it by a quality continuous
surge protection class III with high-frequency filter at the boundary of LPZ 2→3. If there
are adjacent structures between which power and communication cables pass, the
earthing system shall be interconnected, and it is beneficial to have many parallel paths to
reduce current in the cables. A meshed earthing system fulfills this requirement. The
lightning currents are further reduced, e.g. by enclosing all the cables in metal conduits or
gridlike reinforced concrete ducts, which must be integrated into the meshed earthing
system.
E.S.E Lightning Conductor
SCHIRTEC E.S.E Lightning Conductor
The main function of the lightning protection system installed on the existing building is to capture a lightning stroke and then
conduct discharge current safety to the ground.
In some conditions, however the active lightning system is the only possible method to protect from direct lightning strokes. Due
to the arguments mentioned above, we recommended to use the active lightning protection whenever the conventional solution
solution is inconvenient or when the former is more preferable to the latter as in the case of the efficient protection of architect.
The lightning discharge is initiated by so-called down conductor which creates an ionised air path (downwards or upwards)
between the cloud and the ground for the necessary flow of any lightning currents.
Operating Principle:
Schirtec-A lightning conductor is formed by two armatures. One of them is connected to ground, while the other remains at
atmospheric potential. The great magnitude of the electric field during the thunderstorm produces that, although armatures are
separated by a very short distance, the difference of potential between them during lightning approaching becomes
considerable.
This difference of potential is the power supply of the lightning conductor internal device. The internal device is located in the
body of Schirtec-A and is called Variable Impedance Unit . Therefore, the device working is regulated by the atmospheric field.
The advantages of these characteristics are, on one side, that in normal conditions the device is not working, avoiding then
unnecessary stress to the components. On another side, during thunderstorms the device detects when a proper electric field
exists, and when the downward leader is approaching, because it provokes a strong and rapid increase of the atmospheric
electric field.
During normal atmospheric conditions, the charge is also neutral in every area (also at the air), and the internal device is not
working.
The first difference with a simple lightning rod starts already when storm clouds appear. Inside the components of the internal
device, equi-potential lines become very close together, causing the necessity of a strong concentration of charges at the
armature surface. The device is designed in such a way that the transitory current does not get lost, but remains as
electromagnetic fields in the components of the electrical device. The electric field value, able to ionise the air around the tip, is
reached earlier than with a simple rod, because the internal device makes the voltage increase over ground level. Then, air
charges become also a part of the internal current. Therefore, the ionised area is growing much faster than with a simple rod.
The previous phase to the formation of the upward leader is the formation of corona discharges (streamers) that propagate
towards the downward leader. One of these streamers will become the upward leader, which will propagate continuously to the
downward leader, forming then the lightning discharge path.
Inside the lightning conductor, the downward leader approaching and the strong increase of the electric field caused by it are the
factors that activate the mean function of the internal device .When the voltage between the armatures exceeds a certain value
which the circuit is designed for, then the internal trigger works, using the accumulated energy for pumping to designed for, then
the internal trigger works, using the accumulated energy for pumping to inside the ionised area. The strong and sudden
concentration of positive charges cause repellent forces in the ionised area, which break the existing border. The device has
provoked then a streamer effect, avoiding the ‘'glow regime'' that was lowering the effectiveness of a simple lightning rod.
The streamer emission under these conditions favours the upward leader formation, which will progress continuously till
reaching the downward leader, forming then the discharge path. Then, as the Schirtec-A is the point where the upward leader
was formed. It will be the receiver of the lightning strike.
Details of SCHIRTEC-A (S-A)
1. Air Terminal2. Ion Generator3. Accelerator and Atmospheric Electrodes4. Grounding Connection Terminal
Explanation Proteciton Radius Table
Here you will find an explanation on how to read the protection radius table correctly.
Protectionlevel
The protection level of the object depends on several factors such as:
if the object is inhabited or not
if the object is expolosiv or not,
material of the roof and the roof construction (wood, metall,...)
