training module 1 basic module
TRANSCRIPT
2
1. Introduction (nZEB, definition).
2. Directives
3. Basic Physics
4. Insulation Materials and Current
Technology trends
5. Building Automation and HVAC
6. Practical Workshop
Material to be covered
4 Introduction
What is nZEB ?
“nZEB” is defined by the EU Directive 2010/31
“A building with near zero energy consumption”: a Building with very high
energy performance, which is defined according to the annex I.
Need to stress that
The near zero or very low required energy for the building to function
should be covered (or recommended to be covered) by renewable energy
which is produced by the building or near the building.
5 Introduction
Buildings consume around 41% of
primary energy demand in Europe.
Residential buildings consume
around 67% of primary energy
demand in buildings in Europe.
Buildings are responsible for 30% of
CO2 emissions in Europe.
There is a great uncertainty in future
energy supply and the
corresponding prices.
There is a great potential in energy
savings in buildings, both in the
residential and non-residential
sectors.
Why nZEB?
6 Introduction
1970s: Efforts in improving efficiency rates
Introduction of natural gas networks
1980s: Emphasis in the reduction of emissions
New combustion technologies, operating in lower temperatures and emitting
less.
1990s: Introduction of Passive House standard
Reduction of heating load demand
First thoughts on indoor air quality
Increased cooling load demand, even in northern European countries
2000s: Optimization methods
Introduction of smart buildings and systems
Integration of renewables
Introduction of holistic view of buildings as an integrated system of multiple
elements rather than individual systems.
History – evolution of building energy use and efficiency
7
The first discussions appeared in 2002-2003 with the introduction of
directives for building energy consumption
In the subsequent years (2004-2006) we had the first numbers and targets
to reduce the energy consumption by 40% by the year 2020.
Re-evaluation of the above in 2013 for 20% reduction by (2013.C353E/28)
Reduction by 40% by 2050 for gross energy consumption (406.2009.EC)
Introduction
History – recent milestones
8
What is nZEB ?
“nZEB” is defined by the EU Directive 2010/31 as
«The Government of each country is responsible to define the nZEB building
and the subsequent minimum energy requirements for its function”
In other words EACH Government is obliged to define this term in its own
territory
Introduction
10
RES
Directive 2009/28/EC on the promotion of the use of energy from renewable
sources (RES)
EPBD-recast
Directive 2010/31/EU on the energy performance of buildings (recast)
Directives and National Legislation
Directives
11
Driving factors:
Reduction of greenhouse gas emissions and compliance with the Kyoto Protocol to
the United Nations Framework Convention on Climate Change.
Increase security of energy supply.
Promotion of technological development and innovation.
Providing opportunities for employment and regional development.
Directives and National Legislation
RES Directive (1)
12
Overall Goal: to establish a common framework for the promotion of
renewable energy sources in the European Union, setting mandatory national
targets for achieving a 20% share of renewable energy in the gross final
energy consumption and a 10% share of energy from renewable sources in
transport by 2020
Directives and National Legislation
RES Directive (2)
13
A new national law N.112(I)/2013 was voted in September 2013
Mandatory target for the year 2020 of increasing the contribution of
renewable energy sources to:
13% of the gross final energy consumption.
10% in all forms of transport.
Current Status
9% (target: 5.93%) in final
energy consumption.
2.42% in all forms of transport.
Annual RES share and minimum trajectory defined on the Directive 2009/28/EC for Cyprus
Directives and National Legislation
RES Directive - Cyprus
14
RES Directive was integrated in the Greek legislation through the Greek
Law 3851/2010.
In order to achieve the target of 20% RES contribution to the total gross
energy consumption, the aforementioned law stipulates:
40% RES electricity share.
20% RES heating and cooling share.
10% RES transport rate.
Incentives were provided for achieving the goals set especially for the
photovoltaics.
Directives and National Legislation
RES Directive - Greece
15
The following table provides the installed Power per RES till end March
2014 and the targets that have been set till 2014 and 2020.
Technology
Installed Power
(MW) on March
2014
Target 2014
(MW)
Target 2020
(MW)
Wind power station 1,847 4,000 7,500
Biomass power station 47 200 350
Hydroelectric power plants 3,238 3,700 4,650
Small – scale (0-15 MW) 220 300 350
Large – scale (>15 MW) 3,018 3,400 4,300
Photovoltaic power plants 2,212 1,500 2,200
Installations from farmers by
profession 273 500 750
Other installations 1,939 1,000 1,450
Solar thermal power station 0.00 120 250
Directives and National Legislation
RES Directive - Greece
16
The development of renewable energy sources has been one of the priorities
of Italy’s energy policy for some time, together with the promotion of energy
efficiency.
The objectives of such a policy are:
energy supply security.
reduction in energy costs for businesses and individual citizens.
promotion of innovative technology.
environmental protection (reduction in polluting and greenhouse gas emissions).
sustainable development.
In the medium to long term, Italy aims to redress the balance of its energy mix,
which is currently too dependent on imported fossil fuels. This process will also
involve significant measures to relaunch the use of new-generation nuclear
power.
Directives and National Legislation
RES Directive - Italy
17
According to the baseline trend scenario of the PRIMES model, which the
European Commission has taken as a reference point, Italy’s gross final energy
consumption in 2020 could reach a value of 166.50 Mtoe, compared with the
value of 134.61 Mtoe recorded in 2005.
The 2009 update to the PRIMES model, which also takes into account the effect
of the financial crisis, estimates Italy’s 2020 gross final energy consumption at
145.6 Mtoe.
Italy’s primary objective is therefore to make an extraordinary commitment to
increasing energy efficiency and reducing energy consumption. This strategy
will also be a determining factor in reaching the targets for reductions in
greenhouse gas emissions and the proportion of total energy consumption to be
covered by renewable sources.
Directives and National Legislation
RES Directive - Italy
18
Italy has already been putting significant emphasis on the mobilization of
renewable energies for some time.
Numerous support mechanisms are therefore already available, ensuring
remuneration for investment in various renewable energy and energy efficiency
operations, and encouraging the growth of related industries.
Nevertheless, the targets and the scale of Directive 2009/28/EC do require a
renewed commitment, based on principles which will ensure balanced
development of the various sectors which contribute to reaching said targets,
and with consideration of the cost-benefit ratio.
Equally, there will be increased commitment in terms of infrastructure, research,
training and, in general, every element which could contribute to the balanced
growth in renewable energy use.
Directives and National Legislation
RES Directive - Italy
19
The Parliament has compiled implementation criteria for the directive.
By implementing all these measures effectively, and by combining the effects of
individual actions, we can reach our goal:
national measures alone are unlikely to be enough, and in order to achieve
efficiency these should be integrated into international cooperation schemes;
during this process action will be needed to overcome potential restrictions
and criticalities, modify or improve certain measures, adapt the support
schemes to the continually changing economic and energy-use situations,
and take advantage of new technological applications.
References: Ministry of Economic Development (MSE); National Network of Local Energy Agencies (RENAEL); National Agency for new technologies, sustainable energy and economic development (ENEA
Directives and National Legislation
RES Directive - Italy
22
In order to achieve its own national objectives, Italy intends to strengthen and
rationalize the existing support mechanisms, within a framework which
integrates:
- efficacy in concentrating efforts along routes which will make the maximum
contribution to achieving the objectives;
- efficiency in introducing flexibility in incentives, limiting their contribution to
what is strictly necessary to make up for market shortcomings;
- financial sustainability for the end consumer, the party which bears a large
part of the burden of incentive schemes;
- careful consideration of all measures to be promoted in the three sectors in
which action will be taken: heating, transport, electricity.
Directives and National Legislation
RES Directive - Italy
23 Directives and National Legislation
RES Directive - Portugal
The National Energy Strategy (NES 2020) attributes a pivotal role to renewable
energy in the energy strategy and the targets that have been delineated for this
sector, with a very significant impact on the Portuguese economy.
24
Key parameters of NEEAP/NEAPR together with EPBD requirements on plans
for increasing the number of nearly zero-energy buildings
Source: http://repositorio.lneg.pt/handle/10400.9/2283
Directives and National Legislation
RES Directive - Portugal
25
The main objectives of the national energy policy include:
To guarantee compliance with Portugal’s commitments in the context of
European energy policies and policies to combat climate change, ensuring
that 31% of the gross final energy consumption, 60% of the electricity
produced and 10% of the energy consumption in the road transport sector
will be derived from renewable sources in 2020;
To reduce Portugal’s energy dependence on external sources, based on the
consumption and importation of fossil fuels, to around 74% in 2020, by
means of increasing use of endogenous energy resources (estimated
reduction using a Brent reference of 112 USD/bbl);
Directives and National Legislation
RES Directive - Portugal
26
To reduce the balance of energy imports by 25% (around € 2 billion) with the
energy produced from endogenous sources, making it possible to reduce
imports by an estimated 17 million barrels of oil and 3 billion cubic meters of
gas;
To consolidate the industrial cluster associated with wind energy and to
create new clusters associated with new technologies in the renewable
energy sector, ensuring a Gross Added Value of 2.7 billion Euros and
creating 70,000 new jobs in addition to the existing 29,000 jobs associated
with the production of electricity from RES by 2020;
Directives and National Legislation
RES Directive - Portugal
27
To promote sustainable development, creating the necessary conditions to
meet the commitments that Portugal has made with regard to reducing
greenhouse gases, by means of a greater use of RES and energy
efficiency.
Directives and National Legislation
RES Directive - Portugal
28
Portuguese overall target for the share of energy from renewable energy
sources in gross final energy consumption in 2005 and 2020
A) Share of energy from renewable sources in gross final energy consumption in 2005 (%) 19.8
B) Target of energy from renewable sources in gross final energy consumption in 2020 (%) 31.0
C) Expected total adjusted energy consumption in 2020 ((ktoe) 16,623
D) Expected amount of energy from renewable sources corresponding to the 2020 target
(calculated as B x C) (ktoe) 5,153
Solar thermal for residential and non-residential buildings: increasing area from 1 million m2 to 2.2 million m2
Residential : 700,000 m2 in 2013 plus 800,000 m2 in 2016 and 1,2 millions in 2020.
Non-residential: 300,00 m2 in 2013 and plus 330,000 m2 in 2016 and 500,00 m2 in 2020.
Directives and National Legislation
RES Directive - Portugal
29
Projections for Renewable Electricity in 2020 (PNAEE and PNAER)
MW
installed
RES Electricity Generation
(GWh)
% in Electricity
Consumption
Large Hydro 8,540 13,613
Hydro (below or equal to 10 MW) 400 916
Geothermal 29 226
Photovoltaic 670 1,039
Solar Thermal Electricity 50 100
Tidal, Wave, Ocean 6 15
Wind Onshore 5,273 11,601
Wind Offshore 70
Biomass (solid, biowaste, bioliquid) 4,306
Biogas 59 413
Total 15,824 32,300 59.6
Source: EREC road Map; DR 70/2013
Directives and National Legislation
RES Directive - Portugal
30
Renewable Electricity Generation in 2014
RES Electricity Generation (GWh)
Large Hydro 15,314
Hydro (below or equal to 10 MW) 1,509
Wind 11,813
Thermal 2,697
Cogeneration 1,526
Solar 592
Source: REN
Directives and National Legislation
RES Directive - Portugal
31
Source: REN
Energy supply in Portugal
Directives and National Legislation
RES Directive - Portugal
32
Renewable Energy production share in Portugal
Source: DGEG and REN
0
10
20
30
40
50
60
70
80
90
100
%
Renewable Non-renewable
Directives and National Legislation
RES Directive - Portugal
33
RES target, production and potential in Portugal
Source: ECOFYS
Directives and National Legislation
RES Directive - Portugal
34
RES target, production
and potential in Portugal
Source: ECOFYS
Directives and National Legislation
RES Directive - Portugal
35
Available local renewable energy
resources for Portugal
Distribution of potential renewable energy in Portugal
Source: DGEG
Contribution of Renewable Energy:
Solar collectors
Photovoltaic systems
Wind energy systems
Biomass
Geothermal
Hydro
Heat pumps
Directives and National Legislation
RES Directive - Portugal
36
Production of electricity from renewable sources in Portugal (GWh)
Distribution of potential renewable energy in Portugal
Source: DGEG
Directives and National Legislation
RES Directive - Portugal
37
Directive on the Energy Performance of Buildings (EPBD) - (Directive
2002/91/EC) first published in 2002
Directive on the Energy Performance of Buildings (EPBD) - recast
(Directive 2010/31/EU) adopted in 2010
Directives and National Legislation
EPBD Directive (history)
38
1. To promote the improvement of the energy performance of buildings
within the EU, taking into account outdoor climatic and local conditions,
as well as indoor climate requirements and cost-effectiveness.
2. Lay down requirements regarding:
a. A common general framework for a methodology for calculating the
integrated energy performance of buildings and building units.
b. The application of minimum requirements to the energy performance of new
buildings.
Directives and National Legislation
EPBD – Scope (1)
39
c. The application of minimum requirements to the energy performance of:
i. Existing buildings that are subject to major renovation.
ii. Building elements that form part of the building envelope, and have a significant
impact on its energy performance, when they are retrofitted or replaced
iii. Technical building systems whenever they are installed, replaced or upgraded
d. National plans for increasing the number of nearly zero energy buildings.
e. Energy certification of buildings.
f. Regular inspection of heating and air-conditioning systems in buildings.
g. Independent control systems for energy performance certificates and
inspection reports.
Directives and National Legislation
EPBD – Scope (2)
40
National (or regional) methodologies for assessing the energy performance
of buildings and Energy Performance Certification of buildings across EU
member states.
Building Energy Audits.
Mandatory inspection of boiler based heating systems as well as cooling
systems installed in buildings.
Overall view of the Building and treating all building components as
integrated parts of a larger system rather than individual components.
Establishing a correlation of building commercial value with its energy
performance .
Directives and National Legislation
EPBD – Major Outputs (1)
41
Definition of near Zero Energy Buildings (nZEB) and mandatory
introduction of nZEB buildings by:
31 December 2020 for all new buildings.
31 December 2018 for new buildings occupied and owned by public authorities.
Directives and National Legislation
EPBD – Major Outputs (2)
42
Implementation of the EPBD in Cyprus is ensured through 3 basic laws:
1. N.142(I)/2006 – Regulating the Energy Performance of Buildings
Law of 2006.
2. N. 30(I)/2009 – Regulating the Energy Performance of Buildings
(amendment) Law of 2009.
3. N.210(I)/2012 – Regulating the Energy Performance of Buildings
(amendment) Law of 2012.
Directives and National Legislation
Transposition to national legislation – Cyprus (1)
43
On a second level of legislation control national regulations are
issued:
i. Regulations regarding the energy certification of buildings.
ii. Regulations regarding the energy performance of buildings
correlated with the “Roads & Buildings Law”
iii. Regulations regarding the inspection of HVAC systems
iv. Regulations regarding the inspection of boiler-based heating
systems
Directives and National Legislation
Transposition to national legislation – Cyprus (2)
44
Finally, parameters and details are regulated through ministerial
orders:
i. Ministerial orders regarding the energy certification of buildings.
ii. Ministerial orders regarding the energy performance of
buildings correlated with the “Roads & Buildings Law”.
iii. Ministerial orders regarding the inspection of HVAC systems.
iv. Ministerial orders regarding the inspection of boiler-based
heating systems .
