kSIST FprEN ISO 11855-2:2021
(Main)Building environment design - Embedded radiant heating and cooling systems - Part 2: Determination of the design heating and cooling capacity (ISO/FDIS 11855-2:2021)
Building environment design - Embedded radiant heating and cooling systems - Part 2: Determination of the design heating and cooling capacity (ISO/FDIS 11855-2:2021)
Umweltgerechte Gebäudeplanung - Flächenintegrierte Strahlheizungs- und -kühlsysteme - Teil 2: Bestimmung der Auslegungs-Heiz- bzw. Kühlleistung (ISO/FDIS 11855-2:2021)
Dieses Dokument legt Verfahren und Bedingungen fest, welche die Bestimmung der Wärmestromdichte von Flächenheiz- und -kühlsystemen mit Wasserdurchströmung bezüglich der Heiz- und Kühlmittel-übertemperatur für diese Systeme ermöglichen. Die Bestimmung der Wärmeleistung von Flächenheiz- und -kühlsystemen mit Wasserdurchströmung und ihrer Übereinstimmung mit diesem Dokument wird durch Berechnung nach den Planungsdokumenten und einem Modell vorgenommen. Dies ermöglicht eine einheitliche Bewertung und Berechnung von Flächenheiz- und -kühlsystemen mit Wasserdurchströmung.
Das Ergebnis daraus sind die Oberflächentemperatur und Temperaturgleichmäßigkeit der beheizten bzw. gekühlten Oberfläche, die Nenn-Wärmestromdichte zwischen dem Wasser und dem Raum, die zugehörige Nenn-Heiz- bzw. -Kühlmittelübertemperatur und das Kennlinienfeld für die Beziehung zwischen Wärme-stromdichte und den entscheidenden Variablen.
Dieses Dokument enthält ein allgemeines Verfahren, das auf der Finite-Differenzen-Methode und der Finite-Elemente-Methode und vereinfachten Berechnungsmethoden beruht, die von der Position der Rohre und der Art der Gebäudestruktur abhängig sind.
Conception de l'environnement des bâtiments - Systèmes intégrés de chauffage et de refroidissement par rayonnement - Partie 2: Détermination de la puissance calorifique et frigorifique à la conception (ISO/FDIS 11855-2:2021)
Načrtovanje notranjega okolja v stavbah - Vgrajeni sevalni ogrevalni in hladilni sistemi - 2. del: Določanje načrtovane grelne in hladilne moči (ISO/FDIS 11855-2:2021)
General Information
RELATIONS
Standards Content (sample)
SLOVENSKI STANDARD
oSIST prEN ISO 11855-2:2020
01-maj-2020
Načrtovanje okolja v stavbah - Vgrajeni hladilni in ogrevalni sistemi - 2. del:
Določanje načrtovane grelne in hladilne moči (ISO/DIS 11855-2:2020)
Building environment design - Embedded radiant heating and cooling systems - Part 2:
Determination of the design heating and cooling capacity (ISO/DIS 11855-2:2020)Umweltgerechte Gebäudeplanung - Flächenintegrierte Strahlheizungs- und -
kühlsysteme - Teil 2: Bestimmung der Auslegungs-Heiz- bzw. Kühlleistung (ISO/DIS
11855-2:2020)
Conception de l'environnement des bâtiments - Systèmes intégrés de chauffage et de
refroidissement par rayonnement - Partie 2: Détermination de la puissance calorifique et
frigorifique à la conception (ISO/DIS 11855-2:2020)Ta slovenski standard je istoveten z: prEN ISO 11855-2
ICS:
91.140.10 Sistemi centralnega Central heating systems
ogrevanja
91.140.30 Prezračevalni in klimatski Ventilation and air-
sistemi conditioning systems
oSIST prEN ISO 11855-2:2020 en,fr,de
2003-01.Slovenski inštitut za standardizacijo. Razmnoževanje celote ali delov tega standarda ni dovoljeno.
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oSIST prEN ISO 11855-2:2020
DRAFT INTERNATIONAL STANDARD
ISO/DIS 11855-2
ISO/TC 205 Secretariat: ANSI
Voting begins on: Voting terminates on:
2020-03-16 2020-06-08
Building environment design — Embedded radiant heating
and cooling systems —
Part 2:
Determination of the design heating and cooling capacity
Conception de l'environnement des bâtiments — Systèmes intégrés de chauffage et de refroidissement par
rayonnement —Partie 2: Détermination de la puissance calorifique et frigorifique à la conception
ICS: 91.040.01THIS DOCUMENT IS A DRAFT CIRCULATED
This document is circulated as received from the committee secretariat.