The more valuable and vulnerable the object is the higher the level of protection needed. e.g. an inhabited house, with a metal
roof could be attributed to protection class 1. A telephone pole of low value could attributed to the protection class 4. The safety
class can be calculated with our lightning risk program.
h
Installation height, the higher the lightning conductor is installed the greater the protective radius Rp (m)
Rp(m)
Radius protection, we recommend to install the lightning conductor in a height of 5 to 6 meters because you can then achieve a
high level of protection.
Protection Level Calculator
FORMULAS VALUES RESULTS
The Equivalent Collection Area of Structure
L=50
Ae=LW+6H(L+W)+9πH2
(For rectangular fields)W=30 Ae=15061.7251
H=15
Expended Lightning Frequency
Td=30
Ng=0,04.Td1.25
Nd=Ng.Ae.C1.10-6
Ng=2.8084
Ae=15061.7251 Nd=0.0423
C1=1
Accepted Lightning Frequency
C=C2.C3.C4.C5Nc=5,5.10-3/C
C1=1
C2=0.5
C3=1 Nc=0.0022
C4=1
C5=5
C=2.5
If Nd ≤ Nc...Optional Protection
If Nd>Nc...Protection Required Efficiency , E=1-(Nc/Nd)
EfficiencyE= 0.95
Active Lightning Protection Levels
E > 0,98 LEVEL I + Add
0,95 <E ≤ 0,98 LEVEL I
0,90 <E ≤ 0,95 LEVEL II
0,80 < E≤ 0,90 LEVEL III
0<E≤0,80 LEVEL IV
Example 1 for S-A:
Single-familiy-home; Protection Level 1
Example 2 for S-A:
Factoryhall; 150 m x 50m, Protection Level 1
The lightning conductor S-A has been installed at a
height of 4m.
The protection radius has to be specified according
to NF C 17-102 standard with 63m, the effective
protection is bigger, according to our test reports.
There were two lightning conductors S-A installed at a height
of 6m.
The radii overlap and provide for the entire production facility
sufficient protection.
The protection radius must be specified according to NF C
17-102 with 79m, the effective protection is bigger, according
to our test reports
Protection Radius Table
Rp(m) S-A (��L: 60m) S-AS (��L: 30m) S-DA (��L: 60m) S-DAS (��L: 45m)
h I II III IV I II III IV I II III IV I II III IV
2 31 35 39 43 19 22 25 28 31 35 39 43 25 28 32 36
The Protection Radius For SCHIRTEC E.S.E. Lightning Conductors(According to NFC 17 102)
Rp SCHIRTEC-AS(ΔL=15m)
SCHIRTEC-DAS(ΔL=45m)
SCHIRTEC-A/DA(ΔL=60m)
H(m) I II III IV I II III IV I II III IV
2 13 15 18 20 25 28 32 36 31 35 39 43
4 25 30 36 41 51 57 64 72 63 69 78 85
5 32 37 45 51 63 71 81 89 79 86 97 107
6 32 38 46 52 63 71 81 90 79 87 97 107
8 33 39 47 54 64 72 82 91 79 87 98 108
10 34 40 49 56 64 72 83 92 79 88 99 109
20 35 44 55 63 65 74 86 97 80 89 102 113
30 35 45 58 69 65 75 89 101 80 90 104 116
60 35 45 60 75 65 75 90 105 80 90 105 120
4 63 69 78 85 38 44 51 57 63 69 78 85 51 57 64 72
5 79 86 97 107 48 55 63 71 79 86 97 107 63 71 81 89
6 79 87 97 107 48 55 64 72 79 87 97 1007 63 71 81 90
8 79 87 98 108 49 56 65 73 79 87 98 108 64 72 82 91
10 79 88 99 109 49 57 66 75 79 88 99 109 64 72 83 92
20 80 89 102 113 50 59 71 81 80 89 102 113 65 74 86 97
30 80 90 104 116 50 60 73 85 80 90 104 116 65 75 89 101
60 80 90 105 120 50 60 75 90 80 90 105 120 65 75 90 105
Key:
h: Installation height
I/II/III/IV: Protectionlevel
Rp(m):Protectionradius
in m
5
6
Recommended
installation height