Directives and National Legislation
Transposition to national legislation – Cyprus (3)
45
Law 142(Ι)/2006-On the energy performance of buildings basic
law and amending laws N30(I)/2009 & N210(I(/2012
KDP148/2013-On the energy performance of buildings (Inspection of boiler-based
heating systems of nominal power 20-100 kW) Ministerial Act of 2013.
KDP149/2013-On the energy performance of buildings (Inspection of boiler-based heating systems of nominal power >100
kW) Ministerial Act of 2013.
KDP 119/2011-On the energy performance of buildings (Inspection of
boiler-based heating systems) Regulations of
2011.
Inspection of boiler-based heating systems
Directives and National Legislation
Transposition to national legislation – Cyprus (4)
46
Boiler-based heating system category
Frequency of inspection
Systems with boiler of nominal capacity 20-100 kW and use of solid, liquid or gaseous fuel
Every five (5) years following 31/12/2014
Systems with boiler of nominal capacity >100 kW and use of solid or liquid fuel
Every two (2) years following 31/12/2013
Systems with gas boiler of nominal capacity >100 kW
Every four (4) years following 31/12/2013
Inspection of boiler-based heating systems
Directives and National Legislation
Transposition to national legislation – Cyprus (5)
47
The inspection is performed from a qualified “inspector of boiler-based
heating systems”.
The inspection is performed according to the “Inspection of boiler-based
heating systems national guidelines” (KDP 238/2011).
An inspection certificate is issued to be presented to the national authority
when asked
Inspection of boiler-based heating systems
Directives and National Legislation
Transposition to national legislation – Cyprus (6)
48
Law 142(Ι)/2006-On the energy performance of buildings basic law and
amending laws N30(I)/2009 & N210(I(/2012
KDP 413/2009-On the energy performance of buildings (Inspection of
HVAC systems) Ministerial Act of 2009.
KDP 163/2009-On the energy performance of buildings (Inspection of
HVAC systems) Regulations of 2009.
Inspection of HVAC systems
Directives and National Legislation
Transposition to national legislation – Cyprus (7)
49
HVAC system category Frequency of inspection
HVAC Systems of nominal capacity 12-250 kW
Every five (5) years following 31/12/2011 or five (5) years after their installation date
HVAC Systems of nominal capacity >250 kW
Every three (3) years following 31/12/2011 or three (3) years after their installation date
HVAC Systems of nominal capacity less than 12 kW but with the overall capacity installed in the building exceeding 50 kW
Every five (5) years following 31/12/2010 or five (5) years after their installation date
Inspection of HVAC systems
Directives and National Legislation
Transposition to national legislation – Cyprus (8)
50
The inspection is performed from a qualified “inspector of HVAC systems”.
The inspection is performed according to the “Inspection of HVAC systems
national guidelines” (KDP 163/2009).
An inspection certificate is issued to be presented to the national authority
when asked.
Inspection of HVAC systems
Directives and National Legislation
Transposition to national legislation – Cyprus (9)
51
Law 142(Ι)/2006-On the energy performance of buildings basic law and
amending laws N30(I)/2009 & N210(I(/2012
KDP 39/2014-On the energy performance of
buildings (Energy Performance Certification
of buildings) amending Regulations of 2014.
KDP 164/2009-On the energy performance of
buildings (Energy Performance Certification of buildings) Regulations
of 2009.
Energy Performance Certification of buildings
Directives and National Legislation
Transposition to national legislation – Cyprus (10)
52
Related Ministerial Acts:
KDP432/2013: On the Energy Performance of Buildings regulating
Ministerial Act of 2013 (Minimum building energy performance
requirements).
KDP33/2015: On the Energy Performance of Buildings regulating
Ministerial Act of 2015 (Methodology for the assessment of the energy
performance of buildings).
KDP343/2013: On the Energy Performance of Buildings regulating
Ministerial Act of 2013 (Methodology for assessing the optimal cost level of
the Minimum building energy performance requirements).
Energy Performance Certification of buildings
Directives and National Legislation
Transposition to national legislation – Cyprus (11)
53
KDP386/2013: On the Energy Performance of Buildings regulating
Ministerial Act of 2013 (Performance requirements of building systems, in
current buildings or building units, that are newly installed, replaced or
upgraded).
KDP366/2014: On the Energy Performance of Buildings regulating
Ministerial Act of 2014 (Minimum energy performance and technical
specifications requirements that must be met by a near Zero Energy
Building).
Energy Performance Certification of buildings
Directives and National Legislation
Transposition to national legislation – Cyprus (12)
54
The energy performance of buildings is assessed based on the
corresponding national methodology.
Energy Performance Certificates (EPC) are issued only by qualified
experts registered in the records of the Cyprus Energy Service.
A valid EPC of minimum “Energy Category B” is required prior any new
building obtaining a building permit from local authorities.
A valid EPC is required for any building (new or old, residential or not
residential) used for commercial purposes (sale, rent, commercial space,
etc.).
Energy Performance Certification of buildings
Directives and National Legislation
Transposition to national legislation – Cyprus (13)
55
Based on the ministerial order KDP 366-2014, the following minimum
requirements are set for defining an nZEB:
Maximum consumption of primary energy in residential buildings: 100
kWh/m2/year.
Maximum consumption of primary energy in non-residential buildings: 125
kWh/m2/year.
Maximum consumption of primary energy used for heating in residential
buildings: 15 kWh/m2/year.
At least 25% of total primary energy consumed in the building should
originate from RES
Parameter Definition of NZEB
Directives and National Legislation
Transposition to national legislation – Cyprus (14)
56
Maximum thermal transmittance coefficient (U-value) of walls and
structural elements (columns and beams) of the building envelope: U≤0.4
W/m2K.
Maximum thermal transmittance coefficient (U-value) of horizontal
structural elements (rooftops, floor in pilotis, etc.) of the building envelope:
U≤0.4 W/m2K.
Maximum thermal transmittance coefficient (U-value) of doors and
windows that are part of the building envelope: U≤2.25 W/m2K.
Maximum mean installed lighting power in buildings dedicated as office
spaces: 10 W/m2.
Parameter Definition of NZEB
Directives and National Legislation
Transposition to national legislation – Cyprus (15)
57
The EPBD Directive 2002/91/EC was integrated in the Greek legislation
through the Greek Law 3661/2008.
Based on the aforementioned law, the Regulation for Energy Efficiency of
Buildings (KENAK) was issued in 2010
The recast EPBD Directive 2010/31/EU was integrated in the Greek
legislation through the Greek Law 4122/2013.
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Greece (1)
58
According to the Greek Law 3661/2008 and KENAK, relative legislation
came into force through ministerial orders regarding:
Guidelines to be followed during the construction / inspection of new build
buildings and fully renovated buildings the guidelines were issued by the
Technical Chamber of Greece.
Building legislation Greek Law 4067/2012.
Energy Performance Certificates
Required for new build buildings, fully renovated buildings and in case of
selling / renting a property (building).
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Greece (2)
59
Energy Inspectors are responsible in issuing the EPCs, for which there are 3
categories and 2 levels for each category (A and B):
o The Energy Inspectors for Buildings.
o The Energy Inspectors for Heating Systems.
o The Energy Inspectors for Cooling Systems.
o A- level License.
o B- level License.
Energy inspectors are qualified experts registered in a corresponding national
Registry.
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Greece (3)
Categories
Levels
60
General definition of nZEB concept, as per the recast EPBD Directive
Greek Law 4122/2013, however:
No minimum technical requirements and primary energy consumption for
nZEBs have been defined yet
No National Plan has been issued yet
No promotion actions have been done yet
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Greece (4)
61
In Italy the overall responsibility for the implementation of the Energy
Performance of Buildings Directive (EPBD) rests with the Ministry for
Economic Development.
The first decree setting the basis for the national legislative EPBD framework
was enacted in 2005.
After that, a number of legal acts (legislative, ministerial and presidential
decrees) have been issued to progressively define and specify all aspects of
the national EPBD transposition.
EPBD Directive – National implementation
Directives and National Legislation
Transposition to national legislation – Italy (1)
62
According to the Constitution, energy- related topics are a shared task
between the State and the 21 Regions and Autonomous Provinces.
Consequently, regional authorities may implement autonomous transpositions
of the EPBD, as long as they do not contradict the general principles and
requirements provided by national and EU regulations.
The national regulation stays in force for those regions which have not
published their own legislation.
At present, 11 Regions and Autonomous Provinces (Liguria, Emilia
Romagna, Toscana, Val d’Aosta and Lombardia, Friuli Venezia- Giulia, Puglia,
Sicilia, Toscana and the Autonomous Provinces of Trento and of Bolzano) out
of 21 have enacted their local transposition of the EPBD. All the others
follow the national legislation.
EPBD Directive – National implementation
Directives and National Legislation
Transposition to national legislation – Italy (2)
63
Except for the inspection of air-conditioning systems, the Legislative Decree
192/2005 has drawn the general framework for the transposition of the EPBD
at national level, setting the minimum requirements for the Energy
Performance (EP), and the U-values for windows, walls, floors and roofs, in
case of new buildings and major renovations.
In 2009, the Presidential Decree n. 59 extended the calculation
methodologies and minimum requirements to the summer EP of cooling and
lighting systems; it also updated the minimum requirements for the EP of
buildings and of heating systems.
EPBD Directive – National implementation
Directives and National Legislation
Transposition to national legislation – Italy (3)
64
With the Legislative Decree 28/2011 transposing the Renewable Energy
Services (RES) Directive, the requirements regarding the share of renewable
energy for new buildings and major renovations were increased, establishing
a calendar with a progressively larger share of renewable quota for Domestic
Hot Water (DHW), heating and cooling energy demand:
A. 20% renewable quota for all building permits requested between the 31st
of May 2012 and the 31st of December 2013;
B. 35% renewable quota for all building permits requested between the 1st
of January 2014 and the 31st of December 2016;
C. 50% renewable quota for all building permits requested from the 1st of
January 2017 onwards.
EPBD Directive – National implementation
Directives and National Legislation
Transposition to national legislation – Italy (4)
65
Since January 2010, after a transition phase with intermediate requirements,
new residential and non-residential buildings must fully comply with the
minimum requirements for winter performance, set by the Legislative Decree
192/2005.
EP values vary according to building type (EP for residential buildings is
expressed in terms of kWh/m2 year of primary energy, while EP for non-
residential buildings is expressed in terms of kWh/m3 year of primary energy),
climatic zone, local degree days, and surface area to volume ratio of the
building.
EPBD Directive – format of national transposition and implementation
of existing regulations
Directives and National Legislation
Transposition to national legislation – Italy (5)
66
Table 1: Minimum EP requirements for heating in residential buildings
(kWh/m2)
Table 2: Minimum EP requirements for heating in non residential
buildings (kWh/m2)
EPBD Directive – format of national transposition and implementation
of existing regulations
Directives and National Legislation
Transposition to national legislation – Italy (6)
67
Table 3: Minimum EP requirements for cooling in
residential buildings (kWh/m2)
Table 4: Minimum EP requirements for cooling in non
residential buildings (kWh/m3)
Table 5: Minimum required U values for
building elements (W/m2K)
EPBD Directive – format of national transposition and implementation
of existing regulations
Directives and National Legislation
Transposition to national legislation – Italy (7)
68
In case of new buildings and major renovations, the designer is expected
to:
Introduce compulsorily window sun shades, and calculate their contribution
to the winter and summer performance;
Either check that the mass external walls, except North-East to North-
West, is larger than 230 kg/m2, or that their value for periodic thermal
transmittance (a dynamic parameter introduced with the Standard UNI EN
ISO 13786:2008) is lower than 0.12 W/m2K;
Check that the periodic thermal transmittance for North-East to North-
West external walls only, is lower than 0.20 W/m2K.
EPBD Directive – format of national transposition and implementation
of existing regulations
Directives and National Legislation
Transposition to national legislation – Italy (8)
69
Minimum requirements are differentiated according to the degree of the
planned renovation. The minimum EP requirements for new buildings apply
fully in case of:
• Demolition/reconstruction or renovation of all the building elements (for
buildings with heated floor area >1000 m2);
• Building enlargements over 20% of the original volume, only for the newly
built section.
EPBD Directive – format of national transposition and implementation
of existing regulations
Directives and National Legislation
Transposition to national legislation – Italy (9)
70
When designing their local EPBD implementation, regional governments and
Autonomous Provinces are allowed to set stricter minimum requirements.
Table 6 shows the state of EPBD implementation among Regions and
Autonomous Provinces.
Requirements for public buildings
Public authority buildings are expected to set an example, and to play a
leading role. Therefore:
EP and U-values are set 10% lower than those required for private
buildings;
Seasonal efficiency for heating systems should be higher than (75 + 4 log
Pn)%;
Only centralized heating systems are allowed.
EPBD Directive – Minimum requirements in specific Regions
Directives and National Legislation
Transposition to national legislation – Italy (10)
71
Table 6: State of EPBD implementation among Regions and Autonomous Provinces
EPBD Directive – Minimum requirements in specific Regions
Directives and National Legislation
Transposition to national legislation – Italy (11)
72
The leading role of public buildings in the progression to nearly zero-energy
performance has been emphasized in the National Energy Efficiency Action
Plan (NEEAP).
In order to promote and support energy efficiency measures in the public
sector, the NEEAP foresees that an observatory will be set up.
The aim of this observatory will be to build a reference framework on the
status of implementation of energy efficiency programs and their effectiveness
at local level, as well as to support the process of defining policies and
specifying the implementation measures in a system shared among
institutions and stakeholders, both public and private.
EPBD Directive – Minimum requirements in specific Regions
Directives and National Legislation
Transposition to national legislation – Italy (12)
73
The Second National Energy Efficiency Action Plan, issued in July 2011, carried
some preliminary milestones for setting a national strategy for nearly Zero-
Energy Buildings (nZEB). It is stated that:
New minimum requirements for building EP and for building elements will be
set: the requirements should be laid down with a view to achieving cost-
optimality.
Economy and Finance, and the Ministry for Economical Development shall
join in a task force to program and manage a national incentive scheme.
Social housing: introduction of an incentive/bonus for projects adopting
innovative solutions (cool roof, active building envelope systems, etc.),
integration of renewables, use of ecologic components and materials,
optimization of local economic resources.
EPBD Directive – Action plan for progression to nZEB
Directives and National Legislation
Transposition to national legislation – Italy (13)
74
Introduction of standardization in the use of Building Energy Management
Systems (BEMS) for public buildings.
Residential buildings: focus on the cluster of existing buildings built before
1976 (which sums up to more than 70% of all buildings). Provide incentives
through low interest rate revolving fund schemes for renovations leading to a
50% decrease in energy consumption.
Stakeholders involvement: the National Energy Agency (ENEA) will involve
stakeholders in working groups, with the goal of proposing new lines of
action.
An observatory will be set up in order to monitor the effectiveness of the
programs and schemes.
School buildings: simplified procedures to involve Energy Service
Companies (ESCOs).
EPBD Directive – Action plan for progression to nZEB
Directives and National Legislation
Transposition to national legislation – Italy (14)
75
According to the Constitution, energy-related topics (technical standards
and building regulations relating to energy) are a shared task between the State
and the 21 Regions and Autonomous Provinces.
Regional authorities may implement autonomous transpositions of the
EPBD, as long as they do not contradict the general principles and
requirements provided by national and EU regulations.
As a consequence, there are two levels of standards and regulations:
a national level that establishes the national minimum energy performance
requirements;
a regional or local level that could be more onerous.