FOR COMMENT AND APPROVAL. IT IS
THEREFORE SUBJECT TO CHANGE AND MAY
NOT BE REFERRED TO AS AN INTERNATIONAL
STANDARD UNTIL PUBLISHED AS SUCH.
IN ADDITION TO THEIR EVALUATION AS
ISO/CEN PARALLEL PROCESSING
BEING ACCEPTABLE FOR INDUSTRIAL,
TECHNOLOGICAL, COMMERCIAL AND
USER PURPOSES, DRAFT INTERNATIONAL
STANDARDS MAY ON OCCASION HAVE TO
BE CONSIDERED IN THE LIGHT OF THEIR
POTENTIAL TO BECOME STANDARDS TO
WHICH REFERENCE MAY BE MADE IN
Reference number
NATIONAL REGULATIONS.
ISO/DIS 11855-2:2020(E)
RECIPIENTS OF THIS DRAFT ARE INVITED
TO SUBMIT, WITH THEIR COMMENTS,
NOTIFICATION OF ANY RELEVANT PATENT
RIGHTS OF WHICH THEY ARE AWARE AND TO
PROVIDE SUPPORTING DOCUMENTATION. ISO 2020
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oSIST prEN ISO 11855-2:2020
ISO/DIS 11855-2:2020(E)
COPYRIGHT PROTECTED DOCUMENT
© ISO 2020
All rights reserved. Unless otherwise specified, or required in the context of its implementation, no part of this publication may
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Published in Switzerland
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oSIST prEN ISO 11855-2:2020
ISO/DIS 11855-2:2020(E)
Contents Page
Foreword ........................................................................................................................................................................................................................................iv
Introduction ..................................................................................................................................................................................................................................v
1 Scope ................................................................................................................................................................................................................................. 1
2 Normative references ...................................................................................................................................................................................... 1
3 Terms and definitions ..................................................................................................................................................................................... 1
4 Symbols and abbreviations ....................................................................................................................................................................... 1
5 Concept of the method to determine the heating and cooling capacity ......................................................3
6 Heat exchange coefficient between surface and space ................................................................................................. 4
7 Simplified calculation methods for determining heating and cooling capacity or
surface temperature ......................................................................................................................................................................................... 5
7.1 Universal single power function .............................................................................................................................................. 6
7.2 Thermal resistance methods ...................................................................................................................................................... 9
8 Use of basic calculation programmes ..........................................................................................................................................11
8.1 Basic calculation programmes ...............................................................................................................................................11
8.2 Items to be included in a complete computation documentation ...........................................................12
9 Calculation of the heating and cooling capacity ...............................................................................................................12
Annex A (normative) Calculation of the heat flux ................................................................................................................................13
Annex B (normative) General resistance method ...............................................................................................................................34
Annex C (normative) Pipes embedded in wooden construction ..........................................................................................40
Annex D (normative) Method for verification of FEM and FDM calculation programmes ........................48
Annex E (normative) Values for heat conductivity of materials and air layers .....................................................52
Bibliography .............................................................................................................................................................................................................................54
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Foreword
ISO (the International Organization for Standardization) is a worldwide federation of national standards
bodies (ISO member bodies). The work of preparing International Standards is normally carried out
through ISO technical committees. Each member body interested in a subject for which a technical
committee has been established has the right to be represented on that committee. International
organizations, governmental and non-governmental, in liaison with ISO, also take part in the work.
ISO collaborates closely with the International Electrotechnical Commission (IEC) on all matters of
electrotechnical standardization.International Standards are drafted in accordance with the rules given in the ISO/IEC Directives, Part 2.
The main task of technical committees is to prepare International Standards. Draft International
Standards adopted by the technical committees are circulated to the member bodies for voting.
Publication as an International Standard requires approval by at least 75 % of the member bodies
casting a vote.Attention is drawn to the possibility that some of the elements of this document may be the subject of
patent rights. ISO shall not be held responsible for identifying any or all such patent rights.
ISO 11855-2 was prepared by Technical Committee ISO/TC 205, Building environment design.
