TREES Training for Renovated Energy Efficient Social housing

Similar documents
A SIMPLE MODEL FOR THE DYNAMIC COMPUTATION OF BUILDING HEATING AND COOLING DEMAND. Kai Sirén AALTO UNIVERSITY

Calculating the heat transfer coefficient of frame profiles with internal cavities

THERMAL TRANSMITTANCE OF MULTI-LAYER GLAZING WITH ULTRATHIN INTERNAL PARTITIONS. Agnieszka A. Lechowska 1, Jacek A. Schnotale 1

Δ q = ( ψ L) HDH (1) here, Δq is the additional heat transfer caused by the thermal bridge, Ψ and L are the linear thermal transmittance and length of

Customer: Ashton Industrial Sales Ltd. South Road, Harlow Essex CM20 2AR UNITED KINGDOM. Project/Customer: Profilex HM spacer

FUNDAMENTALS OF HVAC

CAE 331/513 Building Science Fall 2016

TRANSPARENT INNOVATIVE MATERIALS: ENERGETIC AND LIGHTING PERFORMANCES EVALUATION

5. AN INTRODUCTION TO BUILDING PHYSICS

Energy flows and modelling approaches

EFFECT OF INTERNAL LONG WAVE RADIATION AND CONVECTION ON FENESTRATION SIMULATION

Solar Control in Traditional Architecture, Potentials for Passive Design in Hot and Arid Climate

SIMULATION OF FRAME CAVITY HEAT TRANSFER USING BISCO v10w

ISO INTERNATIONAL STANDARD. Thermal performance of windows, doors and shutters Calculation of thermal transmittance Part 1: Simplified method

AR/IA 241 LN 231 Lecture 4: Fundamental of Energy

Here Comes the Sun. Rachel Wagner. Duluth Energy Design Conference 26 February

DYNAMIC INSULATION APPLIED TO THE RESIDENTIAL BUILDING (PART 2) Numerical Evaluation of Thermal Insulation Effect on Air Supply Window System

Experimental measurements and analysis of the indoor conditions in Italian museum storerooms: a study case

Winter Thermal Comfort in 19 th Century Traditional Buildings of the Town of Florina, in North-Western Greece

ISO INTERNATIONAL STANDARD

Definitions of U- and g-value in case of double skin facades or vented windows

Thermal Comfort; Operative Temperature in the Sun

Determining of Thermal Conductivity Coefficient of Pressed Straw (Name of test)

Aalborg Universitet. Publication date: Document Version Publisher's PDF, also known as Version of record

PAUL RUDOLPH Oriental Masonic Gardens

Fundamentals of WUFI-Plus WUFI Workshop NTNU / SINTEF 2008

METHOD OF IN-SITU MEASUREMENT OF THERMAL INSULATION PERFORMANCE OF BUILDING ELEMENTS USING INFRARED CAMERA

NUMERICAL ANALYSIS OF HEAT STORAGE AND HEAT CONDUCTIVITY IN THE CONCRETE HOLLOW CORE DECK ELEMENT

Parametric Study on the Dynamic Heat Storage Capacity of Building Elements Artmann, Nikolai; Manz, H.; Heiselberg, Per Kvols

Aalborg Universitet. Empirical Test Case Specification Larsen, Olena Kalyanova; Heiselberg, Per Kvols. Publication date: 2006

ADVANCED ROOF COATINGS: MATERIALS AND THEIR APPLICATIONS

COMMERCIAL HEAT GAIN - HEAT LOSS CALCULATION LOAD FORM

Design for Airtightness and Moisture Control in New Zealand housing

3D UNSTEADY STATE ANALYSIS OF THERMAL PERFORMANCE OF DIFFERENTLY INSULATED FLOORS IN CONTACT WITH THE GROUND

CFD MODELLING AND ANALYTICAL CALCULATIONS OF THERMAL TRANSMITTANCE OF MULTI-LAYER GLAZING WITH ULTRATHIN INTERNAL GLASS PARTITIONS

Serge 600 COLLECTION REFLECTS SUNLIGHT OUTDOORS GLASSFIBRE OF = 5%

The energy performance of an airflow window

5. Thermal Design. Objective: Control heat flow to: Maintain comfortable indoor conditions

Warm surfaces warm edges Insulated glass with thermally improved edge seal

Cooling of Electronics Lecture 2

Response function method

Building heat system sizing

Aalborg Universitet. Comparative Test Case Specification Larsen, Olena Kalyanova; Heiselberg, Per Kvols. Publication date: 2007

Natté P CLARITY & COMFORT POLYESTER OF = 1-10% COPACO NATTÉ P

Project 2. Introduction: 10/23/2016. Josh Rodriguez and Becca Behrens

Experimental Performance and Numerical Simulation of Double Glass Wall Thana Ananacha

