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APPLICATION NOTE
FIRE-RESISTANT CABLE SIZING
Sizing of conductors supplying electrical equipment that must remain
functional during a fire
Marko Ahn, Bruno De Wachter, Franck Gyppaz, Angelo Baggini
December 2022
ECI Publication No Cu0109
Available from https://help.leonardo-energy.org
Publication No Cu0109
Issue Date: December 2022
Page i
Document Issue Control Sheet
Document Title: Application Note – Fire-resistant Cable Sizing
Publication No: Cu0109
Issue: 04
Release: Public
Content provider(s) Marko Ahn, Franck Gyppaz, Angelo Baggini
Author(s): Bruno De Wachter, Franck Gyppaz, Angelo Baggini
Editorial and language review Andrew Wilson
Content review: Marko Ahn, Franck Gyppaz, Angelo Baggini
Document History
Issue Date Purpose
1 December
2010
Initial publication written by J. Wiatr, Z.Hanzelka, D. Chapman, S. Fassbinder
2 June 2014 Reviewed by Roman Targosz
3 December
2022
Rewritten by Marko Ahn (Kabelwerk Eupen, Europacable), Angelo Baggini (University
of Bergamo), Bruno De Wachter (ECI), and Franck Gyppaz (Nexans, Europacable)
Disclaimer
While this publication has been prepared with care, European Copper Institute and other contributors provide
no warranty with regards to the content and shall not be liable for any direct, incidental or consequential
damages that may result from the use of the information or the data contained.
Copyright© European Copper Institute.
Reproduction is authorized providing the material is unabridged and the source is acknowledged.
Publication No Cu0109
Issue Date: December 2022
Page ii
CONTENTS
Summary ........................................................................................................................................................ 1
Introduction.................................................................................................................................................... 2
The development of a fire............................................................................................................................... 3
Fire-resistant cables........................................................................................................................................ 4
Conductor sizing of fire-resistant cables ......................................................................................................... 5
The conductor resistance under fire conditions.....................................................................................................5
Calculating the voltage drop...................................................................................................................................6
Application in buildings............................................................................................................................7
Motor starting currents............................................................................................................................9
Assessing current-carrying capacity .......................................................................................................................9
Conclusion .................................................................................................................................................... 11
Publication No Cu0109
Issue Date: December 2022
Page 1
SUMMARY
The integrity and functionality of the electricity supply cables is vital for keeping safety services operational
during a building fire. Choosing a cable that is tested and classified as fire resistant is a first step when designing
an electrical circuit to supply equipment that must remain functional during a fire. The next step – equally
important – is to calculate the appropriate cable conductor cross section. This requires particular attention
because of the fact that electrical resistance increases sharply as temperature rises.
To calculate the electrical resistance under fire conditions, the fire temperature must be known. First, it must
be determined for how long the safety services must remain operational. The standard durations of fire
resistance classes are 30, 60, 90, and 120 minutes. When this time span is known, the fire temperature can be
derived from the standard temperature-time curve as defined in ISO 834. The electrical resistance under fire
conditions can then be obtained by applying the Wiedemann-Franz law. This will establish an electrical
resistance correction factor which facilitates the calculation of the voltage drop under fire conditions.
The voltage drop over the entire length of the supply cables must be restricted to ensure that fire safety
equipment will maintain functionality for the required length of time. Usually, the maximum voltage drop will
be specified in the equipment’s user guide. If this is not the case, one must consider a maximum voltage drop of
10%. Because buildings are often compartmentalised into fire zones, cables feeding fire protection equipment
are rarely exposed to fire temperatures over their entire length. The part of the cable not affected by the fire
will operate at normal temperature, while the part exposed to the fire will have increased resistance. The total
resistance over the whole length of the cable is calculated by applying the electrical resistance correction factor
only to that part of the cable affected. From the maximum voltage drop of the fire safety equipment, the
electrical resistance correction factor and the compartmentalisation of the cable route, the maximum electrical
resistance the cable is allowed to have at normal temperature (20°C) can be calculated. The minimum conductor
cross section can then be derived from this using Tables 1 to 4 of the international standard EN/IEC 60228, or
their equivalent in national standards.
The electrical insulation of fire-resistant cables is designed to withstand extreme temperatures, a fact which
could lead to the false assumption that there is no limit to the current-carrying capacity of these cables. In
reality, fire-resistant cables are not tested for the potential additional heat produced as a result of the increased
electrical resistance at high temperature. Moreover, any additional temperature rise above that represented by
the standard temperature-time curve (ISO 834, post-flashover fire) could bring the cable close to the melting
temperature of copper. Laboratory tests have demonstrated that this additional heat production does not affect
the cable performance up to the 90 minute mark of the ISO 834 temperature-time curve. For these cases, the
conductor cross sections and associated current-carrying capacities can be chosen based on the IEC 60364-5-52
standard for cables working under normal service conditions. If the installation must remain functional beyond
90 minutes (safety class 120), measures should be taken to avoid a loss of integrity in the cable.
The cross-section to be chosen is the highest value obtained from the voltage drop and current-carrying capacity
assessments.
Publication No Cu0109
Issue Date: December 2022
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INTRODUCTION
When there is a fire in a building, safety services should not fail. They can save the lives of occupants and
emergency workers. The first objective is to provide safe evacuation routes from the affected areas and to
ensure that all services required for firefighting are maintained for as long as necessary. Another objective may
be to ensure that services in areas not directly affected by fire are secured to provide a safe environment for
occupants who are evacuated, pending complete evacuation or the end of the incident. Preserving property is
also at stake.
The length of time for which safety services are required to operate depends on the building’s use, the number
and type of occupants, and the specifications given by national regulation and insurance companies. While it
may be feasible to evacuate a dwelling or a small office building quickly, larger or taller structures and many
public buildings will take much longer. The longer safety services can remain operational, the better the chance
of bringing a fire under control, avoiding injuries, and reducing property damage.
A prerequisite for keeping safety services operational during a fire is to maintain a reliable power supply.