ISO 11855 consists of the following parts, under the general title Building environment design —
Design, dimensioning, installation, control and input parameters for the energy calculation of embedded
radiant heating and cooling systems:— Part 1: Defintion, symbols, and comfort criteria
— Part 2: Determination of the design and heating and cooling capacity
— Part 3: Design and dimensioning
— Part 4: Dimensioning and calculation of the dynamic heating and cooling capacity of Thermo Active
Building Systems (TABS)— Part 5: Installation
— Part 6: Control
— Part 7: Input parameters for the energy calculation
Part 1 specifies the comfort criteria which should be considered in designing embedded radiant
heating andcooling systems, since the main objective of the radiant heating and cooling system is to satisfy thermal
comfort of the occupants. Part 2 provides steady-state calculation methods for determination of the
heating and cooling capacity. Part 3 specifies design and dimensioning methods of radiant heating
and cooling systems to ensure the heating and cooling capacity. Part 4 provides a dimensioning and
calculation method to design Thermo Active Building Systems (TABS) for energy-saving purposes,
since radiant heating and cooling systems can reduce energy consumption and heat source size by using
renewable energy. Part 5 addresses the installation process for the system to operate as intended. Part
6 shows a proper control method of the radiant heating and cooling systems to ensure the maximum
performance which was intended in the design stage when the system is actually being operated in a
building. Part 7 presents a calculation method for input parameters to ISO 52031.
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Introduction
The radiant heating and cooling system consists of heat emitting/absorbing, heat supply, distribution,
and control systems. The ISO 11855 series deals with the embedded surface heating and cooling system
that directly controls heat exchange within the space. It does not include the system equipment itself,
such as heat source, distribution system and controller.The ISO 11855 series addresses an embedded system that is integrated with the building structure.
Therefore, the panel system with open air gap, which is not integrated with the building structure, is
not covered by this series.The ISO 11855 series shall be applied to systems using not only water but also other fluids or electricity
as a heating or cooling medium.The object of the ISO 11855 series is to provide criteria to effectively design embedded systems. To do
this, it presents comfort criteria for the space served by embedded systems, heat output calculation,
dimensioning, dynamic analysis, installation, control method of embedded systems, and input
parameters for the energy calculations.© ISO 2020 – All rights reserved v
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oSIST prEN ISO 11855-2:2020
DRAFT INTERNATIONAL STANDARD ISO/DIS 11855-2:2020(E)
Building environment design — Embedded radiant heating
and cooling systems —
Part 2:
Determination of the design heating and cooling capacity
1 Scope
This part of ISO 11855 specifies procedures and conditions to enable the heat flow in water based
surface heating and cooling systems to be determined relative to the medium differential temperature
for systems. The determination of thermal performance of water based surface heating and cooling
systems and their conformity to this part of ISO 11855 is carried out by calculation in accordance with
design documents and a model. This should enable a uniform assessment and calculation of water based
surface heating and cooling systems.The surface temperature and the temperature uniformity of the heated/cooled surface, nominal heat
flux between water and space, the associated nominal medium differential temperature, and the field
of characteristic curves for the relationship between heat flux and the determining variables are given
as the result.This part of ISO 11855 includes a general method based on Finite Difference or Finite Element Methods
and simplified calculation methods depending on position of pipes and type of building structure.
The ISO 11855 series is applicable to water based embedded surface heating and cooling systems in
residential, commercial and industrial buildings. The methods apply to systems integrated into the
wall, floor or ceiling construction without any open air gaps. It does not apply to panel systems with
open air gaps which are not integrated into the building structure.The ISO 11855 series also applies, as appropriate, to the use of fluids other than water as a heating or
cooling medium. The ISO 11855 series is not applicable for testing of systems. The methods do not apply
to heated or chilled ceiling panels or beams.2 Normative references
The following referenced documents are indispensable for the application of this document. For dated
references, only the edition cited applies. For undated references, the latest edition of the referenced
document (including any amendments) applies.ISO 11855-1, Building environment design — Design, dimensioning, installation, control and input
parameters for the energy calculation of embedded radiant heating and cooling systems — Part 1:
Vocabulary, symbols, and comfort criteriaEN 1264, Water based surface embedded heating and cooling systems (2012)
3 Terms and definitions
For the purposes of this document, the terms and definitions given in ISO 11855-1 apply.
