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Furse, Wilford Road, Nottingham, NG2 1EB • Tel: +44 (0)115 964 3700 • Email:

enquiry@furse.com

• Web:

www.furse.com

TSC-0912 - 09.10.12

What transients are and why you need protection

The information provided in these introductory

pages follows the requirements for transient

overvoltage (surge) protection provided by both

BS EN/IEC 62305 and the latest amendment

of the IET Wiring Regulations 17th Edition,

BS 7671:2008(+A1:2011).

Transient overvoltages

Transient overvoltages are short duration, high

magnitude voltages peaks with fast rising edges,

commonly referred to as surges. Often described as a

“spike”, transient voltages can reach up to 6000 V on a

low-voltage consumer network, with no more than

millisecond duration.

Lightning strikes are the most common source of

extreme transient overvoltages where total outage of

an unprotected system can occur with damage to

cabling insulation through flashover potentially

resulting in loss of life through fire and electric shock.

However, electrical and electronic equipment is also

continually stressed by hundreds of transients that

occur every day on the power supply network through

switching operations of inductive loads such as

air-conditioning units, lift motors and transformers.

Switching transients may also occur as a result

of interrupting short-circuit currents (such as

fuses blowing).

Although switching transients are of a lower magnitude

than lightning transients, they occur more frequently

and equipment failures unexpectedly occur often after a

time delay; degradation of electronic components within

the equipment is accelerated due to the continual stress

caused by these switching transients.

Transient overvoltages, whether caused by lightning or

by electrical switching, have similar effects: disruption

(e.g. data loss, RCD tripping), degradation (reduced

equipment lifespan), damage (outright equipment

failure, particularly concerning for essential services

such as fire and security alarm systems) and downtime -

the biggest cost to any business such as lost

productivity and product spoilage, staff overtime,

delays to customers and sales lost to competitors.

Protection against lightning and

switching transients

BS EN/IEC 62305 takes account of protection measures

on metallic service lines (typically power, signal and

telecom lines) using transient overvoltage or surge

protective devices (SPDs) against both direct lightning

strikes as well as the more common indirect lightning

strikes (often described as the secondary effects of

lightning) and switching transients.

Standards such as BS EN 61643 series define the

characteristics of lightning currents and voltages to

enable reliable and repeatable testing of SPDs (as well

as lightning protection components).

Although these waveforms may differ from actual

transients, the standardized forms are based upon

years of observation and measurement (and in some

cases simulation). In general they provide a fair

approximation of the real world transient.

Transient waveforms have a fast rising edge and a

longer tail. They are described through their peak

value (or magnitude), rise time and their duration (or

fall time). The duration is measured as the time taken

for the test transient to decay to half its peak value.

The figures below illustrate the common current and

voltage waveforms that are used to test SPDs for

mains, signal and telecom lines.

Transient overvoltage

damage to the circuit

board, left, is clear to

see, but most damage

is barely visible, as

below.

Time t (µs)

Surge Voltage (kA)

0

1

2

3

4

0

300

600

900

1200

1500

1.2/50 µs Waveform

10/700 µs Waveform

2

V

peak

@t = 50 µs

V

peak

@t = 1.2 µs

V

peak

@t = 10 µs

2

V

peak

@t = 700 µs

Figures 1 & 2: The common current and voltage waveforms used to

test SPDs for mains, signal and telecom lines

Surge Current (kA)

0

10

20

30

0

200

400

600

2

800

1000

Time t (µs)

8/20 µs Waveform

I

imp

@t = 350 µs

10/350 µs Waveform

2

I

max

@t = 20 µs

I

max

@t = 8 µs

I

imp

@t = 10 µs