Choosing a power cable tested and classified as fire resistant is a first step when designing an electrical circuit
supplying equipment that must remain functional during a fire. The second step – just as crucial – is to calculate
the minimum cable conductor cross section, which is the main subject of this application note.
Publication No Cu0109
Issue Date: December 2022
Page 3
THE DEVELOPMENT OF A FIRE
How a building fire develops depends on many factors, of which the fire load is the most important. The fire load
is the average calorific value of combustible material per square metre of fire zone and is expressed in mega-
joules per square metre (MJ/m2
).
The key to being able to specify a suitable fire-resistant cable is having a sound knowledge of the temperature
rise characteristics in areas affected by the fire. Although the exact process depends on the location and fire
load, standard temperature-time curves that model typical fires have been developed. In this application note
we will use the standard temperature-time curve of post-flashover fire as defined in ISO 834. This standard curve
is the most common in the fire-testing of buildings and is used in construction products regulation (CPR) tests.
For some application areas, alternative temperature-time curves, such as hydrocarbon or tunnel curves, must
be used.
The ISO 834 standard temperature-time curve of a post-flashover fire is expressed by the formula:
𝑇𝑇 = 345 log(8𝑡𝑡 + 1) + 20
where:
T is the temperature, in °C
t is time, in minutes
FIGURE 1 – TEMPERATURE-TIME CURVE FOR A STANDARD TEMPERATURE-TIME CURVE (ISO 834, POST-FLASHOVER FIRE)
After 30 minutes of fire, the temperature is already in excess of 800°C. It will continue to rise and reach more
than 1000°C after 90 minutes.
Publication No Cu0109
Issue Date: December 2022
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FIRE-RESISTANT CABLES
There are a number of circumstances where high risk demands enhanced fire protection. These include buildings
with high numbers of occupants, especially where they are unfamiliar with their environment. The need for
enhanced protection can also depend on the nature of the activities, or risk in terms of loss of life, historic
artefacts, or economic value.
Typical locations include:
• Public buildings and spaces – cinemas, theatres, hotels, museums, transport hubs, and shopping centres
• Buildings with vulnerable occupants – schools, hospitals, and day-care centres
• Where evacuation and rescue access may be difficult – mines, tunnels
• Hazardous locations – chemical manufacturing and storage, bulk powder storage
• Sensitive infrastructure – data centres, communications facilities, banks
• High-rise buildings, where fire could spread very quickly, hampering firefighting and evacuation
The types of equipment that must be available during a fire include:
• Smoke venting systems, including pressurisation and depressurisation fans
• Electrically operated fire shutters and smoke curtains
• Firefighting lifts
• Sprinkler and wet-riser pumps
• Equipment for explosion prevention and suppression
• Command and communications systems, including audible warning devices addressing the public
• Emergency lighting
Cables commonly used for electrical installations would already suffer damage at temperatures much lower than
those experienced in a fire. For this reason, one of the following measures must be put in place:
• Protect the cables by installing them in a fire-resistant sleeve, conduit, or trunk, or
• Use cables with intrinsic fire-resistance, specifically designed for the purpose.
Cables with intrinsic fire-resistance can be used unprotected and are classified based on the minimum time they
are able “to maintain a reliable form of power supply when exposed to the conditions of the standard
temperature-time curve” (EN 13501-3 §5.1.6), expressed in minutes. The standard durations of fire resistance
are 30, 60, 90, and 120 minutes – hereunder simply called “fire safety classes”.
Calculating the minimum cable cross section for cables that must remain functional during a fire is different from
the calculations for cables operating under normal conditions. Because of the high temperatures, the electrical
resistance will be much higher. This must be taken into account when assessing the voltage drop and current-
carrying capacity. This is discussed in detail in the following chapters.
Publication No Cu0109
Issue Date: December 2022
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CONDUCTOR SIZING OF FIRE-RESISTANT CABLES
We will first calculate the electrical resistance under fire conditions, before relating it to the voltage drop and
the current carrying capacity of the cable. The appropriate conductor cross section will follow from a
combination of both assessments.
THE CONDUCTOR RESISTANCE UNDER FIRE CONDITIONS
In normal electrical applications, the resistance of a copper conductor can be calculated using the following
formula, which is valid up to about 200 °C:
𝑅𝑅 = 𝑅𝑅20(1 + 𝛼𝛼20∆𝑇𝑇)
where:
20
R is the conductor resistance at 20°C, in Ω
α20 is the temperature coefficient of resistance at 20°C, per °C. α = 0.0039 for copper
∆T = Tk – 20 is the temperature difference, in °C
Tk is the final temperature, in °C.
At temperatures higher than 200°C, the relationship between the temperature and the conductor's resistance
becomes non-linear and is given by the formula:
𝑅𝑅 = 𝑅𝑅20(1 + 𝛼𝛼20∆𝑇𝑇 + 𝛽𝛽20∆𝑇𝑇2
)
where:
β20 = 6.0 x 10-7
°C-2
Alternatively, application of the Wiedemann-Franz law yields:
𝑅𝑅 = 𝑅𝑅20 �
𝑇𝑇
𝑇𝑇20
�
1.16
= 𝑅𝑅20 �
𝑇𝑇
293
�
1.16
where:
R is the resistance at temperature T
R20 is the resistance at 20°C (293 K)
T is the temperature in K (i.e., temperature in °C + 273)
Neither formula are exact laws of physics, but they are both useful approximations. The minor differences in
outcomes of the two formulae, and their slight variance with physical reality, are negligible compared to the
range of uncertainties involved in modelling a fire situation.
Using the Wiedemann-Franz law, the correction factor m to be applied when calculating the electrical resistance
at fire temperature Ty (in K) compared to the resistance at base temperature Tx (in K) can be obtained from:
𝑚𝑚𝑥𝑥 = �
𝑇𝑇𝑦𝑦
𝑇𝑇𝑥𝑥
�
1.16
Publication No Cu0109
Issue Date: December 2022
Page 6
FIGURE 2 – EVOLUTION OF THE ELECTRICAL RESISTANCE, RELATIVE TO THE ELECTRICAL RESISTANCE AT 20°C, OF A CABLE SUBJECTED TO
A STANDARD TEMPERATURE-TIME CURVE. AFTER 120 MINUTES, THE ELECTRICAL RESISTANCE IS ALMOST 6 TIMES HIGHER.