4 Symbols and abbreviationsFor the purposes of this document, the symbols and abbreviations in Table 1 apply.
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Table 1 — Symbols and abbreviations
Symbol Unit Quantity
α — Parameter factors for calculation of characteristic curves
A m Surface of the occupied area
A m Surface of the heating/cooling surface area
A m Surface of the peripheral area
b — Calculation factor depending on the pipe spacing
B, B , B W/(m ⋅K) Coefficients depending on the system
G 0
D m External diameter of the pipe, including sheathing where used
d m External diameter of the pipe
d m Internal diameter of the pipe
d m External diameter of sheathing
c kJ/(kg⋅K) Specific heat capacity of water
h W/(m ⋅K) Total heat transfer coefficient (convection + radiation) between surface and space
K W/(m ⋅K) Equivalent heat transmission coefficientK — Parameter for heat conducting devices
k — Parameter for heat conducting layer
L m Width of heat conducting devices
L m Width of fin (horizontal part of heat conducting device seen as a heating fin)
finL m Length of installed pipes
m — Exponents for determination of characteristic curves
m — Exponents for determination of characteristic curves
m — Exponents for determination of characteristic curves
m — Exponents for determination of characteristic curves
m kg/s Design heating/cooling medium flow rate
n, n — Exponents
q W/m Heat flux at the surface
q W/m Heat flux in the occupied area
q W/m Design heat flux
des
q W/m Limit heat flux
q W/m Nominal heat flux
q W/m Heat flux in the peripheral area
q W/m Outward heat flux
R m ⋅K/W Partial inwards heat transmission resistance of surface structure
R m ⋅K/W Partial outwards heat transmission resistance of surface structure
R m ⋅K/W Thermal resistance of surface covering
λ,B
R m ⋅K/W Thermal resistance of thermal insulation
λ,ins
s m In Type B systems, thickness of thermal insulation from the outward edge of the
insulation to the inward edge of the pipes (see Figure 2)s m In Type B systems, thickness of thermal insulation from the outward edge of the
insulation to the outward edge of the pipes (see Figure 2)s m Thickness of thermal insulation
ins
s m Pipe wall thickness
s m Thickness of the layer above the pipe
s m Thickness of heat conducting device
S m Thickness of the screed (excluding the pipes in type A systems)
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Table 1 (continued)
Symbol Unit Quantity
W m Pipe spacing
h W/(m ⋅K) Heat exchange coefficient
λ W/(m⋅K) Heat conductivity of the heat diffusion device material
θ °C Maximum surface temperature
s,max
θ °C Minimum surface temperature
s,min
θ °C Design indoor temperature
θ °C Temperature of the heating/cooling medium
θ °C average surface temperature
s,m
θ °C Return temperature of heating/cooling medium
θ °C Supply temperature of heating/cooling medium
θ °C Indoor temperature in an adjacent space
Δθ K Heating/cooling medium differential temperature
Δθ K Design heating/cooling medium differential temperature
H,des
Δθ K Limit of heating/cooling medium differential temperature
H,G
Δθ K Nominal heating/cooling medium differential temperature
Δθ K Heating/cooling medium differential supply temperature
Δθ K Design heating/cooling medium differential supply temperature
V,des
λ W/(m⋅K) Thermal conductivity
σ K Temperature drop θ −θ
V R
φ — Conversion factor for temperatures
ψ — Volume ratio of the attachment studs in the screed
5 Concept of the method to determine the heating and cooling capacity
A given type of surface (floor, wall, ceiling) delivers, at a given average surface temperature and indoor
temperature (operative temperature θ ), the same heat flux in any space independent of the type of
embedded system. It is therefore possible to establish a basic formula or characteristic curve for cooling
and a basic formula or characteristic curve for heating, for each of the type of surfaces (floor, wall,
ceiling), independent of the type of embedded system, which is applicable to all heating and cooling
surfaces (see Clause 6).Two methods are included in this part of ISO 11855:
— simplified calculation methods depending on the type of system (see Clause 7);
— Finite Element Method and Finite Difference Method (see Clause 8).