EPBD Directive – Action plan for progression to nZEB
Directives and National Legislation
Transposition to national legislation – Italy (15)
76
A different consequence of the regional independence is that a number of
regions have not yet implemented a certification scheme. The majority of these
regions are in the South of Italy.
In fact, according to the CTI report 2011 on the state of implementation of the
EPBD in Italy, 1,375,000 EPCs had been delivered in 18 of the 21 Regions and
Autonomous Provinces, 710,000 (more than the half) of which in Lombardia,
creating a marked difference in the level of expertise within the market
operators, and also in the level of awareness and trust within the population.
EPBD Directive – National/regional transposition
Directives and National Legislation
Transposition to national legislation – Italy (16)
77
In the northern part of the Country almost all regions have implemented
specific schemes as to what concern the application of the EPBD.
At present, 11 Regions and Autonomous Provinces (Liguria, Emilia-
Romagna, Toscana, Val d’Aosta and Lombardia, Friuli Venezia-Giulia,
Puglia, Sicilia, Toscana and the Autonomous Provinces of Trento and of
Bolzano) out of 21 have enacted their local transposition of the EPBD.
At the end of 2012, 6 Regions (Liguria, Emilia Romagna, Toscana, Val
d’Aosta, Lombardia and the Autonomous Province of Bolzano) have
transposed the EPBD recast.
EPBD Directive – National/regional transposition
Directives and National Legislation
Transposition to national legislation – Italy (17)
78
In the south those that have done
so are still the vast minority (just
Sicilia and Puglia).
The national regulation stays in
force for those regions which have
not published their own legislation,
so all the others follow the national
legislation.
Figure 1 In gray: regional EPBD regulations
EPBD Directive – National/regional transposition
Directives and National Legislation
Transposition to national legislation – Italy (18)
79
The EPBD was transposed into national law through:
Decree-Law n.º 78/2006 of April 4th - National System Energy Certification
and Indoor Air Quality in buildings,
Decree-Law nº 79/2006, of April 4th - Regulation of Energy Systems and
Air-conditioning in buildings (for office buildings),
Decree-Law n.º 80/2006, April 4th - Regulation of Thermal Performance of
Buildings (for residential buildings).
This regulations promoted energy efficiency of buildings, and the acquisition of
relevant experience in this area → increasing of the efficiency of the energy
certification system, but also on the identification of relevant aspects of its
application.
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Portugal (1)
80
The creation and operation of the certification system, along with the effort
employed in its application, contributed to highlight issues related to increasing
energy efficiency and use of renewable energy in buildings.
The 2006 Portuguese Building energy certification system and energy efficiency
codes were revised to transpose the 2010 recast EPBD (the process started in
2010 and the technical committees completed their work in 2012).
The transposition into national law of the Directive 2010/31/EU created an
opportunity to improve the systematization and scope of the energy certification
system and respective regulations, as well as align national requirements
impositions.
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Portugal (2)
81
Decree-Law n.º 118/2013 ensures not only the transposition of the Directive
2010/31/EU, but also a review of national legislation, including in a single
document, the Buildings Energy Certification System (SCE), Rules of the
Energy Performance of Housing Buildings (REH) and the Regulation on Energy
Performance of Office and Commercial Buildings (RECS).
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Portugal (3)
82
Building Thermal Legislation - Decree-Law 118/2013
Requisites
Thermal performance of opaque envelope Uelement ≤ Umax
Thermal performance of plane thermal bridges (PTB):
Umáx [W/m2.ºC]
Climatic zone
I1 I2 I3
Envelope elements and elements separating
useful and non useful areas (elevator shafts,
common circulation areas) with btr 0.7 (thermal
conditions similar to outdoors)
Vertical elements 1.75 1.60 1.45
Horizontal
elements 1.25 1.00 0.90
Construction elements between buildings and
non useful areas (elevator shafts, common
circulation areas) with btr ≤ 0.7 (thermal
conditions similar to indoors)
Vertical elements 2.00 2.00 1.90
Horizontal
elements 1.65 1.30 1.20
UPTB ≤ 0.9 W/m2.ºC
or UPTB ≤ 2 Uwall & UPTB ≤ Umáx
Maximum U-values, Umax [W/(m2.°C)]
Winter and Sumer climatic zones
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Portugal (4)
83
Reference U-Values - Evolution of the Reference U-values, Uref, Mainland Portugal [W/(m2.°C)]
Note: These values might be updated until 2020 to take into account cost-optimal studies and nZEB requisites.
Envelope, Uref [W/(m2.ºC)] RCCTE REH 31 – Dez. - 2015
I1 I2 I3 I1 I2 I3 I1 I2 I3
Envelope elements and
elements separating useful
and non useful areas (elevator
shafts, common circulation
areas) with btr 0.7 (thermal
conditions similar to outdoors)
Opaque vertical
elements 0.70 0.60 0.50 0.50 0.40 0.35 0.40 0.35 0.30
Opaque horizontal
elements 0.50 0.45 0.40 0.40 0.35 0.30 0.35 0.30 0.25
Construction elements
between buildings and non
useful areas (elevator shafts,
common circulation areas)
with btr ≤ 0.7 (thermal
conditions similar to indoors)
Opaque vertical
elements 1.40 1.20 1.00 1.00 0.80 0.70 0.80 0.70 0.60
Opaque horizontal
elements 1.00 0.90 0.80 0.80 0.70 0.60 0.70 0.60 0.50
Windows (Uw) (doors and windows) 4.30 3.30 3.30 2.90 2.60 2.40 2.80 2.40 2.20
Elements in contact with the ground - 0.5 0.5
EPBD Directive - Building Thermal Legislation - Decree-Law 118/2013
Directives and National Legislation
Transposition to national legislation – Portugal (5)
84
In Portugal, the information needed for calculating the energy performance
certificate and the suggested energy savings measures, the general information
about the building and the expert is stored in a central register.
Examples of extracted added value from EPC data are:
average building stock label;
benchmarking for revision of building regulation;
dissemination of renewable DHW systems; and
most recommended energy-efficiency measures.
ADENE’s website provides detailed information on the SCE (training courses, a list
of qualified experts, and lists of valid EPCs) to licensing authorities, professionals of
the sector, property owners and developers, and also to the general public.
www.adene.pt
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Portugal (6)
85
The energy performance of buildings is assessed based
on the national methodology (Decree-Law 118/2013 and
related mandamus and ordinances).
Energy Performance Certificates (EPC) are issued only
by qualified experts.
A valid EPC of minimum “Energy Category B-” is required
prior any new building or subjected to major renovation
works obtaining a building permit from local authorities.
A valid EPC is required for any building (new or existing
when on the market for sale or rent, residential or not
residential, commercial space, etc.).
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Portugal (7)
86
Distribution of Energy Performance certificates
Source: http://www.buildup.eu/publications/38183
The application of EPBD to the new and renovated buildings is still limited
50,000 new buildings are build each year in Portugal
The impact of applying energy performance requirement for new buildings
is low compared to the whole building stock.
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Portugal (8)
87
Energy label and Energy Performance Certificates distribution for new and existing buildings
Source: http://www.buildup.eu/publications/38183
EPBD Directive
Directives and National Legislation
Transposition to national legislation – Portugal (9)
88
The national action plan for the progression to nearly zero-energy buildings is
now under development, and the key targets and milestones defined.
The adopted definition of the nZEB, establishes a relation with cost optimal
evaluations.
nZEBs are defined as buildings that cumulatively offer:
components compatible with the upper level of the cost optimal
evaluations;
EPBD Directive – Action plan for progression to nZEB
Directives and National Legislation
Transposition to national legislation – Portugal (10)
89
implementation of renewable energy (produced on site, whenever possible
and/or as nearby as possible) that covers a very significant fraction of the
reduced building energy needs. Numerical indicators are also being studied
and will be made available following the conclusion of the cost optimal
procedures.
The primary energy factors, that also play an important role, will be gradually
revised until 2020, to incorporate the effort made by Portugal to have clean and
renewable electricity.
EPBD Directive – Action plan for progression to nZEB
Directives and National Legislation
Transposition to national legislation – Portugal (11)
90
Status of development of the nZEB definition
September 2014
EPBD Directive – Action plan for progression to nZEB
Directives and National Legislation
Transposition to national legislation – Portugal (12)
92
1. The building envelope/shell
2. Thermal Losses
3. Mechanisms
4. Thermal Gains
Basic Physics & the building envelope
Material to be covered
93
Every element of the building that connects the building’s conditioned
spaces with the external environment or any other adjoined constructions
Basic Physics & the building envelope
Building Shell - Definition
94
Vertical structural building elements
Walls
Columns/beams
Horizontal structural building elements
Rooftops
Floors in touch with the ground or in “pilotis”
Doors/windows and glazing
Shading systems
Basic Physics & the building envelope
Building shell / envelope elements
95
A building is loosing thermal energy to
the external environment:
through the roof.
through the walls.
through the windows.
through draughts due to insufficient
air-tightness.
into the ground.
Basic Physics & the building envelope
Thermal losses through the building envelope
96
Conditioned Space, Ti
External Environment, To
To
Ti
Tsi
Tso
Air gap / thermal
boundary, hsi Air gap / thermal
boundary, hso
Structural element, λ
d
Q Q
Basic Physics & the building envelope
Thermal losses through the walls (1)
Structural element thickness
98
Conditioned Space, Ti
External Environment, To
To
Ti
Tsi
Tso
Air gap / thermal
boundary, hsi Air gap / thermal
boundary, hso
Structural element, λ
d
Q Q
Basic Physics & the building envelope
Thermal gains through the walls (1)
99 Basic Physics & the building envelope
Thermal gains through the walls (2)
0.00
5.00
10.00
15.00
20.00
25.00
1-27-2012 0:00 1-27-2012 12:00 1-28-2012 0:00 1-28-2012 12:00 1-29-2012 0:00
Te
mp
era
ture
oC
Time
Temperature distribution across a west-orientated wall section
Internal Room Temperature
Internal West Wall Surface Temperature
External West Wall Surface Temperature
Ambient Temperature
101
Thermal losses based on the typical convection-conduction-convection
mechanism (just like the wall presented earlier)
Thermal gains due to solar radiation in sunny days
Increased thermal losses due to radiation during clear-sky nights
Basic Physics & the building envelope
Thermal losses/gains through the roof (1)
102 Basic Physics & the building envelope
Thermal losses/gains through the roof (2)
0.00
5.00
10.00
15.00
20.00
12-29-2011 12:00 12-29-2011 18:00 12-30-2011 0:00 12-30-2011 6:00 12-30-2011 12:00 12-30-2011 18:00
Te
mp
era
ture
(oC
)
Time
Temperature Distribution on Roof Section
Internal Roof Temperature
External Air Temperature
Intrnal Roof Surface Temperature External Roof Surface Temperature
104
Requirements for windows and shading systems:
Limit thermal losses to the external environment
Typical losses (just like the walls).
Losses through draughts.
Control direct solar radiation entering the building
Direct solar radiation provides heat gains to the conditioned building spaces
during the winter.
Direct solar radiation exposure increases cooling demand during summer time.
Visual contact to the external environment
Direct visual contact to the external environment (despite the existence of any
shading systems) is beneficial to the occupants psychological health.
Basic Physics & the building envelope
Windows and shading systems (1)
105
Glare control
Depending on workspace, there might be restrictions to the desired light density
entering the building (e.g. office spaces with computers).
Internal space illumination
Artificial light increases internal gains as well as operating costs.
Natural light is beneficial to the occupants health.
Basic Physics & the building envelope
Windows and shading systems (2)
106
Basic Mechanisms
Heat is transferred
through the windows
by direct solar
radiation.
Through convection
and conduction.
Basic Physics & the building envelope
Windows and shading systems (3)
107
Low-e coating
Used in double or triple glazing
Coated in the external surface of the
internal glazing
Limits thermal losses from the
internal conditioned space to the
environment (acts as a heat barrier
– undesired effects for summertime).
Basic Physics & the building envelope
Windows and shading systems (4)
Basic Mechanisms
108
Solar protective coating
Used in double or triple glazing
Coated in the internal surface of the
external glazing
Limits internal gains from direct solar
radiation (useful in the summer for
avoiding over-heating, undesired
effect for winter)
Limits space illumination
Basic Mechanisms
Basic Physics & the building envelope
Windows and shading systems (5)
109
Fixed shading systems
Flexible shading systems
External shading systems
Internal shading systems
Window integrated shading systems
Categories of shading systems
Basic Physics & the building envelope
Windows and shading systems (6)
110
Category of shading system based on installation origin
Shading system type
Externally installed shading system
Blinds Venetian blinds Awnings Screens
Window-integrated shading system
Blinds
Internally installed shading system
Blinds Vertical blinds Pleated blinds
Basic Mechanisms
Basic Physics & the building envelope
Windows and shading systems (7)
111
Architectural Association with funding from BMU/UBA. Further Training C02-Reduction 1995 source: PACER; U. Fischer
External fixed shading
device External movable
shading devices
Examples of shading devices
Basic Physics & the building envelope
Windows and shading systems (8)
112
fixed horizontal and vertical
elements
blinds/ venetian blinds
light controlling systems
/ roller-blinds
awnings
solar control glass
Examples of shading devices
Basic Physics & the building envelope
Windows and shading systems (9)
113
+ effective shading devices
+ adjustable fins – controllability of
visual contact and light
incidence
+ shading even with opened
windows
- susceptible to wind – no shading
during high wind velocities
Window with external
adjustable blinds
External shading devices
Basic Physics & the building envelope
Functional properties of different Shading Devices (1)
114
External shading systems can
provide efficient protection
from direct solar radiation
External shading devices
Basic Physics & the building envelope
Functional properties of different Shading Devices (2)
115
+ requires no cleaning, requires
little space
+ adjustable fins – controllability of
visual contact and light
incidence
- no shading with opened
windows
- joint controlling complex and
costly
Double-glazed window with
integrated blinds
Window –integrated Shading Devices
Basic Physics & the building envelope
Functional properties of different Shading Devices (3)
116
Integrated shading systems
can efficiently control glare
and illumination but on the
same time provide adequate
thermal protection
Window –integrated Shading Devices
Basic Physics & the building envelope
Functional properties of different Shading Devices (4)
117
Internal adjustable blinds
+ glare control
+ subsequent installation possible
- allows solar radiation to enter
the room and thus adding to
thermal load
Fixed roof curtains
Internal Shading Devices
Basic Physics & the building envelope
Functional properties of different Shading Devices (5)
118
Example of solar radiation entering the room and
thus adding to thermal load
Internal Shading Devices
Basic Physics & the building envelope
Functional properties of different Shading Devices (6)
119
Walls ~ 35%
Roof ~ 25%
Ground ~15%
Glazing ~ 10%
Draughts ~ 15%
Basic Physics & the building envelope
Overall losses in a typical residential building
120
Overall building shell
construction affects:
Internal envelope surface
temperature
Internal temperature and
humidity
Direct solar radiation and
illumination
Basic Physics & the building envelope
Building Shell
121
U
[W/m²K]
q
[W/m²]
θe
[°C]
θsi
[°C]
1.4 35 -5 15.45
0.5 12.5 -5 18.37
0.25 6.25 -5 19.18
Degree of insulation greatly affects internal
environment and temperature distribution, thus
affecting the perceived internal temperature and
heat direction
Basic Physics & the building envelope
Thermal loss
124
1. Definition
2. Available materials & general
properties
3. Current trends
4. Future technologies
5. Thermal Insulation Construction
Techniques
Thermal Insulation Materials
Material to be covered
125
Any material that limits heat transfer (primarily by conduction) from an
environment (body, element, building internal space, etc.) of high temperature
to an environment of lower temperature can be considered of being an
insulating material. Main thermal property for insulating material classification
is the thermal conductivity (k or λ).