CALCULATING THE VOLTAGE DROP
To ensure that all fire safety equipment will maintain its functionality for the required length of time, the voltage
drop in the cable supplying it must be restricted. Usually, the maximum voltage drop will be specified in the
equipment’s user guide. If this is not the case, one must consider a maximum voltage drop of 10%.
Since the voltage drop is caused by the energy losses over the entire length of the cable, those losses must be
restricted. This can be done by choosing an adequate cable cross section.
The voltage drop can be calculated from the following formulae for single-phase and three-phase circuits:
1/ for a single-phase circuit:
∆𝑈𝑈 = 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 . (𝑅𝑅𝑓𝑓 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼 = 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 . (𝑅𝑅20 .
𝑅𝑅𝑓𝑓
𝑅𝑅20
. cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼
2/ for a three-phase circuit:
∆𝑈𝑈 = √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. (𝑅𝑅𝑓𝑓 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼 = √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. (𝑅𝑅20.
𝑅𝑅𝑓𝑓
𝑅𝑅20
. cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼
where:
𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 is the total cable length
Rf is the electrical resistance per cable length in case of a fire
Cos ϕ is the power factor
Publication No Cu0109
Issue Date: December 2022
Page 7
𝜔𝜔 is the radial frequency
L is the inductance per cable length
R20 is the electrical resistance per cable length at 20°C
I is the rated current
The relation between the resistance at 20°C (R20) and the cable cross section is given in national standards and
in Tables 1 to 4 of IEC/EN 60228.
The quotient
𝑅𝑅𝑓𝑓
𝑅𝑅20
is given by the correction factor m20.
APPLICATION IN BUILDINGS
Because buildings are often compartmentalised into fire zones, cables feeding fire protection equipment are
rarely exposed to fire temperatures over their entire length. The part of the cable not affected by the fire will
operate at normal temperature, while that exposed to fire will have increased electrical resistance. The task of
the designer is to assess which areas may be simultaneously affected by fire in the worst-case scenario, and
what proportion of the cable runs through those affected areas. The total conductor resistance is then calculated
by assuming normal resistance for the length unaffected by fire and applying the correction factor m to the
length that is affected by fire. This means the total correction factor q20 can be calculated from:
𝒒𝒒𝟐𝟐𝟐𝟐 =
𝑹𝑹𝑻𝑻
𝑹𝑹𝟐𝟐𝟐𝟐
=
�(𝟏𝟏𝟏𝟏𝟏𝟏−𝒚𝒚)+(𝒚𝒚 . 𝒎𝒎𝟐𝟐𝟐𝟐)�
𝟏𝟏𝟏𝟏𝟏𝟏
(EQUATION 1)
where:
y is the percentage of the cable length estimated to be affected by fire
m20 is the electrical resistance correction factor, relative to the value at 20°C
The value of m20 at 30, 60, 90 and 120 minutes of the standard cellulosic curve are shown in Table 1.
TABLE 1
The resulting values of q20 are given in Table 2.
30' (842°C) 60' (945°C) 90' (1006°C) 120' (1049°C)
Electrical resistance correction factor m20,
relative to the resistance of a cable specified at 20°C
4.71 5.22 5.53 5.74
Fire resistance class, standard temperature-time curve
(ISO 834)
Publication No Cu0109
Issue Date: December 2022
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TABLE 2
With this, we can write the voltage drop formulae as follows:
1/ for a single-phase circuit:
∆𝑈𝑈 = 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 . (𝑅𝑅20 . 𝑞𝑞20 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼
2/ for a three-phase circuit:
∆𝑈𝑈 = √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. (𝑅𝑅20 . 𝑞𝑞20 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼
The maximum electrical resistance at 20°C (R20) that will limit the voltage drop to ∆𝑈𝑈 under fire conditions can
be calculated from:
1/ for a single-phase circuit:
𝑅𝑅20 =
∆𝑈𝑈
2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑
−
𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑
𝑞𝑞20 . cos 𝜑𝜑
2/ for a three-phase circuit:
𝑅𝑅20 =
∆𝑈𝑈
√3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑
−
𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑
𝑞𝑞20 . cos 𝜑𝜑
For conductor cross sections less than 16 mm², the inductive part may be ignored.
For cross sections greater than 16 mm², 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 can be approximated by the value 0.048 in all cases.
Following on from this:
1/ for a single-phase circuit:
𝑅𝑅20 =
∆𝑈𝑈
2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑
−
0.048
𝑞𝑞20 . cos 𝜑𝜑
2/ for a three-phase circuit:
Proportion in hot zone
10% 1.37 1.42 1.45 1.47
20% 1.74 1.84 1.91 1.95
30% 2.11 2.27 2.36 2,42
40% 2.48 2.69 2.81 2.90
50% 2.85 3.11 3.26 3.37
60% 3.23 3.53 3.72 3.84
70% 3.60 3.95 4.17 4.32
80% 3.97 4.38 4.62 4.79
90% 4,34 4.80 5.08 5.27
100% 4.71 5.22 5.53 5.74
Correction factor q20
Fire safety class (minutes)
30' 60' 90' 120'
Publication No Cu0109
Issue Date: December 2022
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𝑅𝑅20 =
∆𝑈𝑈
√3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑
−
0.048
𝑞𝑞20 . cos 𝜑𝜑
With q20 given by Table 2, or calculated by Equation 1 (and m20, given by Table 1).
When the maximum voltage drop ∆𝑈𝑈 is known, the formulae above give the maximum electrical resistance R20.
The appropriate cable cross section associated with R20 can be obtained from national standards, or from Tables
1 to 4 of IEC/EN 60228.