Different simplified calculation methods are included in Clause 7 for calculation of the surface
temperature (average, maximum and minimum temperature) depending on the system construction
(type of pipe, pipe diameter, pipe distance, mounting of pipe, heat conducting devices, distribution
layer) and construction of the floor/wall/ceiling (covering, insulation layer, trapped air layer, etc.). The
simplified calculation methods are specific for the given type of system, and the boundary conditions
listed in Clause 7 shall be met. In the calculation report, it shall be clearly stated which calculation
method has been applied.In case a simplified calculation method is not available for a given type of system, either a basic
calculation using two or three dimensional finite element or finite difference method can be applied
(see Clause 8 and Annex D).NOTE In addition, laboratory testing (for example EN 1264:2012) may be applied.
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Based on the calculated average surface temperature at given combinations of medium (water)
temperature and space temperature, it is possible to determine the steady state heating and cooling
capacity (see Clause 9).6 Heat exchange coefficient between surface and space
The relationship between the heat flux and mean differential surface temperature [see Figure 1 and
Equations (1) to (4)] depends on the type of surface (floor, wall, ceiling) and whether the temperature
of the surface is lower (cooling) or higher (heating) than the space temperature.
Figure 1 — Basic characteristic curve for floor heating and ceiling coolingFor floor heating and ceiling cooling in Figure 1, the heat flux q is given by:
1,1 2
q = 8,92 (θ −θ ) (W/m) (1)
S,m i
where
θ is the average surface temperature in°C;
S,m
θ is the nominal indoor operative temperature in °C.
For other types of surface heating and cooling systems, the heat flux q is given by:
Wall heating and wall cooling: q = 8 (|θ −θ |) (W/m ) (2)s,m i
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Ceiling heating: q = 6 (|θ −θ |) (W/m ) (3)
s,m i
Floor cooling: q = 7 (|θ −θ |) (W/m ) (4)
s,m i
The heat transfer coefficient is combined convection and radiation.
NOTE In many building system simulations using dynamic computer models, the heat transfer is often split
up in a convective part (between heated/cooled surface and space air) and a radiant part (between heated/
cooled surface and the surrounding surfaces or sources). The radiant heat transfer coefficient may in the normal
temperature range 15-30 °C be fixed to 5,5 W/m K. The convective heat transfer coefficient depends on type of
surface, heating or cooling, air velocity (forced convection) or temperature difference between surface and air
(natural convection).For using the simplified calculation method in Annex A the characteristic curves present the heat
flux as a function of the difference between the heating/cooling medium temperature and the indoor
temperature. For the user of Annex A, this means not to do any calculations by directly using values
of heat transfer coefficients. Consequently, Annex A does not include values for such an application or
special details or equations concerning heat transfer coefficients on heating or cooling surfaces.
Thus, the values α of Table A.12 of Annex A are not intended to calculate the heat flux directly. In
fact, they are provided exclusively for the conversion of characteristic curves in accordance with
Equation (A.32) in Clause A.3. For simplifications these calculations are based on the same heat transfer
coefficient for floor cooling and ceiling heating, 6,5 W/m K.For every surface heating and cooling system, there is a maximum allowable heat flux, the limit heat flux
q . This is determined for a selected design indoor room temperature of θ (for heating, often 20 °C and
G ifor cooling, often 26 °C) at the maximum or minimum surface temperature θ and a temperature
F,maxdrop σ = 0 K.
For the calculations, the centre of the heating or cooling surface area, regardless of the type of system,
is used as a reference point for θ .S,max
The average surface temperature, θ , which determines the heat flux (refer to the basic characteristic
S,mcurve) is linked with the maximum or minimum surface temperature: θ < θ and. θ > θ
S,m S,max S,m S,minalways applies.
The attainable value, θ , depends not only on the type of system, but also on the operating conditions
S,m(temperature drop σ = θ −θ , outward heat flow q and heat resistance of the covering R ).
V R u λ,BThe following assumptions form the basis for calculation of the heat flux:
— heat transfer between the heated or cooled surface and the space occurs in accordance with the
basic characteristic curve;— the temperature drop σ = 0. The dependence of the characteristic curve on the temperature drop is
determined by using the logarithmically determined mean differential heating medium temperature
Δθ [see Equation (1)];m kg
— turbulent flow in pipe: > 4000 ;
d hm⋅
— no lateral heat flow.
7 Simplified calculation methods for determining heating and cooling capacity
or surface temperature
Two types of simplified calculation methods can be applied according to this part of ISO 11855:
— one method is based on a single power function product of all relevant parameters developed from
the finite element method (FEM);© ISO 2020 – All rights reserved 5
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oSIST prEN ISO 11855-2:2020
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— another method is based on calculation of equivalent thermal resistance between the temperature
of the heating or cooling medium and the surface temperature (or room temperature).