As a rule of thumb, any material with a thermal conductivity k≤0.1 W/mK can
be classified as an insulating material.
Thermal Insulation Materials
Definition
126
Inorganic materials
Foamy
o Foam glass
Fibrous
o Glass-wool
o Rock-wool
Organic materials
Foamy
o Expanded polystyrene
o Extruded polystyrene
o polyurethane foam
Foamy expanded
o cork
o Melamine foam
o Phenol foam
XPS
EPS
Cork
Glass wool
Glass foam
Thermal Insulation Materials
Insulating materials categories (1)
127
Organic materials (cont.)
Fibrous
o Sheep-wool
o Cotton-wool
o Coconut fibers
o Cellulose
Combined materials
Siliconated Calcium
Gypsum foam
Wood-wool
Cement composites
o With glass fibers
o Foam cement boards (e.g. with polyurethane foam)
o etc.
Gypsum
foam Cellulose
Cement foam
boards
Glass fiber reinforced
composite
Thermal Insulation Materials
Insulating materials categories (2)
128
State of the art materials
Vacuum Insulation Panels (VIP)
Gas Filled Panels (GFP)
Aerogels
Reflective materials and radiant barriers
Phase Changing Materials (PCM)
Future materials & technologies
Vacuum Insulation Materials (VIM)
Gas Insulation Materials (GIM)
Nano Insulation Materials (NIM)
Dynamic Insulation Materials (DIM)
Thermal Insulation Materials
Insulating materials categories (3)
129
Physical properties
Density
Mechanical strength
Thermal insulation ability – thermal conductivity
Resistance to moisture
Resistance to heat
Resistance to fire
Sound absorption
Aging
etc.
Environmental impact properties
Primary embodied energy
Gas emissions during production
Use of additives against biological impacts
Thermal Insulation Materials
Insulating materials properties (1)
130
Environmental impact properties (cont.)
Re-usability
Recyclability
Classification of their treatment as waste
Environmental impact based on LCA approach – environmental labelling.
etc.
Public health (during production, use and final stage of disposal) properties
Dust and fibers emissions
Biopersistence
Toxicity in case of fire
etc.
Thermal Insulation Materials
Insulating materials properties (2)
131
Covers the family of glass wool and rock wool
Produced in the form of mats, boards, as well
as filling material.
Light and soft mineral wool products are used
for cavity insulation and frame houses.
Harder mineral wool boards with high mass
densities are used in cases where thermal
insulation is intended in carrying loads (e.g.
floors, roofs, etc.).
Thermal Insulation Materials
Traditional thermal building insulating materials (1)
Mineral Wool
132
Typical thermal conductivity values are
between 30 and 40 mW/mK
(0.03 W/mK ≤ k ≤ 0.04 W/mK).
thermal conductivity increases with moisture
increasing content (from 37 to 55 mW/mK for
a moisture increase from 0% to 10%).
Thermal Insulation Materials
Traditional thermal building insulating materials (2)
Mineral Wool
133
Made from small spheres of polystyrene (from crude
oil) containing an expansion agent.
Casted as boards or continuously on production line.
Partly open pore structure.
Typical thermal conductivity values are between 30
and 40 mW/mK (0.03 W/mK ≤ k ≤ 0.04
W/mK).
thermal conductivity increases with moisture
increasing content (from 36 to 54 mW/mK for a
moisture increase from 0% to 10%).
Thermal Insulation Materials
Traditional thermal building insulating materials (3)
Expanded polystyrene (EPS)
134
produced from melted polystyrene (from crude
oil) by adding an expansion gas (e.g HFC,
CO2, C6H12).
Produced in continuous lengths which are cut
after cooling on a production line.
closed pore structure
showing relatively high resistance to humidity
(especially compared to EPS).
Thermal Insulation Materials
Traditional thermal building insulating materials (4)
Extruded polystyrene (XPS)
135
Installed on roofs and wall parts which are in
contact with the ground.
Typical thermal conductivity values are
between 30 and 40 mW/mK (0.03 W/mK ≤ k ≤
0.04 W/mK).
thermal conductivity increases with moisture
increasing content (from 34 to 44 mW/mK for
a moisture increase from 0% to 10%).
Thermal Insulation Materials
Traditional thermal building insulating materials (5)
Extruded polystyrene (XPS)
136
Manufactured from recycled paper or wood
fibre mass.
Production process gives the material a
consistence similar to wool.
Boric acid (H3BO3) and borax (sodium
borates) are added to improve product
properties.
Produced mainly as a filler material but boards
and mats are also produced.
Thermal Insulation Materials
Traditional thermal building insulating materials (6)
Cellulose – polysaccharide (C6H10O5)n
137
Typically installed by blowing in cavities and
frame houses.
Typical thermal conductivity values are
between 40 and 50 mW/mK (0.04 W/mK ≤ k ≤
0.05 W/mK).
thermal conductivity increases with moisture
increasing content (from 40 to 66 mW/mK for
a moisture increase from 0% to 6%).
Thermal Insulation Materials
Traditional thermal building insulating materials (7)
Cellulose – polysaccharide (C6H10O5)n
138
Made primarily by cork oak
Produced both as a filler material, as well as
boards.
Typical thermal conductivity values are
between 40 and 50 mW/mK (0.04 W/mK ≤ k ≤
0.05 W/mK).
Exhibits also good acoustic properties for
sound insulation.
Thermal Insulation Materials
Traditional thermal building insulating materials (8)
Cellulose – polysaccharide (C6H10O5)n
139
Formed by reaction between isocyanates and
polyols (alcohol containing multiple hydroxyl
groups).
During the expansion process the closed
pores are filled with an expansion gas (HFC,
CO2, C6H12).
Usually produced as boards, sandwich panels
or in the form of an expansion.
Thermal Insulation Materials
Traditional thermal building insulating materials (9)
Polyurethane (PUR)
140
Used in external thermal insulation or most commonly
in the form of an expansion foam on site to insulate
difficult to reach cavities, frame houses, etc.
Typical thermal conductivity values are between 20
and 30 mW/mK (0.02 W/mK ≤ k ≤ 0.03 W/mK).
thermal conductivity varies with temperature,
moisture and mass density.
e.g. increases with moisture increasing content (from
25 to 46 mW/mK for a moisture increase from 0% to
10%).
Thermal Insulation Materials
Traditional thermal building insulating materials (10)
Polyurethane (PUR)
141
safe in its intended use but raises serious
health concerns and hazards in case of fire
during burning phase, PUR releases
hydrogen cyanide (HCN) and isocyanates,
which are highly toxic and very poisonous,
and can prevent cellular respiration
Thermal Insulation Materials
Traditional thermal building insulating materials (11)
Polyurethane (PUR)
142
Material Thermal
conductivity
k (W/mK)
Resistance
to heat
Resistance
to fire
Moisture
permeability
aging Resistance to
parasites
Mineral wool 0.03-0.04 Excellent Excellent High Excellent Excellent
EPS 0.03-0.04 Good Poor High Excellent Vulnerable to
rats
XPS 0.03-0.04 Good Poor Medium Excellent Vulnerable to
rats
Cork 0.04-0.05 Good Poor High Excellent Vulnerable to
rats
Polyurethane 0.02-0.03 Medium Poor Small Excellent Excellent
Cellulose 0.04-0.05 Medium Poor High Good Vulnerable to
rats and insects
Thermal Insulation Materials
Traditional thermal building insulating materials (12)
Typical properties overview
143
+ Relatively cheap and easy to handle
+ Can be perforated, cut or adjusted on construction
site without any loss of thermal resistance or other
physical properties
- Susceptible to moisture and temperature fluctuations
(thermal properties worsen with moisture penetration
and temperature increase)
- Thermal properties deteriorating with aging
- Requirement for increased insulation material
thickness to achieve low U-values
Thermal Insulation Materials
Traditional thermal building insulating materials (12)
Pros and Cons
146
Building
Structural
Elements
EnEV 2007 EnEV 2009 Tightening
(%) Umax (W/m2K)
External Walls
(external
insulation)
0.35 0.24 31
External
Windows,
French Windows
1.7 1.30 24
Slabs, roofs and
inclined roofs
0.30 0.24 20
Cellar Slabs
(cold-sided
cladding)
0.40 0.30 25
Thermal Insulation Materials
Market Evolution (3)
Evolution of Energy Saving Ordinance (EnEV) in Germany
147
Equivalent insulation effect
10x less thickness
Direct comparison of a traditional insulating
material versus a Vacuum Insulation Panel (VIP)
Thermal Insulation Materials
Market Evolution (4)
148
Consisting of an open porous core of fumed
silica, enveloped in several metallized polymer
layers (single, double or triple layer structure).
Manufactured primarily as boards/panels.
Thermal Insulation Materials
State of the art building thermal insulating materials (1)
Vacuum Insulation Panels (VIPs)
149
Typical thermal conductivity values are between 3 and 4
mW/mK (0.003 W/mK ≤ k ≤ 0.004 W/mK).
Due to the VIP’s material core nature of an open porous
structure, they are susceptible to:
Cuts, punctures and other external induced wear (thermal
conductivity can rise up to five times – 20 mW/mK in such
cases).
Moisture and air penetration from the envelope layer to the
core material (thermal conductivity can double after 25 years
reaching values up to 8 mW/mK).
Thermal Insulation Materials
State of the art building thermal insulating materials (2)
Vacuum Insulation Panels (VIPs)
150
As a result, VIPs cannot be cut or adjusted on site and their thermal
properties worsen with age.
Thermal Insulation Materials
State of the art building thermal insulating materials (3)
Vacuum Insulation Panels (VIPs)
151
Similar structure to VIP.
Constructed by a barrier foil and an internal
baffle structure where a gas (e.g. Argon – Ar,
Krypton – Kr or Xenon - Xe) less thermally
conductive than air is applied.
Typical theoretical thermal conductivity values
are less than 10 mW/mK (k ≤ 0.01 W/mK),
even though prototype GFPs measured
exhibit thermal conductivities of up to 40
mW/mK.
Thermal Insulation Materials
State of the art building thermal insulating materials (4)
Gas-filled Panels (GFP)
152
Compared to VIP, they exhibit a higher
thermal conductivity but have an advantage
on the fact that due to the presence of the
filling gas do not have to maintain a vacuum,
thus making them less susceptible to moisture
and air penetration.
Additionally, low emissivity surfaces inside the
GFP reduce radiative heat transfer.
Similarly to VIP, they are vulnerable to cuts,
punctures and other external induced wear.
Thermal Insulation Materials
State of the art building thermal insulating materials (5)
Gas-filled Panels (GFP)
153
They are practically dried gels with very high
porosity.
Synthesized by traditional low-temperature sol-
gel chemistry.
Most commonly used material is silica.
Synthesis and gel preparation: silica solid
nanoparticles, dispersed in a liquid,
agglomerate together to form a continuous 3D-
network. Then, by drying out the gel, the solid
framework is isolated from its liquid medium.
Thermal Insulation Materials
State of the art building thermal insulating materials (6)
Aerogels
154
Theoretical thermal conductivity values can reach as low as 4 mW/mK
(k ~ 0.004 W/mK) at a pressure of 50 mbar.
Currently, commercially available
state-of-the-art aerogels have been
reported to achieve thermal
conductivities in the range of 13-14
mW/mK .
They exhibit high compression
strength but are very fragile due to
very low tensile strength.
Thermal Insulation Materials
State of the art building thermal insulating materials (7)
Aerogels
155
Aerogels exhibit a very high
resistance to fire and heat.
Matches on top of an aerogel cylindrical
disc are protected from the beneath lit
fire.
Thermal Insulation Materials
State of the art building thermal insulating materials (8)
Aerogels
156
They can be produced as either opaque, translucent or transparent
materials, thus exhibiting a great variety of potential building applications.
Thermal Insulation Materials
State of the art building thermal insulating materials (9)
Aerogels
157 Thermal Insulation Materials
State of the art building thermal insulating materials (10)
Aerogels
158
Reflective materials and radiant barriers are materials used to reduce
the transport of energy across air spaces in a building envelope.
They include surfaces with low emittance and high reflectance in the
thermal spectrum 2-50 μm (i.e. near infra red and mid infra red).
Reflective insulation systems are characterized by having enclosed air
spaces adjacent to low-emittance surfaces.
Radiant barrier systems are associated with large ventilated or
unventilated spaces.
Reflective insulation materials usually consist of one or more aluminum
foils or metallized aluminum films bound to substrates.
Thermal Insulation Materials
State of the art building thermal insulating materials (11)
Reflective Materials & Radiant Barriers
159
Radiant barrier materials are most commonly single sheet materials
consisting of aluminum foils or film bonded to reinforced plastic or paper
or in some cases wood sheathing.
Reflective insulation materials usually consist of one or more aluminum
foils or metallized aluminum films bound to substrates.
Aluminum products are relatively cheap and can exhibit emittance factors
as low as 0.03.
The performance of radiant barriers and reflective materials is based on a
reduction in heat transfer by radiation between hot and cold surfaces.
Thermal Insulation Materials
State of the art building thermal insulating materials (12)
Reflective Materials & Radiant Barriers
160
If surface one is hot and surface 2 is cold, then the net radiative transfer Q12 is
given by the following equation:
The net radiative transfer between parallel surfaces
depends on the temperatures of the surfaces, the
emittances of the surfaces and the orientation of the
surfaces.
For large parallel surfaces (such as the applications of reflective insulation
systems in building envelopes) with emittances ε1 and ε2 F12 is given by
equation:
Thermal Insulation Materials
State of the art building thermal insulating materials (13)
Reflective Materials & Radiant Barriers
161
Ιn building applications the temperature differences (T1-T2) are relatively small
with the result that the radiative heat flux Q12/A can be approximated as
follows:
The heat flux for the convection-convection term is represented by hc with the
resulting total heat flux being the sum of the two terms as shown below:
Thermal Insulation Materials
State of the art building thermal insulating materials (14)
Reflective Materials & Radiant Barriers
162
A combination of the former equation with the definition of R-value gives an
expression for the equivalent thermal resistance of the enclosed air space:
The term hc depends on the heat flow direction since it includes buoyance
driven free convection. Thus, it can be derived that reflective materials and
radiant barriers thermal insulation performance is orientation based.
Thermal Insulation Materials
State of the art building thermal insulating materials (15)
Reflective Materials & Radiant Barriers
163
It can also be observed that, since R-value is inversely proportional to E, the
lower the value of E the higher the value of the thermal insulation system’s
resistance R.
Thus, the lower the emittance factor of the reflective surface (the higher E
becomes), the higher the value of the thermal insulation system’s resistance R.
Thermal Insulation Materials
State of the art building thermal insulating materials (16)
Reflective Materials & Radiant Barriers
164
Reflective materials and radiant barriers are met in single or double brick walls
insulation systems, or used for thermal insulation of roofs or floors. Other
applications include roof solar reflectance coatings to reduce building thermal
gains in hot climates.
Thermal Insulation Materials
State of the art building thermal insulating materials (17)
Reflective Materials & Radiant Barriers
165
The main property of phase change materials is the storage of heat
energy in a latent form, leading to greater heat storage capacity per
unit volume than that of conventional building materials.
They are not really considered to be insulating materials (but they are
similarly applied in structure surfaces – walls, roofs, etc.).