Consulting the cable manufacturer is advised to validate these calculations. Depending on national regulations,
some modification may be necessary.
MOTOR STARTING CURRENTS
Electric motors draw starting currents many times greater than the running current. Fire pump motors are not
usually equipped with soft starters or variable speed drives to mitigate this phenomenon. Add to this the
increased electrical resistance under fire conditions, and these currents could lead to a voltage drop that is too
great for the motors to continue their start-up. Fire safety circuits must be designed to avoid such failures.
Squirrel-cage induction motors are often used to drive fire pumps because of their simple construction and good
reliability. For this type of motor, and in the working conditions of a fire pump, the voltage drop must in no
scenario exceed 10%. This figure is to be taken as an initial indication; the exact maximum permissible voltage
drop value will be indicated in the motor’s user guide and/or in the national regulation.
ASSESSING CURRENT-CARRYING CAPACITY
The IEC 60364-5-52 standard stipulates the maximum current-carrying capacity for cables working under normal
service conditions, depending on the nominal cross-section of the conductor(s), the type of electrical insulation,
and the installation method. The limiting factor is the maximum temperature the cable insulation can withstand
– typically 70°C or 90°C. In the case of fire-resistant cables, the electrical insulation is designed to withstand
extreme temperatures for a defined duration (30, 60, 90 or 120 minutes), which could lead to the false
assumption that there is no limit in the current-carrying capacity of those cables.
In reality, Joule losses might cause fire resistant cables to reach higher temperatures than those they were
designed for, since the prevailing testing protocols described in the standards do not fully take into account the
potential additional heat production caused by the increased electrical resistance at high temperature combined
with the reduced heat dissipation under fire conditions.
Indeed, the cable’s thermal balance depends on:
• Internal heat production due to electrical losses (Joule losses), and
• Heating or heat dissipation through radiation, convection, and conduction.
The Joule losses are proportional to the square of the current. In fire conditions, their contribution to the cable’s
thermal balance will be more significant due to:
• The increased electrical resistance at high temperature, and
• The reduced heat exchange with the cable surroundings due to the high temperature of flames.
The Joule losses could consequently result in a cable temperature surpassing the maximum value it was designed
for, in particular towards the end of the duration corresponding to the safety class under consideration. To
investigate whether this could affect cable performance, laboratory tests were carried out at Nexans in Lyon,
France in November 2022, while a second series of tests is due to be carried out in a different laboratory in the
first half of 2023 to validate the results.
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Issue Date: December 2022
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The tests were carried out on:
• 1.5 mm2
fire-resistant cables carrying 25 A
• 4 mm2
fire-resistant cables carrying 45 A
They followed the standard temperature-time curve of a post-flashover fire as defined in ISO 834.
The tests revealed that, up to 90 minutes, the Joule losses do not affect the performance of the copper
conductors. After that time, they lead to a conductor temperature approaching the copper melting point,
causing the conductor to break. If the installation must remain functional beyond 90 minutes (safety class 120),
measures should be taken to avoid such a loss of integrity in the cable. It is highly recommended to consult cable
manufacturers or fire engineers who can assist in modelling the thermal balance of the cable under fire
conditions according to the IEC 60287-1 analytical method. Subsequently, the conductor cross-section can be
increased until the impact of the Joule losses on the thermal balance is sufficiently minimized. This measure can
be combined with the installation of additional support structures to reduce the mechanical stress on the cable.
Up to safety class 90, following the IEC 60364-5-52 standard for cables under normal working conditions is
sufficient to guarantee the current-carrying capacity, with no further calculations required.
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CONCLUSION
Just as cables used in normal operating conditions, fire resistant cables must have a minimum conductor cross
section to ensure that the voltage drop is restricted and the current-carrying capacity guaranteed. When making
calculations, however, the increased electrical resistance at high temperature must be taken into account.
1. Limiting the voltage drop
The maximum voltage drop ∆𝑈𝑈 will normally be specified in the user guides of the fire safety
equipment. If this is not the case, one must consider a maximum voltage drop of 10%. The associated
maximum electrical resistance at 20°C (R20) can be calculated from:
For a single-phase circuit:
𝑅𝑅20 =
∆𝑈𝑈
2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑
−
0.048
𝑞𝑞20 . cos 𝜑𝜑
For a three-phase circuit:
𝑅𝑅20 =
∆𝑈𝑈
√3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑
−
0.048
𝑞𝑞20 . cos 𝜑𝜑
where:
𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 is the total cable length
Cos ϕ is the power factor
I is the rated current of the circuit
q20 is the electrical resistance correction factor under fire conditions, compared to 20°C
For cables smaller than 16 mm2
, the last term of the equation (0.048/q20 . cos 𝜑𝜑) can be ignored.
The value of q20 can be obtained from Table 2 or from:
𝑞𝑞20 =
�(100 − 𝑦𝑦) + (𝑦𝑦 . 𝑚𝑚20)�
100
where:
y is the percentage of the cable length estimated to be affected by fire, taking
compartmentalisation into account
m20 is the electrical resistance correction factor, relative to the value at 20°C; see Table 1 for a
standard cellulosic curve
The maximum cross section associated with R20 can be obtained from national standards for cables
operating under normal service conditions, or from Tables 1 to 4 of IEC/EN 60228.
2. Ensuring the current-carrying capacity
Up to 90-minute mark of the standard temperature-time curve as defined in ISO 834, the Joule losses do
not affect the performance of the copper conductors. The IEC 60364-5-52 standard for cables under normal
working conditions is sufficient to guarantee the current-carrying capacity.
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Issue Date: December 2022
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After that time (safety class 120), the Joule effect, combined with the fire conditions, lead to a conductor
temperature approaching the copper melting point, with the risk of cable breakage. If safety class 120
applies, it is highly recommended to consult cable manufacturers or fire engineers who can assist in
modelling the thermal balance of the cable and formulating the required measures.
3. Determining the minimum cable cross section
The cross-section to be chosen is the higher of the two values from assessments 1 and 2.