A given system construction can only be calculated with one of the simplified methods. The correct
method to apply depends on the type of system, A to G (position of pipes, concrete or wooden
construction) and the boundary conditions listed in Table 2.Table 2 — Criteria for selection of simplified calculation method
Type of Reference to
Pipe position Figure Boundary conditions
system method
In screed A, C 2 a) W ≥ 0,050 m s ≥ 0,01 m 7.1
Thermally decoupled from the structural 0,008 m ≤ d ≤ 0,03 m A.2.2
base of the building by thermal insulation
s /λ ≥ 0,01
u e
In insulation, conductive devices B 2 b) 0,05 m ≤ W ≤ 0,45 m 7.1
Not wooden constructions except for 0,014 m ≤ d ≤ 0,022 m A.2.3
weight bearing and thermal diffusion layer
0,01 m ≤ s /λ ≤ 0,18
u e
Plane section system D 2 c) 7.1,
A.2.4
In concrete slab E 4 S /W ≥ 0,3 7.2,
B.1
Capillar tubes in concrete surface F 5 d /W ≤ 0,2 7.2, B.2
Wooden constructions, pipes in sub floor G 6 λ ≥ 10 λ 7.2, Annex C
wl surroundingmaterial
or under sub floor, conductive devices
S λ ≥ 0,01
7.1 Universal single power function
The heat flux between embedded pipes (temperature of heating or cooling medium) and the space is
calculated by the general equation:i 2
qB=⋅ ()a ⋅” θ (W/m) (5)
∏ i H
where
B is a system-dependent coefficient in W/(m ⋅K). This depends on the type of system;
i is the power product, which links the parameters of the structure (surface covering, pipe
()a∏ i
spacing, pipe diameter and pipe covering).
This calculation method is given in Annex A for the following four types of systems:
— Type A with pipes embedded in the screed or concrete (see Figure 2 and A.2.2);— Type B with pipes embedded outside the screed (see Figure 2 and A.2.3);
— Type C with pipes embedded in the screed (see Figure 2 and A.2.2);
— Type D plane section systems (see A.2.4).
Figure 2 shows the types as embedded in the floor, but the methods can also be applied for wall and
ceiling systems with a corresponding position of the pipes.This method shall only be used for system configurations meeting the boundary conditions listed for
the different types of systems in Annex A.6 © ISO 2020 – All rights reserved
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oSIST prEN ISO 11855-2:2020
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a) Type A and C
Key
1 floor covering
2 weight bearing and thermal diffusion layer (cement screed, anhydrite screed, asphalt screed)
3 thermal insulation4 structural bearing
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b) Type B
Key
1 floor covering
2 weight bearing and thermal diffusion layer (cement screed, anhydrite screed, asphalt screed, wood)
3 heat diffusion devices4 thermal insulation
5 structural bearing
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c) Type D
Key
1 floor covering R , B
2 weight bearing and thermal diffusion layer (cement screed, anhydrite screed, asphalt screed, timber)
3 thermal insulation4 structural bearing
Figure 2 — System types A, B and C covered by the method in Annex A
7.2 Thermal resistance methods
The heat flux between embedded pipes (temperature of heating or cooling medium) and the space or
surface is calculated using thermal resistances.The concept is shown in Figure 3.
An equivalent resistance, R , between the heating or cooling medium to a fictive core (or heat
conduction layer) at the position of the pipes is determined. This resistance includes the influence of
type of pipe, pipe distance and method of pipe installation (in concrete, wooden construction, etc.).
In this way a fictive core temperature is calculated. The heat transfer between this fictive layer and
the surfaces, R and R (or space and neighbour space) is calculated using linear resistances (adding of
i eresistance of the layers above and below the heat conductive layer).
The equivalent resistance of the heat conductive layer is calculated in different ways depending on the
type of system.This calculation method, using the general resistance concept, is given in Annex B for the following two
types of systems:— Type E with pipes embedded in massive concrete slabs (see Figure 4 and B.1);
— Type F with capillary pipes embedded in a layer at the inside surface (see Figure 5 and B.2).
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Figure 3 — Basic network of thermal resistance
Figure 4 — Pipes embedded in a massive concrete layer, Type E
10 © ISO
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