They provide solutions especially in buildings with low thermal mass
due to extensive use of light-weight materials (thermal energy storage
in buildings seems to provide better thermal comfort for occupants).
PCMs change phase from solid state to liquid when heated, thus
absorbing energy in the endothermic process.
Thermal Insulation Materials
State of the art building thermal insulating materials (18)
Phase Changing Materials (PCM)
166
When the ambient temperature drops again, the liquid PCMs will turn
into solid state materials again while giving off the earlier absorbed heat
in the exothermic process.
Such a phase change cycle stabilizes the indoor building temperature,
cuts-off peak cooling loads and decreases the heating loads.
Desired properties (thermal, physical, kinetic & chemical) of PCMs:
From a thermal point of view, a suitable phase change temperature range
(melting temperature), a high latent heat of fusion (melting enthalpy) and a
good heat transfer towards the PCM are desired. The desired phase
change temperature will depend on climatic conditions and the desired
comfort temperature.
Thermal Insulation Materials
State of the art building thermal insulating materials (19)
Phase Changing Materials (PCM)
167
From a physical point of view, a favourable phase equilibrium, i.e. no phase
segregation, a high density and small volume changes at the phase
change are desired for easy incorporation in existing building materials or
structures.
From a kinetic point of view, no supercooling and a sufficient crystallization
rate are desired to make optimal use of the properties and possibilities of
PCMs. Supercooling, i.e. the process of lowering the temperature of a
liquid below its freezing point without becoming a solid, could strongly
affect the performance of the PCMs based on the chosen suitable phase
change temperature by influencing this temperature.
Thermal Insulation Materials
State of the art building thermal insulating materials (20)
Phase Changing Materials (PCM)
168
From a chemical point of view, a long-term chemical stability of the PCM
despite cycling, compatibility with construction materials, non-toxicity and
no fire hazard is desired.
Thermal Insulation Materials
State of the art building thermal insulating materials (21)
Phase Changing Materials (PCM)
169
PCM categories:
Organic compounds:
o Paraffins.
o Non-paraffins.
Inorganic compounds.
Inorganic eutectics or
eutectic mixtures.
Thermal Insulation Materials
State of the art building thermal insulating materials (22)
Phase Changing Materials (PCM)
170
+ Very low thermal conductivity values resulting in ultra low
requirement in insulating material thickness
+ Substantial space saving which can make them financially
profitable in areas of very high cost-sale value/m2.
- Thermal properties deteriorating with aging (even though
much less compared to traditional insulating materials)
- Very expensive at the moment
- Vulnerable to cuts, punctures and/or other external induced
wear, thus cannot be perforated or adjusted on construction
site without major loss of thermal properties
Thermal Insulation Materials
State of the art building thermal insulating materials (23)
Pros and Cons
171
Nanotechnology is expected to be applied as a scientific tool to make high
performance thermal insulation materials. Even though the normal focus in
nanotechnology is to control matter (typical particles, of dimensions between
0.1 nm and 100 nm, i.e. at an atomic and molecular scale), in the case of
thermal insulation materials, the focus is shifted from particles to controlling
pores in the nano range.
Thermal Insulation Materials
Future building thermal insulating materials (1)
Employing Nanotechnology
172
As an advancement to VIPs, VIM is basically a homogenous material
with a closed small pore structure filled with vacuum, with an overall
thermal conductivity of less than 4 mW/mK in pristine condition.
Due to its nanostructure nature, it is not susceptible to moisture and air
infiltration to the nanopores, thus it will present excellent ageing
characteristics.
Thermal Insulation Materials
Future building thermal insulating materials (2)
Vacuum Insulation Materials (VIM)
173
The VIM can be cut and adapted at the building site with no loss of low
thermal conductivity.
Perforating the VIM with a nail or similar would only result in a local
heat bridge, i.e. no loss of low thermal conductivity.
Thermal Insulation Materials
Future building thermal insulating materials (3)
Vacuum Insulation Materials (VIM)
174
As an advancement to GFPs, GIM is basically a homogenous material
with a closed small pore structure filled with a low conductance gas
(e.g. Argon – Ar, Krypton – Kr or Xenon - Xe), with an overall thermal
conductivity of less than 4 mW/mK in pristine condition.
Due to its nanostructure nature, it is not susceptible to moisture and air
infiltration to the nanopores, thus it will present excellent ageing
characteristics.
Similar to the VIM, with the only difference being that the vacuum is
replaced by a low-conductance gas.
Thermal Insulation Materials
Future building thermal insulating materials (4)
Gas Insulation Materials (GIM)
175
Originating from the idea of VIP and VIM, NIM is basically a
homogenous material with a closed or open small pore structure, with
an overall thermal conductivity of less than 4 mW/mK in pristine
condition.
unlike VIMs and GIMs, the grid structure in NIMs do not need to
prevent air and moisture penetration into their pore structure during
their service life (greater than 100 years). NIMs achieve their low
thermal conductivity without applying a vacuum in the pores by utilizing
the Knudsen effect. The gas thermal conductivity λgas taking into
account the Knudsen effect may be written in a simplified way as:
Thermal Insulation Materials
Future building thermal insulating materials (5)
Nano-Insulation Materials (NIM)
176
λgas=gas thermal conductivity in the pores (W/(mK))
λgas,0=gas thermal conductivity in the pores at STP
(standard temperature and pressure) (W/(mK))
β=coefficient characterizing the molecule–wall
collision energy transfer efficiency (between 1.5
and 2.0)
kB = Boltzmann's constant ≈ 1.38 × 10−23 J/K
T=temperature (K)
d=gas molecule collision diameter (m)
p=gas pressure in pores (Pa)
δ=characteristic pore diameter (m)
σmean=mean free path of gas molecules (m)
Thermal Insulation Materials
Future building thermal insulating materials (6)
Nano-Insulation Materials (NIM)
177
These result that the smaller the pores diameter, the lower is the value
λ of the NIM thermal conductivity.
Since NIMs are not affected by moisture or air infiltration to the nano-
pores, they are expected to present excellent ageing characteristics.
Thermal Insulation Materials
Future building thermal insulating materials (7)
Nano-Insulation Materials (NIM)
178
A dynamic insulation material (DIM) is a material where the thermal
conductivity can be controlled within a desirable range. One can control
thermal conductivity by being able to change in a controlled manner:
The inner pore gas content or concentration including the mean free path
of the gas molecules and the gas-surface interaction.
The emissivity of the inner surfaces of the pores.
The solid state thermal conductivity of the lattice.
Thermal Insulation Materials
Future building thermal insulating materials (8)
Dynamic Insulation Materials (DIM)
179
DIMs can provide solution to thermal insulation issues in southern
climates where a very low (as low as possible depending purely on
economical aspects) U-value is required to minimize thermal losses
during winter time but, on the other hand, a significantly higher U-value
is required as optimal insulation level to minimize cooling load demand
(it has been observed that ultra-low U-values can have reverse effects
on cooling demand and the corresponding seasonal energy
consumption – for Cyprus a U-value close to 0.3-0.4 W/mK is
considered to be at optimal insulation level regarding cooling demand).
Thermal Insulation Materials
Future building thermal insulating materials (8)
Dynamic Insulation Materials (DIM)
180
Advantages
Minimization of thermal bridging.
Taking full advantage of wall’s thermal mass.
Conditioned space remains heated/cooled substantial time after
switching off the heating/cooling system.
Protection of envelope structural elements from contraction and
expansion due to temperature differences.
Buffering sudden temperature changes and load peaks.
Disadvantages
Increased installation cost.
Susceptible to installation errors.
Difficulties in application in buildings with non uniform exterior
shape design.
Thermal Insulation Materials
Thermal insulation Construction Techniques (1)
External insulation in both walls and beams/columns
181
Advantages
Simple and fast construction.
lower costs.
Protection of insulation materials from external
environment (rain, solar radiation, heat, etc.).
Immediate response of heating/cooling system.
Disadvantages
Reduces conditioned space area.
Quick cooling/heating of conditioned space after switching
off the heating/cooling system.
Possible moisture problems.
Thermal Insulation Materials
Thermal insulation Construction Techniques (2)
Internal insulation in both walls, beams/columns and roof
182
Double brick wall with thermal insulation in
between two layers and external insulation in
beams/columns
Thermal bridge on the joint of wall and pier.
Part of wall’s thermal mass is not utilized.
Thermal insulation interruption
Thermal bridge on the balcony projection where
thermal insulation is interrupted.
Thermal Insulation Materials
Thermal insulation Construction Techniques (3)
Combination/Other
183
Alam, M., Singh, H. and Limbachiya, M.C., 2011. Vacuum Insulation Panels (VIPs) for
building construction industry – A review of the contemporary developments and future
directions. Applied Energy V.88(11), pp. 3592-3602.
Beatens, R., Jelle, B.P., Thue, J.V., Tenpierlk, M.J., Grynning, S., Uvslokk, S. and
Gustavsen, A., 2010. Vacuum insulation panels for building applications: A review and
beyond. Energy and Buildings V.42(2), pp.147-172.
Beatens, R., Jelle, B.P. and Gustavsen, A., 2010. Phase change materials for building
applications: A state-of-the-art review. Energy and Buildings V.42(9), pp.1361-1368.
Beatens, R., Jelle, B.P., Gustavsen, A. and Grynning, S., 2010. Gas-filled panels for
building applications: A state-of-the-art review. Energy and Buildings V.42(11), pp.1969-
1975.
Beatens, R., Jelle, B.P. and Gustavsen, A., 2011. Aerogel insulation for building
applications: A state-of-the-art review. Energy and Buildings V.43(4), pp.761-769.
Thermal Insulation Materials
Bibliography (1)
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Escudero, C., Martin, K., Erkoreka, A., Flores, I. and Sala J.M., 2013. Experimental
thermal characterization of radiant barriers for building insulation. Energy and Buildings
59, pp. 62-72.
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materials and solutions – Properties, requirements and possibilities. Energy and
Buildings V.43(10), pp.2549-2563.
Papadopoulos, A.M., 2005. State of the art in thermal insulation materials and aims for
future developments. Energy and Buildings V.37(1), pp.77-86.
Papadopoulos, A.M., Oxizidis, S. and Papathanasiou, L., 2008. Developing a new library
of materials and structural elements for the simulative evaluation of buildings’ energy
performance. Building and Environment V.43(5), pp.710-719.
Thermal Insulation Materials
Bibliography (2)
186
Some years ago, people had to rely only on their clothing for their thermal
comfort. Today however, people rely on the building environment and the
mechanical systems for this comfort.
HVAC
The Need (1)
187
HVAC
The Need (2)
Under normal condition the human internal body temperature is around
36.6oC, while changes ranging from 36.1oC to 37.3oC are considered
normal. The outside body temperature is around 33oC.
189
The body mechanisms that are employed to reject heat are :
1. By Radiation (40–50%). Thermal energy from the body surface
temperature is radiated to the surrounding.
2. By conduction (2-3%). This mechanism takes into account the loss/gain of
energy that is transferred to/by the human body by its direct contact with
other surrounding bodies.
3. By convection (25-30%). The air that is coming in contact with the body
may absorb/add heat. This process depends largely on the velocity of air,
the temperature of the air and the clothing.
4. The evaporation (25-30%). This is the only active mechanism that the
body employs in order to reject heat. On average a human body may
reject around 700W of thermal energy by this mechanism.
HVAC
The Need (4)
190
The parameters which affect the thermal comfort in a space/room and can
be adjusted by and HVAC system are:
The surrounding air temperature.
The radiation temperature of the surrounding surfaces.
The humidity of the space.
The air movement in the space (velocity).
The human metabolism and activity.
The clothing.
HVAC
The Need (5)
191
Human Metabolism
(Source: ASHRAE Handbook of Fundamentals 2009)
*1 met = 58,1 W/m2
Activity W/m2 met*
Resting
sleeping 40 0.7
laying 45 0.8
Sitting 60 1
Standing 70 1.2
Walking on leveled surface
0,9 m/s 115 2.0
1,34 m/s 150 2.6
1,79 m/s 220 3.8
Office activity
Reading) 55 1.0
Writing 60 1.0
Typing 65 1.1
Filing/Archiving (sitting person) 70 1.2
Filing/Archiving (standing person) 80 1.4
Walking 100 1.7
shelving 120 2.1
Driving
Car 60 - 115 1.0 – 2.0
Airplane 70 1.2
Airplane-landing 105 1.8
Airplane-military 140 2.4
Heavy Vehicle 185 3.2
Professional Activity
Coking 90 - 115 1.6 – 2.0
House cleaning 115 - 200 2.0 – 3.4
Sawing 105 1.8
Light industry 115 - 140 2.0 – 2.4
Heavy industry 235 4.0
Free time activity
Dancing 140 - 255 2.4 – 4.4
Gymnastics 175 – 235 3.0 – 4.0
Tennis 210 - 270 3.6 – 4.0
Basket ball 290 - 440 5.0 – 7.6
Wrestling 410 - 505 7.0 – 8.7
HVAC
The Need (6)
192
The surface of the human body (AD) can be estimated by the so called
DuBois equation as :
AD = the body surface, m2
w = the body mass, kg
h = the height of the human, m
HVAC
The Need (7)
193
Recommended design temperatures for winter
Category Temperature (oC) Rel Humidity(%)
Residences 22 30-50
Office Buildings 21-23 30-35
Libraries-museums 20-22 40-50
Hospitals 24 30
Restaurants and similar place 21-23 30-40
Recommended design temperatures for summer
Category Temperature (oC) Rel Humidity (%)
Residences 25-26 40-50
Office Buildings 25-26 40-50
Libraries-museums 22 40-55
Εστιατόρια, κέντρα διασκέδασης 23-26 50-60
Hospitals
- Rooms 24 45-50
- Operating theater 20-24 50-60
- Patient rooms 24 50-60
HVAC
The Need (8)
194
The heat rejection by the human body is achieved in part by skin
evaporation. At temperatures of 20 to 22C, this heat is rather small. At this
temperature level and relative humidity less than 30% (static electricity is
generated and the throat gets dry) while at the upper limit of 70% odors are
easily generated (very unpleasant) and mould is formed.
If the temperature is higher, the humidity levels are getting very important
as the evaporation from the skin is getting higher. It is very important to
avoid situations that prohibit the evaporation from the human skin. At the
level of 24 to 26°C the levels of the relative humidity can be within the
40% to 60%. According to ASHRAE, the relative humidity should never get
outside the region of 30% - 70%.
HVAC
The Need (9)
195
For thermal comfort, the value of the speed of air within the room is very
important. The range of this speed is between 0,1 and 1 m/s. If the speed is
less than 0.1m/s then this indicates a natural non-forced circulation.
HVAC
The Need (10)
197
Recommended values of air velocities for interior areas.
(ΤΟΤΕΕ 2423/86)
Velocity
(m/s) Effect Rec. Use
0-0.08 Complains about stagnant air none
0.125 Ideal Condition For all
applications
0.125-0.25
Very satisfactory, but the upper
limit approaches the maximum
recommended. (especially for
sitting persons)
For all
applications
0.325
Unsatisfactory for office space.
The air may remove light material
from the room and desks Commercial
spaces 0.375
Maximum Recommended for
moving people in the room.
0.373-1.5 Allowed only for industrial places * The above velocities refer to moving-working areas and up to the height of 2 m from
the floor.