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Fire-Resistant Cable Sizing of conductors supplying electrical equipment that must remain functional during a fire

  • 1. APPLICATION NOTE FIRE-RESISTANT CABLE SIZING Sizing of conductors supplying electrical equipment that must remain functional during a fire Marko Ahn, Bruno De Wachter, Franck Gyppaz, Angelo Baggini December 2022 ECI Publication No Cu0109 Available from https://help.leonardo-energy.org
  • 2. Publication No Cu0109 Issue Date: December 2022 Page i Document Issue Control Sheet Document Title: Application Note – Fire-resistant Cable Sizing Publication No: Cu0109 Issue: 04 Release: Public Content provider(s) Marko Ahn, Franck Gyppaz, Angelo Baggini Author(s): Bruno De Wachter, Franck Gyppaz, Angelo Baggini Editorial and language review Andrew Wilson Content review: Marko Ahn, Franck Gyppaz, Angelo Baggini Document History Issue Date Purpose 1 December 2010 Initial publication written by J. Wiatr, Z.Hanzelka, D. Chapman, S. Fassbinder 2 June 2014 Reviewed by Roman Targosz 3 December 2022 Rewritten by Marko Ahn (Kabelwerk Eupen, Europacable), Angelo Baggini (University of Bergamo), Bruno De Wachter (ECI), and Franck Gyppaz (Nexans, Europacable) Disclaimer While this publication has been prepared with care, European Copper Institute and other contributors provide no warranty with regards to the content and shall not be liable for any direct, incidental or consequential damages that may result from the use of the information or the data contained. Copyright© European Copper Institute. Reproduction is authorized providing the material is unabridged and the source is acknowledged.
  • 3. Publication No Cu0109 Issue Date: December 2022 Page ii CONTENTS Summary ........................................................................................................................................................ 1 Introduction.................................................................................................................................................... 2 The development of a fire............................................................................................................................... 3 Fire-resistant cables........................................................................................................................................ 4 Conductor sizing of fire-resistant cables ......................................................................................................... 5 The conductor resistance under fire conditions.....................................................................................................5 Calculating the voltage drop...................................................................................................................................6 Application in buildings............................................................................................................................7 Motor starting currents............................................................................................................................9 Assessing current-carrying capacity .......................................................................................................................9 Conclusion .................................................................................................................................................... 11
  • 4. Publication No Cu0109 Issue Date: December 2022 Page 1 SUMMARY The integrity and functionality of the electricity supply cables is vital for keeping safety services operational during a building fire. Choosing a cable that is tested and classified as fire resistant is a first step when designing an electrical circuit to supply equipment that must remain functional during a fire. The next step – equally important – is to calculate the appropriate cable conductor cross section. This requires particular attention because of the fact that electrical resistance increases sharply as temperature rises. To calculate the electrical resistance under fire conditions, the fire temperature must be known. First, it must be determined for how long the safety services must remain operational. The standard durations of fire resistance classes are 30, 60, 90, and 120 minutes. When this time span is known, the fire temperature can be derived from the standard temperature-time curve as defined in ISO 834. The electrical resistance under fire conditions can then be obtained by applying the Wiedemann-Franz law. This will establish an electrical resistance correction factor which facilitates the calculation of the voltage drop under fire conditions. The voltage drop over the entire length of the supply cables must be restricted to ensure that fire safety equipment will maintain functionality for the required length of time. Usually, the maximum voltage drop will be specified in the equipment’s user guide. If this is not the case, one must consider a maximum voltage drop of 10%. Because buildings are often compartmentalised into fire zones, cables feeding fire protection equipment are rarely exposed to fire temperatures over their entire length. The part of the cable not affected by the fire will operate at normal temperature, while the part exposed to the fire will have increased resistance. The total resistance over the whole length of the cable is calculated by applying the electrical resistance correction factor only to that part of the cable affected. From the maximum voltage drop of the fire safety equipment, the electrical resistance correction factor and the compartmentalisation of the cable route, the maximum electrical resistance the cable is allowed to have at normal temperature (20°C) can be calculated. The minimum conductor cross section can then be derived from this using Tables 1 to 4 of the international standard EN/IEC 60228, or their equivalent in national standards. The electrical insulation of fire-resistant cables is designed to withstand extreme temperatures, a fact which could lead to the false assumption that there is no limit to the current-carrying capacity of these cables. In reality, fire-resistant cables are not tested for the potential additional heat produced as a result of the increased electrical resistance at high temperature. Moreover, any additional temperature rise above that represented by the standard temperature-time curve (ISO 834, post-flashover fire) could bring the cable close to the melting temperature of copper. Laboratory tests have demonstrated that this additional heat production does not affect the cable performance up to the 90 minute mark of the ISO 834 temperature-time curve. For these cases, the conductor cross sections and associated current-carrying capacities can be chosen based on the IEC 60364-5-52 standard for cables working under normal service conditions. If the installation must remain functional beyond 90 minutes (safety class 120), measures should be taken to avoid a loss of integrity in the cable. The cross-section to be chosen is the highest value obtained from the voltage drop and current-carrying capacity assessments.
  • 5. Publication No Cu0109 Issue Date: December 2022 Page 2 INTRODUCTION When there is a fire in a building, safety services should not fail. They can save the lives of occupants and emergency workers. The first objective is to provide safe evacuation routes from the affected areas and to ensure that all services required for firefighting are maintained for as long as necessary. Another objective may be to ensure that services in areas not directly affected by fire are secured to provide a safe environment for occupants who are evacuated, pending complete evacuation or the end of the incident. Preserving property is also at stake. The length of time for which safety services are required to operate depends on the building’s use, the number and type of occupants, and the specifications given by national regulation and insurance companies. While it may be feasible to evacuate a dwelling or a small office building quickly, larger or taller structures and many public buildings will take much longer. The longer safety services can remain operational, the better the chance of bringing a fire under control, avoiding injuries, and reducing property damage. A prerequisite for keeping safety services operational during a fire is to maintain a reliable power supply. Choosing a power cable tested and classified as fire resistant is a first step when designing an electrical circuit supplying equipment that must remain functional during a fire. The second step – just as crucial – is to calculate the minimum cable conductor cross section, which is the main subject of this application note.