Solar Radiation 230 BTU s per Hr/SF. Performance Glazing Coatings, Layers & Gases

Aalborg Universitet. Final Empirical Test Case Specification Larsen, Olena Kalyanova; Heiselberg, Per Kvols. Publication date: 2008

Natté COLLECTION CLARITY & COMFORT GLASSFIBRE OF = 1-10% COPACO NATTÉ

HIGHLY INSULATING AEROGEL GLAZING

Baker House Dining Room: Thermal Balance Report. + Q c. + Q v. + Q s. + Q e. + Q heating. + Q appliances. =Q appliances,21h Q appliances, x H

Appendix 5.A11: Derivation of solar gain factors

SIMULATED THERMAL PERFORMANCE OF TRIPLE VACUUM GLAZING. Yueping Fang, Trevor J. Hyde, Neil Hewitt

Blockout Déco N203 COLLECTION BLOCK SUNLIGHT BLOCKOUT OF = 0% COPACO BLOCKOUT DÉCO N203

2 Verification of the design prerequisites (Design intent)

The thermal performance of lightweight timber frame structures during the summer period

Double-Skin Facade in Low-Latitude: Study on the Absorptance, Reflectance, and Transmittance of Direct Solar Radiation

Performance of Fixed Horizontal Shading Devices in South Facing Residential Buildings in Dhaka

Window energy rating systems

PASSIVE SOLAR HEATING

CZECH TECHNICAL UNIVERSITY IN PRAGUE FACULTY OF MECHANICAL ENGINEERING DEPARTMENT OF ENVIRONMENTAL ENGINEERING

COVENANT UNIVERSITY NIGERIA TUTORIAL KIT OMEGA SEMESTER PROGRAMME: MECHANICAL ENGINEERING

CityBEM: an Open Source Implementation and Validation of Monthly Heating and Cooling Energy Needs for 3D Buildings in Cities

Orientation of Building

Computer Evaluation of Results by Room Thermal Stability Testing

Coolant. Circuits Chip

BRE Client Report. Calculation of summertime solar shading performance for MicroLouvre. Prepared for: Smartlouvre. BRE Watford, Herts WD25 9XX

THERMAL BUILDING MODELLING ADAPTED TO DISTRICT ENERGY SIMULATION

EXPERIMENTAL DETERMINATION OF SPECTRAL AND ANGULAR DEPENDENT OPTICAL PROPERTIES OF INSULATING GLASSES

Working of a SUNLUX SUNSCREEN

ISO INTERNATIONAL STANDARD. Thermal bridges in building construction Linear thermal transmittance Simplified methods and default values

STUDY OF A PASSIVE SOLAR WINTER HEATING SYSTEM BASED ON TROMBE WALL

THERMAL COMFORT IN HIGHLY GLAZED BUILDINGS DETERMINED FOR WEATHER YEARS ON ACCOUNT OF SOLAR RADIATION. Dominika Knera 1 and Dariusz Heim 1

Building physics. Reinforced concrete/reinforced concrete. Steel/reinforced concrete. Timber/reinforced concrete. Steel/steel.

THERMAL SIMULATION REPORT. TCL2013-Origin-01 Prepared For:

UNIT FOUR SOLAR COLLECTORS

CAE 463/524 Building Enclosure Design Fall 2012

The influence of solar radiation on the distribution of temperatures in historic masonry

Available online at ScienceDirect. Energy Procedia 78 (2015 )

MNFFY 221/SIF 4082 Energy and Environmental Physics. 2002

Homework #4 Solution

(Refer Slide Time: 00:01:19 min)

Description of Benchmark Cases for Window and Shading Performance Calculation

A fire resistance assessment case history G.C. and M.E. Giuliani

Solar Radiation Protections on Façades: A Case Study in a Hot Semi-Humid Climate

LOW E SATINÉ 5500 LOW E

LOW E SATINÉ 5500 LOW E

Quasi-steady state and dynamic simulation approaches for the calculation of building energy needs: Part 1 thermal losses

2. Climate (Outdoor) Altitude. Distance from the ocean. Conditions of the ocean. Store/release heat. angle of solar radiation Amount of solar energy

TECHNICAL COMMITTEE of the EU Cool Roofs Council

QIRT th International Conference on Quantitative InfraRed Thermography

Thermal performance of the new hall of the historical hospital in Florence

Solar Flat Plate Thermal Collector

THERMAL INERTIA OF HOLLOW WALL BLOCKS: ACTUAL BEHAVIOR AND MYTHS

HOT /05/2014. Page 1 of 14 GENERAL HOUSE CHARACTERISTICS. Natural Resources CANADA Version sample house report

Simplified Collector Performance Model

THE INFLUENCE OF GLAZING TYPE, FRAME PROFILES SHAPE AND SIZE OF THE WINODOW OF THE FINAL VALUE OF WINDOW THERMAL TRANSMITTANCE U