HVAC
The Need (12)
198
“clo” values, depending on the clothing used
Clothing type (category) Clo
Naked 0
With shorts 0.1
Light clothing (for tropical areas) 0.3
Light summer clothing 0.5
Light summer -working clothing 0.6
Heavy winter clothing 1.2
Winter -working clothing 1.0
Clothing for the artic 3-4
Practically as heavy as possible 5
HVAC
The Need (13)
199
Thermal comfort in a room or a place depends on a number of parameters.
There have been efforts to combine those parameters into a single thermal
one either for commercial purposes or just to make our life easier.
So, in the past a number of those “combined parameters” have been
developed.
HVAC
The Need (14)
200
The globe temperature ranges between the dry bulb of the air and the
mean radiation temperature of the air in the room. This can be calculated
by the following equation:
tg = Globe temperature(oC)
tr = mean radiation temperature (oC)
ta = dry bulb temperature(oC)
V = velocity of air, m/s
HVAC
The Need (15)
The Globe temperature (spherical thermometer temperature) , tg
201
Effective temperature (ΕΤ), is the combination of the moisture, dry bulb
temperature and velocity of air in a room resulting in a single value. This
value is the older one developed and is based on the experimental work of
YAGLOU. This value does not take into account the radiation and a new
version called CET- Corrected Effective Temperature is usually used.
HVAC
The Need (16)
Effective Temperature, ET
202
This indicator was first used in 1935 by Missenard. Today is used in two
different variations, the first with the dry bulb and the second by wet bulb
temperatures. It takes into account the air temperature, the radiation, the
velocity of the surrounding air (the second takes into account the moisture as
well). The measurement of the dry resultant temperature is done by using a
special thermometer which consists of a black cooper sphere, 0.2mm thick and
of 10cm diameter. In the center, the bulb of a mercury thermometer is
measuring the particular temperature.
HVAC
The Need (17)
Resultant Temperature, tres
203
tg = temperature of spherical thermometer (oC)
tr = mean radiant temperature (oC)
ta = dry bulb temperature (resultant temperature)
v = velocity of air, m/s
When the air velocity is 0,1 m/s, then :
The resultant temperature (tres), can be used as a very good indicator of the
thermal comfort “for the whole body” in most heated spaces. The following
criteria can be used for people with normal clothing, in office work, and where
the thermal convection and radiation is around 65W ~ 83 W. Under the above
condition the criteria of the resultant temperature are:
19 oC ≤ tres ≤ 23 oC
Air velocity ≤ 0,1 m/s
Relative humidity 40% to 70%.
HVAC
The Need (17)
Resultant Temperature, tres
204
Thermal comfort is a very objective term and very difficult to measure. Various
studies however have shown that “thermally comfortable” environment is one
where 90% of the people in it feel comfortably. With tis assumption in mind a new
indicator was established, known as comfort temperature, tcomf. To calculate this
indicator, one takes into account the temperature of the surrounding air, the mean
radiant temperature, the humidity and the velocity of air.
ta = dry bulb temperature(oC)
tr = mean radiant temperature(oC)
v = velocity of air (m/s)
φ = relative humidity (%)
The above equation is valid provited:
tcomf : 21 – 24 oC
ta - tr : 3 Κ
v : 0 – 0.25 m/s
φ : 35 – 75%
HVAC
The Need (18)
Comfort Temperature, tcomf
205
As humans use different clothing to accommodate for the seasonal changes
and their personal activities, ASHRAE developed ASHRAE 55 which defines
the “zones of thermal comfort” for people dressed in typical summer or winter
clothing and sitting activity. This is shown in the following diagram.
HVAC
The Need (19)
Thermal Comfort Chart - ASHRAE
206
The operative temperature, top is the combination of the temperature of the
surrounding air, the mean radiant temperature and their respective convection
coefficients.
hc = clothing convection coefficient, W/m2K
hr = coefficient of the linear heat radiated by the clothing, W/m2K
tr = mean radiant temperature, oC
ta = dry bulb temperature of the surrounding air, oC.
HVAC
The Need (20)
207
The value of the coefficient hr ranges between 3.1 και 5.1 W/m2K depending
on the air velocity and the human activity, while the value of hc for room
conditions is 4.7 W/m2K. For a more precise calculation of the values
ASHARE suggests various values depending on the velocity of air and the
person's’ activity.
HVAC
The Need (21)
208
In a room with a large glass window the air temperature is 23oC, the mean
radiation temperature is 27oC, the velocity of the air 0.15 m/s and the relative
humidity 50%. Calculate the operational temperature of the room and check for
the thermal comfort conditions.
From the ASHRAE thermal comfort chart we observe that for operative
temperature of 24.8 oC and relative humidity 50% the room is within the zone of
thermal comfort. For the winter season however this zone is barely within the
comfort limits.
HVAC
The Need (22)
Example
210
Buildings and rooms receive sensible heat in the summer and loose sensible
heat in the winter. This obvious result is due to the air movement and
radiation. They can also gain or loose latent heat due to moisture. Energy can
also be due to human activity and devices within the building/room. Lighting
can only produce sensible heat in a room/space.
HVAC
The Need
211
Cooling load is defined as the quantity of heat that has to be removed from a
building in order to keep the various rooms/spaces under certain temperature
and humidity levels (other parameter may also be selected). The difference
between the term “gain” and load is the heat that is entering the building. The
load of the building is what usually need to be removed by an HVAC system
in order to keep the space/room under the pre-defined conditions. Cooling
load are measure in units of power, i.e. W.
HVAC
Cooling Load
212
Internal Thermal Gains
The main sources of internal thermal gains are the lighting, the people, and
possible devices that operate within the space to be conditioned.
Lighting
Usually lighting is the main source of internal thermal gains within a space.
Part of the energy used to provide lighting is in the form of radiation.
Florescence lights are considered to provide 59% of their rated power as
radiation and the rest as thermal load, while the usual tungsten type lighting
typically provides 80% radiation and 20% as thermal.
HVAC
Thermal Load
213
The instantaneous rate of thermal gain by electrical lighting can be estimated
as :
W = the total installed lighting power, W
Fu = coefficient of use
Fs = coefficient of special addition (if
fluorescent and halogen lights are
used)
HVAC
Thermal Load
214
The thermal gains due to the tenants has two basic elements. The so called
sensible and the latent. The total amount of heat gains is directly related with the
activity of the tenants. Special attention is required in designing a system and the
thermal gains as the places are getting populated. In places such as theaters,
museums, amphitheaters, is always reasonable to design for more people than
the full capacity of the space.
The sensible thermal gain is calculated by the following equation:
N = maximum number of people in a room
Fu = coefficient of use (unique for a specific space)
HVAC
Thermal Load
Tenants
215
If there is equipment driven by an electrical motor within the space to be air
conditioned then an equivalent thermal power is taken into account in the
calculation of the required cooling load.
HVAC
Thermal Load
Electrical Devices
216
Generally the solar gains depend on the characteristics of the building
surfaces and the direction of the sun’s radiation. To fully define this reality one
needs to take a look at the basic parameters that relate the sun’s radiation in
relation to the building’s position. The basic parameters are
The position of the building on the earth’s surface.
The date of year.
The time of date.
HVAC
Thermal Load
Solar gain thru transparent surfaces
217
General Geometry of the falling Sun radiation: αs = solar altitude angle, γs = solar azimuth angle, β = surface angle 0≤β≤0
0 180
HVAC
Thermal Load
γ = surface azimuth, θ = angle of incidence: the angle of the radiation to the perpendicular to the surface,, θz = the zenith
angle of the sun (=the angle between the rays and the perpendicular to the horizontal level (source: Duffie & Beckman).
218
Declination (δ) Approximate dates
+23o 27’ June 22
+20o May 21, July 24
+15o May 1, August 12
+10 o April 16, August 28
+5 o April 3, September 10
0 March 21, September 23
-5 o March 8, October 10
-10 o February 23, October 20
-15 o February 9, November 3
-20 o January 21, November 22
HVAC
Thermal Load
219
The optical characteristic of a surface are estimated by:
τ = transmittance, the percentage of the radiation passing through the surface
ρ = reflectance, the percentage of the radiation that is reflected
α = absorptance, the percentage of the radiation that is absorbed.
HVAC
Thermal Load
220
The value of each one of the above parameters changes significantly the solar
thermal gain. For transparent surfaces, such as the window in the drawing, the
solar energy that penetrates thru the surface , in Watts, can be calculated as:
It = solar radiation, W/m2
N = percentage of the absorbed radiation that was transferred with conduction and radiation to the
room interior.
HVAC
Thermal Load
221
Under equilibrium conditions N = U/ho, where ho is the convection coefficient of
the external side of the wall in W/m2 K. Thus the equation becomes:
HVAC
Thermal Load
222
This coefficient is used to accommodate for the values of SHGF for other kinds
of glass or take into account the shading due to a shading device.
HVAC
Thermal Load
Shading coefficient, SC
223
Type of glass
Glass
thickness
(mm)
Coefficient of Shading
No
external
shading
Viennese Rollers
Medium Light colored Dark colored Light colored
Single glass
- clear 3 1.00 0.64 0.55 0.59 0.25
- clear 6-12 0.95 0.64 0.55 0.59 0.25
- Heat absorbent
6 0.70 0.57 0.53 0.40 0.30
10 0.50 0.54 0.52 0.40 0.28
Double
- clear 3 0.90 0.57 0.51 0.60 0.25
- clear 6 0.83 0.57 0.51 0.60 0.25
-Reflective 6 0.2-0.4 0.2-0.33 - - -
HVAC
Thermal Load
225
Calculate the position of the sun (angles) in relation to a building in Limassol
at 14.00 on Oct 20th, based on the sun path diagram shown before.
HVAC
Thermal Load
Example
226
Limassol’s position is at a width of 35ο and we can use the previously
presented diagram. From the table we can estimate that the angle
(declination) on Oct 20 is -10ο. The exact location of the sun can then be
estimated on the common point which is:
- Solar angle αs = 38ο
- Azimuth γs = 218ο or 38ο SW.
HVAC
Thermal Load
Example
228
Heating is the process of adding heat to the surrounding air of a space for the purpose of increasing its temperature or keep its temperature at certain levels.
Cooling is the process of removing heat from the surrounding air of a space for the purpose of lowering its temperature or keep its temperature at certain levels.
Humidification is the process of the addition of moisture to the surrounding air of a space for the purpose of increasing the relative humidity or keeping it at certain level.
Dehumidification is the process of removing moisture from the surrounding air of a space for the purpose reducing its relative humidity or keeping it at certain level.
Renewal is the process of getting fresh air and damping quantities of internal air of a space for the purpose of increasing or keeping the quality of air at certain levels.
Cleaning is the process of removing solid particles and biological molecules from the air, for the purpose of increasing or keeping the quality of air at certain levels.
HVAC
Thermal Load
231
In these systems the air is conditioned in the central unit and then brought via ducts to the rooms/spaces to be conditioned. The necessary external air is brought into the system and mixed into a mixing chamber with the returning filtered air. Subsequently, the air returns to the rooms/spaces filtered, conditioned and with a percentage of fresh air.
Heating and Cooling Systems
HVAC – Systems (1)
Systems with air
232
These systems provide conditioned air and water at the supply points. These systems require thus, a dual system consisting of a separate air and a separate water systems, operating in parallel.
Heating and Cooling Systems
HVAC – Systems (2)
Systems of air and water
233
These systems control the air temperature thru devices in which cold/hot water is passed. These devices include fans which force the air to pass thru the cold/hot water exchanger and the room environment is kept at a required set temperature. There is no central air conditioning in those systems and the supply of fresh air is a separate system by itself.
Heating and Cooling Systems
HVAC – Systems (3)
Systems with water only
234
These systems are totally independent systems which use cooling media to cool/heat the surrounding air. They are of two types self contained and split units.
Larger systems with a central control unit and several distribution units are can also be found in the market today.
All the units can offer cooling and heating by reversing the their cycle operating thus as a refrigerator (cooling) and as a heat pump (reversed cycle).
Heating and Cooling Systems
HVAC – Systems (4)
Independent systems
235
ΗS = The sensible heat gain that needs to be removed from a space/room
ΗL = The latent heat gain that needs to be removed from a space/room
ΗΤ = The total heat load that that needs to be removed from a space/room
Heating and Cooling Systems
HVAC – Systems (5)
Room condition line
The room condition line is a straight line on a psychrometric chart which
connects the points that represent the initial air conditions and the conditions
under air treatment. The slope of this line is an indicator called factor of
sensible heat (SHF) and is defined as :
237 Heating and Cooling Systems
HVAC – Systems (7)
Air Conditioned
space
Mixing
chamber
Filter
Heating
Unit Heating
Unit
Adiabatic
spray
Fan
238
(1) Conditioned air, (2) Recycled air, (3) Fresh Air, (2)+(3) mixture of fresh and recycled (4), (4)(5) cooling
and dehumidification, (5)(6) sensible heating process, (6)(1) Air heating due to thermal gains (ducts,
fans etc.), (Α) apparatus dew point temperature, ADP.
Heating and Cooling Systems
HVAC – Typical Summer Condition (1)
239
Point (5), i.e. the condition of the exiting air id due to:
apparatus dew point , ADP (point Α) , and
The by-pass factor, B.F of the cooling unit which is calculated by:
Heating and Cooling Systems
HVAC – Typical Summer Condition (2)
240
Heating and Cooling Systems
HVAC – Typical Winter Condition (1)
Winter Time Air Conditioning Process
During the winter time, some of the thermal losses are recovered by the solar
radiation and the special internal thermal gains (persons present, lighting,
heat generating devices etc.). The main thermal gains are actually due to the
people in the room while the specific humidity of the outside air is usually low
(the relative humidity can be high).
241
(1) Entering air, (2) recycled air, (3) fresh air, (4) mixture of fresh and recycled air (5) preheated air, (6) exiting from spray chamber air, (7) heated air.
Air Conditioned
space
Mixing
chamber
Filter
Heating
Unit Heating
Unit
Adiabatic
spray
Fan
Heating and Cooling Systems
HVAC – Typical Winter Condition (2)
242
Heating and Cooling Systems
HVAC – Typical Winter Condition (3)
The respective processes of the typical winter air conditioning on a
psychrometric chart are shown below.
244 HVAC - Air Supply Systems
Systems of Constant Air Supply
The main systems of constant air supply are:
i. one circuit system of constant air supply.
ii. system of constant air supply with after-heating.
iii. two circuit system of constant air supply.
iv. multi circuit system of constant air supply.
245
Single Circuit constant air supply system
HVAC - Air Supply Systems
Air Conditioned
space
Mixing
chamber
Filter
Heating
Unit Heating
Unit
Adiabatic
spray
Fan
246
Central Air Conditioning Unit
Air Conditioned spaces
Fresh Air
Damped air
Filters
Cold Water in Hot Water in
Returning Air
HVAC - Air Supply Systems
Internal
space Internal
space
Constant air supply system with after-heater
247
Mixing
chamber Fresh
Air
Returning Air
Hot Air Duct
Cold Air Duct
Humidifier Fan
Fan
Cooling
Unit
Heating
Unit
Filter
Zone 1 Zone 3 Zone 3
HVAC - Air Supply Systems
Dual-duct system (1)
248
The dual duct systems are usually the choice for hotels, office buildings,
hospitals, schools and laboratories. The common characteristic of these
buildings is the large variation in the sensible heat load. With the
simultaneous supply of both hot and cold air in every supply unit this system
offers flexibility and instantaneous response to any demand.