  • 6. Publication No Cu0109 Issue Date: December 2022 Page 3 THE DEVELOPMENT OF A FIRE How a building fire develops depends on many factors, of which the fire load is the most important. The fire load is the average calorific value of combustible material per square metre of fire zone and is expressed in mega- joules per square metre (MJ/m2 ). The key to being able to specify a suitable fire-resistant cable is having a sound knowledge of the temperature rise characteristics in areas affected by the fire. Although the exact process depends on the location and fire load, standard temperature-time curves that model typical fires have been developed. In this application note we will use the standard temperature-time curve of post-flashover fire as defined in ISO 834. This standard curve is the most common in the fire-testing of buildings and is used in construction products regulation (CPR) tests. For some application areas, alternative temperature-time curves, such as hydrocarbon or tunnel curves, must be used. The ISO 834 standard temperature-time curve of a post-flashover fire is expressed by the formula: 𝑇𝑇 = 345 log(8𝑡𝑡 + 1) + 20 where: T is the temperature, in °C t is time, in minutes FIGURE 1 – TEMPERATURE-TIME CURVE FOR A STANDARD TEMPERATURE-TIME CURVE (ISO 834, POST-FLASHOVER FIRE) After 30 minutes of fire, the temperature is already in excess of 800°C. It will continue to rise and reach more than 1000°C after 90 minutes.
  • 7. Publication No Cu0109 Issue Date: December 2022 Page 4 FIRE-RESISTANT CABLES There are a number of circumstances where high risk demands enhanced fire protection. These include buildings with high numbers of occupants, especially where they are unfamiliar with their environment. The need for enhanced protection can also depend on the nature of the activities, or risk in terms of loss of life, historic artefacts, or economic value. Typical locations include: • Public buildings and spaces – cinemas, theatres, hotels, museums, transport hubs, and shopping centres • Buildings with vulnerable occupants – schools, hospitals, and day-care centres • Where evacuation and rescue access may be difficult – mines, tunnels • Hazardous locations – chemical manufacturing and storage, bulk powder storage • Sensitive infrastructure – data centres, communications facilities, banks • High-rise buildings, where fire could spread very quickly, hampering firefighting and evacuation The types of equipment that must be available during a fire include: • Smoke venting systems, including pressurisation and depressurisation fans • Electrically operated fire shutters and smoke curtains • Firefighting lifts • Sprinkler and wet-riser pumps • Equipment for explosion prevention and suppression • Command and communications systems, including audible warning devices addressing the public • Emergency lighting Cables commonly used for electrical installations would already suffer damage at temperatures much lower than those experienced in a fire. For this reason, one of the following measures must be put in place: • Protect the cables by installing them in a fire-resistant sleeve, conduit, or trunk, or • Use cables with intrinsic fire-resistance, specifically designed for the purpose. Cables with intrinsic fire-resistance can be used unprotected and are classified based on the minimum time they are able “to maintain a reliable form of power supply when exposed to the conditions of the standard temperature-time curve” (EN 13501-3 §5.1.6), expressed in minutes. The standard durations of fire resistance are 30, 60, 90, and 120 minutes – hereunder simply called “fire safety classes”. Calculating the minimum cable cross section for cables that must remain functional during a fire is different from the calculations for cables operating under normal conditions. Because of the high temperatures, the electrical resistance will be much higher. This must be taken into account when assessing the voltage drop and current- carrying capacity. This is discussed in detail in the following chapters.
  • 8. Publication No Cu0109 Issue Date: December 2022 Page 5 CONDUCTOR SIZING OF FIRE-RESISTANT CABLES We will first calculate the electrical resistance under fire conditions, before relating it to the voltage drop and the current carrying capacity of the cable. The appropriate conductor cross section will follow from a combination of both assessments. THE CONDUCTOR RESISTANCE UNDER FIRE CONDITIONS In normal electrical applications, the resistance of a copper conductor can be calculated using the following formula, which is valid up to about 200 °C: 𝑅𝑅 = 𝑅𝑅20(1 + 𝛼𝛼20∆𝑇𝑇) where: 20 R is the conductor resistance at 20°C, in Ω α20 is the temperature coefficient of resistance at 20°C, per °C. α = 0.0039 for copper ∆T = Tk – 20 is the temperature difference, in °C Tk is the final temperature, in °C. At temperatures higher than 200°C, the relationship between the temperature and the conductor's resistance becomes non-linear and is given by the formula: 𝑅𝑅 = 𝑅𝑅20(1 + 𝛼𝛼20∆𝑇𝑇 + 𝛽𝛽20∆𝑇𝑇2 ) where: β20 = 6.0 x 10-7 °C-2 Alternatively, application of the Wiedemann-Franz law yields: 𝑅𝑅 = 𝑅𝑅20 � 𝑇𝑇 𝑇𝑇20 � 1.16 = 𝑅𝑅20 � 𝑇𝑇 293 � 1.16 where: R is the resistance at temperature T R20 is the resistance at 20°C (293 K) T is the temperature in K (i.e., temperature in °C + 273) Neither formula are exact laws of physics, but they are both useful approximations. The minor differences in outcomes of the two formulae, and their slight variance with physical reality, are negligible compared to the range of uncertainties involved in modelling a fire situation. Using the Wiedemann-Franz law, the correction factor m to be applied when calculating the electrical resistance at fire temperature Ty (in K) compared to the resistance at base temperature Tx (in K) can be obtained from: 𝑚𝑚𝑥𝑥 = � 𝑇𝑇𝑦𝑦 𝑇𝑇𝑥𝑥 � 1.16