Chapter Seven. Solar Energy

STUDENT MODELLING COMPETITION

Transient Analysis of the Buoyancy Driven Flow in a Passive Solar System for Indoor Heating

Transcription:

TREES Training for Renovated Energy Efficient Social housing Intelligent Energy -Europe programme, contract n EIE/05/110/SI2.420021 Section 2 Tools 2.1 Simplified heating load calculation Tamas CSOKNYAI BUTE

Contents Objectives and principle Principle of heating load calculation Heat losses Transmission losses (multi layers stuctures, air gaps, thermal bridges) Ventilation losses (ACH, air tightness, heat recovery) Heat losses during a period: degree hours, balance-point temperature Heat gains Solar gains, shading devices Internal heat charges Thermal mass Conclusions 1

Objectives and principle Objective : decrease the heating energy consumption and the heat demand Principle : decrease of the transmission and ventilation losses, utilization of the solar gains and optimization of the equipments Example : passive house labeling in Germany, Minergie in Switzerland EPBD: European Energy Performance Directive on Buildings, in force since January 2006 Energy certification Regular inspection of boilers and air conditionning systems Tools : simplified energy balance, dynamic simulation tools (see section 2.2) European standards EN 832, EN ISO 13790 2

Heating energy balance of a building Φ Φ tr H + Φ = Φ vent tr + Φ + Φ sol vent + Φ Φ int sol ± Φ Φ T stored int ± Φ T ( Φ Φ ) stored H + Φ system losses system losses = = 0 0 Φ H Φ tr Φ vent Φ sol Φ int Φ stored τ Φ system losses Heating load Transmission losses Ventilation losses Solar gains Internal heat charges Variation of stored heat in function of time Losses of the heating system (distribution losses) 3

Heating load calculation With other words (according to Standard EN ISO 13790) Heating load = = heat losses η. (solar + internal gains) + distribution losses 4

Heat losses Transmission losses through the building envelope Exposed surfaces: facade walls, roof, ground Openings (windows, doors) Thermal bridges Ventilation losses: Opening of windows Losses of mechanical ventilation system In- or exfiltration of air Depends also on the indoor air temperature (control, zones) and the outdoor conditions (latitude, altitude) 5

TRANSMISSION LOSSES 6

Transmission through multim ulti-layer layer structures Transmission losses: Φ tr = U. A. (ϑ i ϑ e ) [W] U-value: Air-to-air conductance (thermal transmittance) R: thermal resistance of a layer U = 1 / ΣR [ W/m 2 /K] A: Surface of the exposed elements [m 2 ] ϑ i : Design indoor air temperature ϑ e : Design outdoor air temperature U = 1 h i + 1 1 h = R + + j + e 1 h i 1 1 h e d λ j j Total heat transfer through a building element is a result of conduction, convection radiation 7

Conductivity of materia rials polystyrene λ = 0.04 W/mK reinforced concrete λ = 2,1 W/mK wood λ = 0.15 W/mK glass λ = 1 W/mK steel λ = 50 W/mK 8

Convection+linearised radiaton h = h c + h r [W / m2 / K] Φ= h. (ϑ 1 ϑ 2 ) h i and h e R i = 1/h i R e = 1/h e 9

Special cases for determining U-value: U Air layers Air gap between two materials Thermal resistance depends on position, width and level of ventilation Thermal resistance in function of the width of air gap width 10

Special cases : Non homogeneous materials Non homogeneous materials, average R (usually given by the producer) Examples : brick of 5 cm, R = 0.11 m 2.K/W insulating masonary blocks (bricks with holes) of 44 cm («Phorotherm»), R = 2.57 m2.k/w 11

Walls, floor and roof Facades Uf Af Uf. Af Floor Ufl Afl Ufl. Afl Roof Ur Ar Ur. Ar TOTAL Σ (U. A) transmission heat losses : ΦT = Σ (U. A). (ϑi ϑe) + windows, doors and thermal bridges 12

Doors and windows Single glazing : U = 5.5 W/m2/K Double glazing : U = 3.3 W/m2/K + low-emissivity coating : U=1.8 W/m2/K + argon filling : U = 1.1 W/m2/K Wooden frame : U = 2.4 W/m2/K PVC frame : U = 1.7 W/m2/K Average U-value: mean value weghted with proportion of area, e.g. 75% glazing, 25% frame + losses caused by spacer Door : according to thickness and material (R) 13

Thermal bridges Ψ [W/mK]: Linear heat loss. Can be determined using: Thermal bridge catalogues Thermal bridge calculation tools Some producers of complete construction systems publish their usual Ψ-values in catalogues 14

Thermal bridges (examples) ψ= 0.05 Ψ= 0.8 -> 1 Ψ= 0.5 -> 0.7 W/m/K Φ = ψ. L. (Ti Te) ψ in W/m/K 15