HVAC - Air Supply Systems
Dual-duct system (2)
249
Cooling
Unit
Heating
Unit Fan
Pre-cooling /
Pre-heating
Unit
Filter
Mixing
chamber
Fan
Returning Air
Zone A
Zone B
Zone C
Fresh Air
HVAC - Air Supply Systems
Multi-circuit system of constant air supply
250
Cooling load Profile Cooling load Profile
Hours Hours
Load, % Load, %
HVAC - Air Supply Systems
Systems of variable air supply (1)
251
The main systems of variable air supply (VAV) are:
i. The single system of variable air supply.
ii. The dual system of variable air supply.
iii. The VAV system with units with embedded fan.
HVAC - Air Supply Systems
Systems of variable air supply (2)
252
Simple system of variable air supply - VAV
Cooling
Unit
Heating
Unit
Filter
Mixing
chamber Fresh Air
Fan
Fan
Returning Air
Room A
Room B
Room C
HVAC - Air Supply Systems
Systems of variable air supply (3)
253
Fresh Air
Damped Air
Central VAV Unit
Filter
Conditioned Spaces
Returning Air
Cold Water Hot Water
HVAC - Air Supply Systems
Systems of variable air supply (4)
Dual system of variable air supply - VAV
Internal
space
Internal
space
Internal
space
255 HVAC – Water Systems
Water only systems
The Water Only system are distinguished in:
Two pipe system
Three pipe system, and
Four pipe system.
256
Fresh air
Fan
Filter
Returning air Water from Boiler/Cooler
Water to Boiler/Cooler
3-way valve
Room Thermostat
Heat Exchanger
soundproofing
HVAC – Water Systems
Two-pipe fan-coil unit (FCU)
drain
Common
cooling/
heating
Unit
257
1 Thermostat
2 Cold water valve
3 Hot water valve
4 Heater/cooler
5 Hot water inlet
6 Cold water inlet
7 Common return
diagram
HVAC – Water Systems
Three-pipe water system (1)
258
1 Cold Water
2 Hot water
3 Thermostat
4 6-way valve
5 Cooler/Heater
6 2 or 3-way cold water valve
7 2 or 3-way hot water valve
8 Heater
9 Cooler
HVAC – Water Systems
Three-pipe water system (2)
260
In these systems the basic operation includes the supply of cold or hot water in suitable air moving devices, located in the room to be conditioned. So, circuits of both air and water need to be erected. There are cases where the supply of air is achieved by a separate independent ducting system.
If the water system is a 3 or 4-pipe one, then the system can supply simultaneously hot and cold water to the local units, making thus feasible the instantaneous and simultaneous heating and cooling of the rooms as required.
The centrally conditioned air is brought to the units and is called primary air while the recirculated air which is re-used is called secondary air.
The main air-water systems are:
the system with Fan-coil units and central distribution of primary air, and
the system with local production.
HVAC - Mixed Systems
HVAC – Air/Water Systems
Air-Water Systems
261
To other circuits
Fresh air
Returning air
Cooling unit
Heating unit
HVAC - Mixed Systems
HVAC – Air/Water Systems
Chiller
Primary water
circuit Pump
secondary water
circuit Pump
Zone re-heating
unit
FCUs
nozzles
263
This system employs an external unit (or an number of units) which can supply a number of delivery (room) units. Depending on the supplier these may be found as VRV (Variable Refrigerant Volume) or as VRF (Variable Refrigerant Flow). In both cases the system operates in a mode of variable refrigerant volume.
External
unit
Internal units
Refrigerant piping
HVAC - Mixed Systems
HVAC – VRV Systems
Variable Refrigerant Volume (VRV) Systems
264
Hea
t
Reje
ctio
n
Hea
t
Su
pp
ly
Cooling
HVAC - Mixed Systems
HVAC – VRV Systems
Cooling Cooling Cooling
Heating Heating Heating Heating
Cooling Cooling Heating Heating
265
The maximum power of an external unit is around 30 kW and can serve up to eight internal units of around 2,5-15 kW each. There are limitations to the maximum distance of the piping between the external unit and the internal ones and this is usually around 100m, with a maximum height difference of 50m.
HVAC - Mixed Systems
HVAC – VRV Systems
267
When air at a different temperature is damped in the environment, then there is room for heat recovery. When fresh air has to be supplied to a space/room then conditioned air is damped in exchange for that air. For the process of conditioning the fresh air by heating or cooling there is room for savings. These savings are usualy done by special systems called recovery systems.
HVAC – Energy Recovery Systems
Energy Recovery Systems
268
Fresh air
Damped air
Recycled
air
Supply
air
HVAC – Energy Recovery Systems
Energy Recovery Systems
Fixed plate exchangers
1. Air supply fan
2. Water droplet collector
3. Humidifier
4. Heating Unit
5. Cooling Unit
6. Drain basin
7. Filters
8. Fresh air damper
9. Filter bags
10. Air to air heat exchanger
11. Rejected air dampers
12. Recycled air damper
13. Recycled air fan
269 HVAC – Energy Recovery Systems
Energy Recovery Systems
Finned tube/coil exchangers
Fresh air
Damped air Recycled
air
Supply
air
1. Air supply fan
2. Water droplet collector
3. Humidifier
4. Heating Unit
5. Cooling Unit
6. Drain basin
7. Filters
8. Air to water heat exchanger
9. Recycled air fan
10. Recycled air damper
271
Ventilation is the process of supplying fresh air in a space/room in order to keep the necessary conditions for comfortable living in the room/space. This supply has first to satisfy the demands for breathing/survival in the space.
These requirements dictate the following:
Removal of CO2 Removal of the all body odors, Removal of all unnecessary heat, Removal of the excess humidity, Removal of all unwanted chemicals and smoke.
HVAC – Air Supply Systems
272
Under normal resting conditions man requires 0.10 to 0.12 l/s of air, while only
5% is led to the lungs as oxygen. The inhaled air mixture has 3-4% of CO2
which represents around 0.004 l/s. The upper limit of CO2 in an inhabited
space is 0.5% (by volume) for an 8-hour exposure.
HVAC – Air Supply Systems
273
Activity
Minimum Requirements for Fresh Air
(l/s per person)
0.10% CO2 0.25% CO2 0.50% CO2
Resting 5.7 1,8 0.85
Light work 8.6 – 18.5 2,7 – 5,9 1.3 – 2.8
Average work - 5,9 – 9,1 2.8 – 4.2
Hard Work - 9,1 – 11,8 4.2 – 5.5
Very Hard Work - 11,8 – 14,5 5.5 – 6.8
HVAC – Air Supply Systems
274
The odors form the human body are necessary to be removed from a
space/room. The minimum requirement for air removal to satisfy this
requirement is 5 l/s per person, but the usual number used is around 8
l/s per person. In large audiences (restaurants, theaters etc.) is safer to
assume 10-15 l/s per person.
HVAC – Air Supply Systems
275
This Criterion is usually used in simple designs of ventilation. The following
table indicates the recommended (empirical) air changes depending on the
space/room usage. The amount of air required can easily be found by
multiplying the number of the table by the volume of the space/room.
HVAC – Air Supply Systems
Hourly air changes
276
Type of Room air changes per hour
Conference rooms 6 – 8
Operation Theaters 15 – 20
Theaters 8 - 10
Rest rooms 4 - 8
Libraries 4 – 5
Offices 4 - 8
Malls 4 – 6
Restaurants 4 - 8
Shops 6 – 8
Cinemas 4 – 6
Κολυμβητήρια 3 – 4
Kitchens
- Large 8 - 12
- average 10 - 20
- small 15 - 30
Baths 5 – 8
Bedrooms 1 - 2
Schools 3 - 6
HVAC – Air Supply Systems
277
Type of Building
People per 100
m2 of room
floor area
Required ventilation
(m3/h)
minimum recommended
Single House
- Sitting room, bedrooms 5 8,5 12 - 17
- Kitchens, showers - 34 50 - 85
Multi Story buildings
- Sitting room, bedrooms 7 8,5 12 - 17
- kitchens, bathrooms - 34 50 - 85
Educational Buildings
- Lecture/teaching rooms 55 17 17 - 26
- Amphitheaters 110 17 26 - 34
- Libraries 22 12 17 - 21
- Laboratories 32 17 17 - 26
Hospitals
- Operating Rooms 55 34 42 - 51
- Surgery rooms - 34 -
- Patient rooms 22 17 26 - 34
Offices
- General 10 25 25 - 42
- Computer rooms 22 8,5 12 - 17
- Drafting rooms 22 12 17 - 25
Hospitals
- Bedrooms 5 12 17 - 25
- Showers - 34 51 - 85
- Corridors 22 17 25 - 34
Museums 75 12 17 - 25
Restaurants 75 17 25 -34
Cafeterias 110 51 60
Bars 150 51 68 - 85 * For more places see ΤΟΤΕΕ 2425/86
HVAC – Air Supply Systems
278
This method is applicable in special places where the rate of evaporation or
rate of injection into the environment of dangerous substance takes place.
Place such as paint shops, or places where there is exhausting of gases are
common place where this method is most appropriate.
The required quantity of air V results from the following equation:
Κ = The generated quantity of dangerous substance (m3/h)
Κa = Ratio of the dangerous substance to the air intake (m3 of dangerous substance per m3 of intake
air)
MAC = maximum allowable concentration of the dangerous substance in the space/room (m3 of
substance per m3 of air)
HVAC – Air Supply Systems
Calculation according to air pollution
279
Substance
Molecular
weight
(Μ)
Density
(kg/m3)
Death
(mg/l)
Dangerous
if inhaled for
½ to 1h
(mg/l)
Dangerous if
inhaled for
extended
periods
(mg/l)
Detectable
(mg/l)
Maximum allowable
in working
environments (MAC)
mg/l cm3/m3
Ammonia 17,03 0,7 3,5 -
7 1,5 – 2,7 0,1 0,035 2,4 1000
Benzene 100,2 4,2 - 30 - 40 5 - 10 1,25 2,0 500
Chlorine 70,91 2,9 2,5 -
3 0,1–0,15 0,01 0,01 0,0003 0,1
CO2 44,01 1,8 360 -
550 90 - 120 20 - 30 odorless 9,0 5000
CO 28,01 1,2 6 - 12 2 - 3 0,2 odorless 0,055 50 * For more substance look at ΤΟΤΕΕ 2425/86
HVAC – Air Supply Systems
280
These can be found in two main categories, depending on the circulation
mode employed. The first type is the so called “natural ventilations” systems
and the second is the so called “mechanical ventilation” system.
HVAC – Air Supply Systems
Ventilation Systems
281
In this kind of systems the air in the room/space is changing by natural
phenomena, and mainly due to the difference in pressure between the internal
and external environment. This change in pressure can be achieved either due
to the difference in temperature or due to the difference created by the local
wind conditions.
The volumetric flow of the air qv thru the various openings (junctions) can be
found from:
V = air volumetric flow, l/s
k = coefficient of intrusion, l/s m Pan
L = length opening, m
ΔP = pressure difference between openings, Pa
n = flow power
HVAC – Air Supply Systems
Natural Ventilation Systems
Ventilation Systems
282
Depending on the pressure in the building and the pressure of the wind outside
the building we may have air removing from the building interior to the
environment outside. The velocity of the wind is generally accepted that is
higher at higher levels, and as buildings are getting taller, the pressure around
the buildings are getting different as well. The velocity of air (v) in z meters
above the ground can be estimated by the following equation (Faber and Kell’s):
v = the average velocity at elevation z from the ground (m/s)
vm = the average velocity of air at 10 m from the ground (m/s)
z = elevation above the ground (m)
ks = coefficient
a = power depending on the building height
HVAC – Air Supply Systems
Natural Ventilation Systems
Ventilation Systems
283
Building position ks a
Level ground,
outdoors
0,68 0,17
Outdoors, non level
ground
0,52 0,20
Large city area 0,35 0,25
City area 0,21 0,33
HVAC – Air Supply Systems
Natural Ventilation Systems
Ventilation Systems
284
A = area of openings, m²
HVAC – Air Supply Systems
Natural Ventilation Systems
Ventilation Systems
C = coefficient of outflow(0,65 – 0,70)
g = 9,81 m/s²
h = differential height, m
Ti = mean internal temperature, K
To = external temperature, K
285
Calculate the natural ventilation achieved due to temperature difference in a
heated room with room temperature of 22 oC while the environmental
temperature is -2 oC if there are two openings in the room walls of 0,3 m2 each
in a vertical distance of 4 m from each other in opposite walls of the room.
HVAC – Air Supply Systems
Natural Ventilation Systems - Example
Ventilation Systems
286
In rooms with a large number of people (such as theaters, cinemas,
conference rooms, etc.) or places where unwanted odors are produced
natural ventilation is not the way to go. In such cases mechanical ventilation
is necessary.
There are three basic types of systems of mechanical ventilation, shown in
the subsequent diagrams. Το σύστημα φυσικής προσαγωγής φρέσκου αέρα
με μηχανική εξαγωγή αέρα
The system of natural intake and mechanical exhaust of the air
The system of mechanical intake and natural exhaust of the air, and
The system where both intake and exhaust are achieved with mechanical
means.
HVAC – Air Supply Systems
Mechanical Ventilation Systems
Ventilation Systems
287
(a) natural intake and
mechanical exhaust of the
air
(b) mechanical intake and
natural exhaust of the air
(c) both intake and exhaust
with mechanical means
Fan
Room
Fan
Room
Fan
Room
Fan
HVAC – Air Supply Systems
Mechanical Ventilation Systems
Ventilation Systems
288
Air distribution in the room
Room
Air supply
Duct
Air nozzle
HVAC – Air Supply Systems
Mechanical Ventilation Systems
Ventilation Systems
Ceiling Fins
289
The air flow is due to the difference in pressure between two points. This
difference in pressure led to force on the air molecules and subsequently a
motion of the molecules from the high pressure point to the low one. The
volume flow (Q) and the velocity of flow (v) are following the equation: Q = v A,
where Q the rate of flow (m3/s), v the velocity of air (m/s) and Α the area of the
section that the flow occurs (m2). This basic equation relates the flow of air
under all circumstances.
HVAC – Air Supply Systems
Mechanical Ventilation Systems
Ventilation Systems
290
The motion of air in a particular velocity will create a pressure known as velocity
pressure. These two values are related as:
pv = velocity pressure (N/m2)
v = velocity (m/s)
ρ = air density (1.2 kg/m3)
HVAC – Air Supply Systems
Mechanical Ventilation Systems
Ventilation Systems
291
Impeller: The rotary part of the fan, (the part that gives air the motion)
Axial Fan: A fan where the air is entering the impeller in a cylindrical
manner and exits parallel to the impeller axis.
Centrifugal fan: A fan where the air is leaving the impeller perpendicular
to the rotating axis.
Casing: The stationary parts of the fan, which guide the air.
Multi-stage fan: Fan with two or more Impellers in series.
HVAC – Air Supply Systems
Mechanical Ventilation Systems
Ventilation Systems
292
Measuring the Fan Total Pressure, pT,
And the Fan Static Pressure, ps.
HVAC – Air Supply Systems
Mechanical Ventilation Systems
Ventilation Systems
293
The operation of fans of the same type is governed by relations usually called
laws. These relations/laws relate the rotational speed, (N), the volumetric flow
rate (Q), the static pressure (p) and the power (P) for a fan.