  • 9. Publication No Cu0109 Issue Date: December 2022 Page 6 FIGURE 2 – EVOLUTION OF THE ELECTRICAL RESISTANCE, RELATIVE TO THE ELECTRICAL RESISTANCE AT 20°C, OF A CABLE SUBJECTED TO A STANDARD TEMPERATURE-TIME CURVE. AFTER 120 MINUTES, THE ELECTRICAL RESISTANCE IS ALMOST 6 TIMES HIGHER. CALCULATING THE VOLTAGE DROP To ensure that all fire safety equipment will maintain its functionality for the required length of time, the voltage drop in the cable supplying it must be restricted. Usually, the maximum voltage drop will be specified in the equipment’s user guide. If this is not the case, one must consider a maximum voltage drop of 10%. Since the voltage drop is caused by the energy losses over the entire length of the cable, those losses must be restricted. This can be done by choosing an adequate cable cross section. The voltage drop can be calculated from the following formulae for single-phase and three-phase circuits: 1/ for a single-phase circuit: ∆𝑈𝑈 = 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 . (𝑅𝑅𝑓𝑓 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼 = 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 . (𝑅𝑅20 . 𝑅𝑅𝑓𝑓 𝑅𝑅20 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼 2/ for a three-phase circuit: ∆𝑈𝑈 = √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. (𝑅𝑅𝑓𝑓 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼 = √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. (𝑅𝑅20. 𝑅𝑅𝑓𝑓 𝑅𝑅20 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼 where: 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 is the total cable length Rf is the electrical resistance per cable length in case of a fire Cos ϕ is the power factor
  • 10. Publication No Cu0109 Issue Date: December 2022 Page 7 𝜔𝜔 is the radial frequency L is the inductance per cable length R20 is the electrical resistance per cable length at 20°C I is the rated current The relation between the resistance at 20°C (R20) and the cable cross section is given in national standards and in Tables 1 to 4 of IEC/EN 60228. The quotient 𝑅𝑅𝑓𝑓 𝑅𝑅20 is given by the correction factor m20. APPLICATION IN BUILDINGS Because buildings are often compartmentalised into fire zones, cables feeding fire protection equipment are rarely exposed to fire temperatures over their entire length. The part of the cable not affected by the fire will operate at normal temperature, while that exposed to fire will have increased electrical resistance. The task of the designer is to assess which areas may be simultaneously affected by fire in the worst-case scenario, and what proportion of the cable runs through those affected areas. The total conductor resistance is then calculated by assuming normal resistance for the length unaffected by fire and applying the correction factor m to the length that is affected by fire. This means the total correction factor q20 can be calculated from: 𝒒𝒒𝟐𝟐𝟐𝟐 = 𝑹𝑹𝑻𝑻 𝑹𝑹𝟐𝟐𝟐𝟐 = �(𝟏𝟏𝟏𝟏𝟏𝟏−𝒚𝒚)+(𝒚𝒚 . 𝒎𝒎𝟐𝟐𝟐𝟐)� 𝟏𝟏𝟏𝟏𝟏𝟏 (EQUATION 1) where: y is the percentage of the cable length estimated to be affected by fire m20 is the electrical resistance correction factor, relative to the value at 20°C The value of m20 at 30, 60, 90 and 120 minutes of the standard cellulosic curve are shown in Table 1. TABLE 1 The resulting values of q20 are given in Table 2. 30' (842°C) 60' (945°C) 90' (1006°C) 120' (1049°C) Electrical resistance correction factor m20, relative to the resistance of a cable specified at 20°C 4.71 5.22 5.53 5.74 Fire resistance class, standard temperature-time curve (ISO 834)
  • 11. Publication No Cu0109 Issue Date: December 2022 Page 8 TABLE 2 With this, we can write the voltage drop formulae as follows: 1/ for a single-phase circuit: ∆𝑈𝑈 = 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 . (𝑅𝑅20 . 𝑞𝑞20 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼 2/ for a three-phase circuit: ∆𝑈𝑈 = √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. (𝑅𝑅20 . 𝑞𝑞20 . cos 𝜑𝜑 + 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 ) . 𝐼𝐼 The maximum electrical resistance at 20°C (R20) that will limit the voltage drop to ∆𝑈𝑈 under fire conditions can be calculated from: 1/ for a single-phase circuit: 𝑅𝑅20 = ∆𝑈𝑈 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑 − 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 𝑞𝑞20 . cos 𝜑𝜑 2/ for a three-phase circuit: 𝑅𝑅20 = ∆𝑈𝑈 √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑 − 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 𝑞𝑞20 . cos 𝜑𝜑 For conductor cross sections less than 16 mm², the inductive part may be ignored. For cross sections greater than 16 mm², 𝜔𝜔 . 𝐿𝐿 . sin 𝜑𝜑 can be approximated by the value 0.048 in all cases. Following on from this: 1/ for a single-phase circuit: 𝑅𝑅20 = ∆𝑈𝑈 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑 − 0.048 𝑞𝑞20 . cos 𝜑𝜑 2/ for a three-phase circuit: Proportion in hot zone 10% 1.37 1.42 1.45 1.47 20% 1.74 1.84 1.91 1.95 30% 2.11 2.27 2.36 2,42 40% 2.48 2.69 2.81 2.90 50% 2.85 3.11 3.26 3.37 60% 3.23 3.53 3.72 3.84 70% 3.60 3.95 4.17 4.32 80% 3.97 4.38 4.62 4.79 90% 4,34 4.80 5.08 5.27 100% 4.71 5.22 5.53 5.74 Correction factor q20 Fire safety class (minutes) 30' 60' 90' 120'
  • 12. Publication No Cu0109 Issue Date: December 2022 Page 9 𝑅𝑅20 = ∆𝑈𝑈 √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑 − 0.048 𝑞𝑞20 . cos 𝜑𝜑 With q20 given by Table 2, or calculated by Equation 1 (and m20, given by Table 1). When the maximum voltage drop ∆𝑈𝑈 is known, the formulae above give the maximum electrical resistance R20. The appropriate cable cross section associated with R20 can be obtained from national standards, or from Tables 1 to 4 of IEC/EN 60228. Consulting the cable manufacturer is advised to validate these calculations. Depending on national regulations, some modification may be necessary. MOTOR STARTING CURRENTS Electric motors draw starting currents many times greater than the running current. Fire pump motors are not usually equipped with soft starters or variable speed drives to mitigate this phenomenon. Add to this the increased electrical resistance under fire conditions, and these currents could lead to a voltage drop that is too great for the motors to continue their start-up. Fire safety circuits must be designed to avoid such failures. Squirrel-cage induction motors are often used to drive fire pumps because of their simple construction and good reliability. For this type of motor, and in the working conditions of a fire pump, the voltage drop must in no scenario exceed 10%. This figure is to be taken as an initial indication; the exact maximum permissible voltage drop value will be indicated in the motor’s user guide and/or in the national regulation. ASSESSING CURRENT-CARRYING CAPACITY The IEC 60364-5-52 standard stipulates the maximum current-carrying capacity for cables working under normal service conditions, depending on the nominal cross-section of the conductor(s), the type of electrical insulation, and the installation method. The limiting factor is the maximum temperature the cable insulation can withstand – typically 70°C or 90°C. In the case of fire-resistant cables, the electrical insulation is designed to withstand extreme temperatures for a defined duration (30, 60, 90 or 120 minutes), which could lead to the false assumption that there is no limit in the current-carrying capacity of those cables. In reality, Joule losses might cause fire resistant cables to reach higher temperatures than those they were designed for, since the prevailing testing protocols described in the standards do not fully take into account the potential additional heat production caused by the increased electrical resistance at high temperature combined with the reduced heat dissipation under fire conditions. Indeed, the cable’s thermal balance depends on: • Internal heat production due to electrical losses (Joule losses), and • Heating or heat dissipation through radiation, convection, and conduction. The Joule losses are proportional to the square of the current. In fire conditions, their contribution to the cable’s thermal balance will be more significant due to: • The increased electrical resistance at high temperature, and • The reduced heat exchange with the cable surroundings due to the high temperature of flames. The Joule losses could consequently result in a cable temperature surpassing the maximum value it was designed for, in particular towards the end of the duration corresponding to the safety class under consideration. To investigate whether this could affect cable performance, laboratory tests were carried out at Nexans in Lyon, France in November 2022, while a second series of tests is due to be carried out in a different laboratory in the first half of 2023 to validate the results.
  • 13. Publication No Cu0109 Issue Date: December 2022 Page 10 The tests were carried out on: • 1.5 mm2 fire-resistant cables carrying 25 A • 4 mm2 fire-resistant cables carrying 45 A They followed the standard temperature-time curve of a post-flashover fire as defined in ISO 834. The tests revealed that, up to 90 minutes, the Joule losses do not affect the performance of the copper conductors. After that time, they lead to a conductor temperature approaching the copper melting point, causing the conductor to break. If the installation must remain functional beyond 90 minutes (safety class 120), measures should be taken to avoid such a loss of integrity in the cable. It is highly recommended to consult cable manufacturers or fire engineers who can assist in modelling the thermal balance of the cable under fire conditions according to the IEC 60287-1 analytical method. Subsequently, the conductor cross-section can be increased until the impact of the Joule losses on the thermal balance is sufficiently minimized. This measure can be combined with the installation of additional support structures to reduce the mechanical stress on the cable. Up to safety class 90, following the IEC 60364-5-52 standard for cables under normal working conditions is sufficient to guarantee the current-carrying capacity, with no further calculations required.
  • 14. Publication No Cu0109 Issue Date: December 2022 Page 11 CONCLUSION Just as cables used in normal operating conditions, fire resistant cables must have a minimum conductor cross section to ensure that the voltage drop is restricted and the current-carrying capacity guaranteed. When making calculations, however, the increased electrical resistance at high temperature must be taken into account. 1. Limiting the voltage drop The maximum voltage drop ∆𝑈𝑈 will normally be specified in the user guides of the fire safety equipment. If this is not the case, one must consider a maximum voltage drop of 10%. The associated maximum electrical resistance at 20°C (R20) can be calculated from: For a single-phase circuit: 𝑅𝑅20 = ∆𝑈𝑈 2 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑 − 0.048 𝑞𝑞20 . cos 𝜑𝜑 For a three-phase circuit: 𝑅𝑅20 = ∆𝑈𝑈 √3 . 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡. 𝐼𝐼 . 𝑞𝑞20 . cos 𝜑𝜑 − 0.048 𝑞𝑞20 . cos 𝜑𝜑 where: 𝑙𝑙𝑡𝑡𝑡𝑡𝑡𝑡 is the total cable length Cos ϕ is the power factor I is the rated current of the circuit q20 is the electrical resistance correction factor under fire conditions, compared to 20°C For cables smaller than 16 mm2 , the last term of the equation (0.048/q20 . cos 𝜑𝜑) can be ignored. The value of q20 can be obtained from Table 2 or from: 𝑞𝑞20 = �(100 − 𝑦𝑦) + (𝑦𝑦 . 𝑚𝑚20)� 100 where: y is the percentage of the cable length estimated to be affected by fire, taking compartmentalisation into account m20 is the electrical resistance correction factor, relative to the value at 20°C; see Table 1 for a standard cellulosic curve The maximum cross section associated with R20 can be obtained from national standards for cables operating under normal service conditions, or from Tables 1 to 4 of IEC/EN 60228. 2. Ensuring the current-carrying capacity Up to 90-minute mark of the standard temperature-time curve as defined in ISO 834, the Joule losses do not affect the performance of the copper conductors. The IEC 60364-5-52 standard for cables under normal working conditions is sufficient to guarantee the current-carrying capacity.
  • 15. Publication No Cu0109 Issue Date: December 2022 Page 12 After that time (safety class 120), the Joule effect, combined with the fire conditions, lead to a conductor temperature approaching the copper melting point, with the risk of cable breakage. If safety class 120 applies, it is highly recommended to consult cable manufacturers or fire engineers who can assist in modelling the thermal balance of the cable and formulating the required measures. 3. Determining the minimum cable cross section The cross-section to be chosen is the higher of the two values from assessments 1 and 2.