To develop the relation we can easily use the dimensional analysis:
The size of a fan is governed by its diameter, D
The speed of a fan by its rotational speed, N
The medium property density, ρ
HVAC – Air Supply Systems
Fan Laws
Ventilation Systems
294
Following a small analysis one easily obtains the so called fan laws as follows:
HVAC – Air Supply Systems
Ventilation Systems
Fan Laws
295
Fans can be categorized in a number of ways and usually according to their
basic characteristics. One way they are usually categorized is according to
the flow direction thru the impeller. Basically, when it comes to room
ventilation, there are three types of fans:
Propeller fans
Axial flow fans
Centrifugal fans
HVAC – Air Supply Systems
Ventilation Systems
Types of fans and fan characteristics
296
rotor
motor
Volumetric air flow rate
Me
ch
an
ical p
ow
er
Sta
tic P
ressu
re
Eff
icie
ncy
HVAC – Air Supply Systems
Ventilation Systems
Typical fan characteristics
efficiency
Power fan static pressure
297
rotor Tip
Power
Efficiency
Static
Pressure
rotor blade
(airfoil section) motor
Volumetric air flow rate
Me
ch
an
ical p
ow
er
Sta
tic P
ressu
re
Eff
icie
ncy
HVAC – Air Supply Systems
Ventilation Systems
Axial fan
298
Impeller
Blades
Air outlet
Casing
Volumetric flow rate
Static Pressure
Power efficiency
HVAC – Air Supply Systems
Ventilation Systems
Centrifugal fan
rotation
Pre
ssu
re, e
ffic
ien
cy,
po
we
r
299
radial blades backward curved
HVAC – Air Supply Systems
Ventilation Systems
Volumetric flow rate
Static Pressure
Power
efficiency
Pre
ssu
re, e
ffic
ien
cy,
po
we
r Volumetric flow rate
Static Pressure Power
efficiency
Pre
ssu
re, e
ffic
ien
cy,
po
we
r
300
Two fans in series
Single fan
HVAC – Air Supply Systems
Ventilation Systems
Two fans in series
Volumetric flow rate (Q) P
ressu
re (
P)
301 HVAC – Air Supply Systems
Ventilation Systems
Two fans in parallel
Two fans in parallel
Single fan
Volumetric flow rate (Q)
Pre
ssu
re (
P)
303
energy = work (sum of all energies equals sum of all work).
energy cannot be destroyed or produced, but only transformed
(conservation of energy).
the energy of an isolated system is constant.
HVAC – Basic Thermodynamics and Energy
Basics
First Law of thermodynamics
304 HVAC – Basic Thermodynamics and Energy
Basics
Second Law of thermodynamics
all natural processes are irreversible.
by itself, heat can only transfer from a higher to a lower temperature
reservoir.
any kind of work or energy, can be transformed completely into heat.
however, heat cannot be completely converted into work energy.
305
DEmechanical
-IN
DEmechanical
-OUT
DEthermal-IN
DEthermal-
OUT
system boundary
DEsteady
HVAC – Basic Thermodynamics and Energy
Basics
306
t [°C]
(1)
][kWQ
(1) heating of ice
(2) melting of ice
(3) heating of liquid water
(4) evaporating of water
(5) heating (overheating) of water vapour
(2) (3) (4) (5)
HVAC – Basic Thermodynamics and Energy
Basics
307
medium r [kJ/kg] remark
ice/water 333.5 melting heat at 0°C
water 2452.8 evaporation heat at 20°C
water 2255.3 evaporation heat at 100°C
water 1940.0 evaporation heat at 200°C
NH3 (ammonia) 1260.66 evaporation heat at 0°C
R134a 197.2 evaporation heat at 0°C
R407C 223.29 evaporation heat at 0°C
methanol 1167 evaporation heat at 20°C
HVAC – Basic Thermodynamics and Energy
Basics
308
medium cp [kJ/kgK] remark
water 4.183 at 0°C, 1bar
ice 2.060 at -5°C
water vapour 1.875 at 0,01bar, 20°C
water vapour 2.020 at 1bar, 120°C
air 1.007 at 20°C, 1bar
monoethylene glycol/water
(30%/70%) 3.696 at -10°C
oil 2.540 mobiltherm 603 bei 200°C
steel 0.460
concrete 0.880
HVAC – Basic Thermodynamics and Energy
Basics
310
4
Q0 = condensing capacity
Pel
1
2
QC = vaporising capacity
3
HVAC – Basic Cooling
Ideal Cooling Cycle
311
s
T
critical point
liquid
liquid / gaseous
gaseous
p = const.
p = const.
GYKT00_54
t = const.
t = const.
t = const.
HVAC – Basic Cooling
312
s
T
critical point
liquid
liquid / gaseous
gaseous
p = const.
p = const.
GYKT00_54
t = const.
t = const.
t = const.
HVAC – Basic Cooling
313
h
log p
critical point
liquid
liquid / gaseous
gaseous
GYKT00_55
p = const.
p = const.
p= const.
HVAC – Basic Cooling
314
h
log p
critical point
liquid
liquid / gaseous
gaseous
GYKT00_55
p = const.
p = const.
p = const.
HVAC – Basic Cooling
316
h (kJ/kg)
0,8
h (kJ/kg)
P
(MPa)
h3=h4
0,14
R134a
0,32
1
23
4
67
58
h7=h8h1 h5
h6h2
A
B
h (kJ/kg)
0,8
h (kJ/kg)
P
(MPa)
h3=h4
0,14
R134a
0,32
1
23
4 1
23
4
67
58
67
58
67
58
h7=h8h1 h5
h6h2
A
B
HVAC – Basic Cooling
Cascaded Systems
317
performance factor: COP, EER
«efficiency» of refrigeration cycles and heat pump cycles.
EER (Energy Efficency Ratio) refers to cooling output.
COP (Coefficent of Performance) refers ot heating output.
HVAC – Basic Cooling
Definitions
318
parameter: SEER
SEER (Seasonal Energy Efficency Ratio); ratio of cooling output to energy
input.
efficiency factor (g)
ratio of the actually achieved COP to the maximum possible
efficiency of an ideal process.
e.g. the COP of a refrigerating machine using the Carnot-cycle.
HVAC – Basic Cooling
Definitions
319
h
log p
GEJO01_013
condensating deheating
Q 1
= m 1 . D h
evaporator
(with sub cooling)
Q C
= m . D h condensor
losses in
suction line
losses in
iquid line
losses in
compressor
losses in
compressor
1
2
3 4 5
6 7
8
effective evaporising temperature
9 10
losses in
pressure gas
line
effective
sub-cooling
prior
expansion valve
11
pressure losses
in distributor
HVAC – Basic Cooling
Real Cycle
320
At to= 0°C and at tc= 40°C, a refrigeration system using R 134a, is to provide
a cooling output of Qo= 50kW:
determine the required mass flow rate of the refrigerant.
what is the theoretical power input?
what is the theoretical condenser output?
HVAC – Basic Cooling
Example
321
Enthalpy [kJ/kg]
140 160 180 200 220 240 260 280 300 320 340 360 380 400 420 440 460 480 500 520 540 560
Pre
ssu
re [
Ba
r]
0,50
0,60
0,700,800,901,001,00
2,00
3,00
4,00
5,00
6,00
7,008,009,00
10,00
20,00
30,00
40,00
50,00
s =
1,7
0
s = 1
,75
s = 1
,80
s = 1
,85
s = 1
,90
s = 1
,95
s = 2
,00
s = 2
,05
s = 2
,10
s = 2
,15
s = 2
,20
s = 2
,25
-40
-40
-30
-20
-20
-10
0
0
10
20
20
30
40
40
50
60
60
70
80
80
90
100
100
120 140 160
0,00
15
0,0020
0,00300,0040
0,00500,0060
0,0070
0,0080
0,0090
0,010
0,015
0,020
0,030
0,040
0,050
0,060
0,070
0,080
0,090
0,10
0,15
0,20
0,30
0,40
0,50
0,60-40
-30
-20
-10
0
10
20
30
40
50
60
70
80
90
10
0
x = 0,10 0,20 0,30 0,40 0,50 0,60 0,70 0,80 0,90
s = 1,00 1,20 1,40 1,60
v= 0,0020
v= 0,0030
v= 0,0040
v= 0,0060
v= 0,0080
v= 0,010
v= 0,015
v= 0,020
v= 0,030
v= 0,040
v= 0,060
v= 0,080
v= 0,10
v= 0,15
v= 0,20
s in [kJ/(kg K)]v in [m^3/kg]T in [°C]
R134a Ref :D.P.Wilson & R.S.Basu, ASHRAE Transactions 1988, Vol. 94 part 2.
HVAC – Basic Cooling
Example
322
from log p,h-Diagram: h1= 401 kJ/kg, h4= 257 kJ/kg
from log p,h-Diagram: h2= 428 kJ/kg
HVAC – Basic Cooling
Example
324
Enthalpy [kJ/kg]
120 140 160 180 200 220 240 260 280 300 320 340 360 380 400 420 440 460 480 500 520 540 560 580
Pre
ssu
re [
Bar]
0,50
0,60
0,700,800,901,001,00
2,00
3,00
4,00
5,00
6,00
7,008,009,00
10,00
20,00
30,00
40,00
50,00
s =
1,7
5
s =
1,8
0
s =
1,8
5
s =
1,9
0
s =
1,9
5
s =
2,0
0
s =
2,0
5s
= 2
,10
s = 2
,15
s = 2
,20
s = 2
,25
s = 2
,30
s = 2
,35
s = 2
,40
-4 0 -2 0 0 2 0 4 0 6 0 8 0 1 0 0 1 2 0 1 4 0 1 6 00,0
020
0,0030
0,00400,0050
0,00600,0070
0,0080
0,0090
0,010
0,015
0,020
0,030
0,040
0,050
0,060
0,070
0,080
0,090
0,10
0,15
0,20
0,30
0,40
0,50
0,60
0,70
0,80
-50
-40
-30
-20
-10
0
10
20
30
40
50
60
s = 1 ,0 0 1 ,2 0 1 ,4 0 1 ,6 0 1 ,8 0
x = 0 ,1 0 0 ,2 0 0 ,3 0 0 ,4 0 0 ,5 0 0 ,6 0 0 ,7 0 0 ,8 0 0 ,9 0
DTU, Department of Energy Engineering
s in [kJ/(kg K)]. v in [m^3/kg]. T in [ºC]
M.J. Skovrup & H.J.H Knudsen. 08-03-05
R407C Ref :DuPont SUVA AC9000
HVAC – Basic Cooling
Example - data
326
refrigerant = working substance of the refrigeration cycle
HVAC – Refrigeration Liquids
Definition & Common substances
Definition
CFCs: chlorofluorocarbons (perfluorinated)
HCFCs: hydrochlorofluorocarbons
HFCs, FCs: chlorine-free hydro-fluorocarbons
Common substances
327
CFCs: such as R11, R12 use banned (federal official journal
309/1990 of 17/05/1990).
HCFCs: such as R22 use prohibited for new systems from
01/01/2002 (federal official journal 750/1995).
HCFCs: use prohibited also for systems in use from 01/01/2015 .
HFCs, FCs: such as R134a, are prohibited for air-conditioning of
vehicles.
HVAC – Refrigeration Liquids
Restrictions of use
328
coefficient of performance
volumetric cooling performance
discharge temperature
compression ratio
boiling pressure
condensation pressure
Oil-miscibility
thermal stability
HVAC – Refrigeration Liquids
Selection criteria (1)
329
Safety
Inflammable
Explosive
Toxic
Environment
ODP (Ozon Depletion Potential)
GWP (Global Warming Potential)
HVAC – Refrigeration Liquids
Selection criteria (2)
330
refrigerant ozone depletion
potential ODP
global warming
potential GWP100
boiling
temperature °C
R134a (CFCH2F) 0 1.300 -26,4
R125 (CF3CHF2) 0 3.200 -48,6
R32 (CH2F2) 0 580 -51,6
R143a (CF3-CH3) 0 4.400 -47,4
R404A (CF3CHF2-CF3CH3-
CF3CH2F) 0 3.800 -46,5
R407C (CH2F2-CF3CHF2-
CF3CHF2F) 0 1.600 -44,0
R507A (CF3-CHF2-CF3CH3) 0 3.800 -47,2
HVAC – Refrigeration Liquids
Various refrigerants & basic properties (1)
331
refrigerant name ozone depletion
potential ODP
global warming
potential GWP100
boiling
temperature °C
ammonia R717
(NH3) 0 0 -33,6
propane R290
(CH3 CH2 CH3) 0 3 -42
Isobutane R600a
(C4H10) 0 3 -11,9
carbon dioxide R744
(CO2) 0 1 -78,4
water R718
(H2O) 0 0 100
HVAC – Refrigeration Liquids
Various refrigerants & basic properties (2)
333
GEJO01_014
condenser
accumulator
evaporator
expansion
valve
Filter/dryer
Sight glass
magnetic
valve
compressor
HVAC – heat exchangers, components & parts
Components
334
open compressors
Motor is not integrated in the compressor casing
hermetic compressors
Motor is integrated in the compressor casing, casing is hermetically
welded or soldered
semi-hermetic compressors
Motor is integrated in the compressor casing; casing is bolted = can be
disassembled
HVAC – heat exchangers, components & parts
Components
335
The motor of hermetic compressors is fully integrated in the casing.
Therefore, it is in general not possible to discharge the waste heat
directly to the surrounding area. Without cooling, the compressor motor
would burn. Most commonly, the suction gas is used for cooling. Before
reaching the cylinder, the suction gas passes the motor. Hence, the
motor is cooled, while the suction gas temperature will rise.
HVAC – heat exchangers, components & parts
Components
Suction gas cooled compressors
336 HVAC – heat exchangers, components & parts
Compressors
reciprocating
piston
sliding vane roll piston rotary piston
339
A…rotor D…piston G… shell
B…stator E…piston rod H…electrical connections
C…cylinder F…sliding crank
HVAC – heat exchangers, components & parts
Compressors
341
capillary tube: thin copper tube - in appropriate length - causing the needed pressure drop.
thermostatic expansion valve: controlling the superheating at the outlet of the evaporator (mechanical).
electronic expansion valve: controlling the superheating at the inlet of the evaporator (electronically).
float valve: modulates the flow of liquid refrigerant to the evaporator or to the collector (when a flooded evaporator is used, the filling level is modulated in the evaporator).
orifice plate: for high capacities (steady operating point).
HVAC – heat exchangers, components & parts
Throttling devices
346
counter flow
parallel flow
cross flow
cross parallel flow
HVAC – heat exchangers, components & parts
Heat Exchangers
347
DTE DTA
t [°C]
length [m]
DTG
DTK
t [°C]
length [m]
HVAC – heat exchangers, components & parts
Heat Exchangers
348
De-superheating
Condensing
Sub-cooling
Q
CQ
0Q
T
P
Vaporising
Superheating
HVAC – heat exchangers, components & parts
Heat Exchangers
356
temporary storage of refrigerant.
protects from overflowing.
secures sub-cooling at condensator outlet.
HVAC – heat exchangers, components & parts
Accumulators
357
removes humidity (water) from the refrigerant
residual moisture when assembling, or repairing
oil
Refrigerant
humidity in refrigerants can cause acidification
frosting around expansion valve at temperatures below 0 °C
obstruction of nozzle low pressure fault
HVAC – heat exchangers, components & parts
Dryers
362
Advantages:
great performances.
low re-cooling temperature possible.
Disadvantages:
water demand (evaporation, elutriation).
Water treatment (hardness stabilisation, softening, chemicals needed).
legionella risk (biocidal treatment).
HVAC – heat exchangers, components & parts
Cooling Towers