VENTILATION LOSSES 16

Calculation of ventilationv losses Minimum ACH determined by: Biological need (fresh air for breathing) Required ACH for fabric protection 2 ways of determination of ACH: Fresh air required per person : 30 m 3 /h,person Minimal air change rate: n min =0,5 h -1 Infiltrations (spontanous losses through window gaps, joints, shafts ) Ventilation losses : ACH.V.ρ.C.(ϑ i ϑ e ) ACH: Air change rate [h -1 ] ρ : density of air, [ m 3 /h ] C : heat capacity of air = 1000 J/kg,K 17

Preheating of ventilation air, heat recovery Supply air Bathroom Living room Fresh air Heat recovery unit Kitchen Bedroom Ventilation heat loss: x (1- η) Efficiency of heat recovery η = 60.. 90% 18

Preheating in a sunspace Buffer space Thermal mass 19

SOLAR GAINS 20

Solar radiation 3 parties : direct, diffuse, reflected Radiation global horizontal Radiation on different vertical orientations 21

Solar gains Utilised solar gains depend on: Climate Geographical position of the site Orientation of glazing Shading objects (neighbouring buildings, trees) Shading coefficient of shading devices g-value of the glazing Thermal mass of the building DESIGN VALUES OF SOLAR RADIATION DEPEND ON THE LOCATION AND ARE GIVEN BY THE STANDARDS 22

Shadowing devices and movable insulation Shadowing devices and movable insulation are of importance both in winter and summer from the points of view of reducing transmission heat losses and controlling solar penetration. If the shadowing device is outside, in front of the glazing, the total solar energy transmittance can be as low as 0,1-0,4. For the same device, if it is behind of the glazing, the shading coefficient is higher: 0,4-0,7. 23

Sun path diagram and shadow mask calculator Sun path diagram and shadow mask calculator are tools to determine the shading effect of the neighbouring objects and shading devices 24

INTERNAL GAINS 25

Internal gains Occupants : about 100 W / person (in function of physical activity) Artificial lighting Office equipments (computers, photocopy machines) Cooking A part is lost (e.g. hot water) 26

Energy consumption reduction by solar and internal gains The real reduction is only a part of the internal and solar gains. Expressed with efficiency: η η depends: - The proportion of the gains (γ : gains Φg / losses ΦL) - The thermal mass and the time constant of the building - Heavy building can utilise more gains than light ones 27

THERMAL MASS 28

Thermal mass The change of the stored heat is proportionate to the change of the temperature, the mass (m) and the specific heat (C): q = m*c* T concrete : C=0.26 Wh/kg/K, 2400 kg/m3 wood : C= 0.36 Wh/kg/K, 630 kg/m3 polistyrene : C= 0.34 Wh/kg/K, 25 kg/m3 glass : C= 0.5 Wh/kg/K, 2500 kg/m3 29

External and internal insulation,, time constant Time constant depends on the level of thermal transmittance (H=A*U) and heat capacity τ = C / H If external insulation: lower H higher τ If heavy structures: higher C higher τ If internal insulation: lower thermal mass lower τ Maximum 10 cm of the inner part of exposed structures can store heat (for 24 hours). Mass and resistance of this layer is a key issue. Intermittent (programmed) heating can result in energy saving because of thermal mass 30

HEATING LOAD CALCULATION FOR A PERIOD 31

Heat losses during a period Heat loss coefficient: losses in case of 1K temperature difference: H = HT + HV HT = {Σ (U. A) + Σ (ψ. L ) thermal bridges) walls, roof, ground, windows and doors HV = ACH.V.ρ.C Φ = H.(ϑ i ϑ e ) Prescribed indoor air temperature for example ϑ i = 20 C ϑ e variable during the heating season Yearly losses = Σ monthly losses = Σ hourly losses Σ H (20 ϑ e ) = H. Σ (20 ϑ e ) Degree - hours based on 20 C 32

Degree - hours Simplification of climatic model Σ (18 ϑ e ) = degree hours based on ϑ i = 18 C Heating not needed if T e >= balanced point temperature, depends on climate e.g. 12 C (internal heat gains) Examples for yearly degree hours: Warshaw: 93 000 degree hours Budapest: 72 000 degree hours Paris : 58 000 degree hours Nice : 32 000 degree hours Athens: 34 000 degree hours Copenhagen: 70 000 degree hours 33

Heating period θext θint η1. Q g / (H. 24 ) θext : daily average outdoor temperature θint : daily average indoor temperature η1 = a / (a+1) (η for γ = 1) Q g : daily average gains H = total heat losses in W/K In case of monthly calculations: a = 1 + τ / 15 Time constant τ = C / H 34

Conclusions EPBD, Energy certification, energy label Links with simulation Normative references: EN 832: Thermal performance of buildings Calculation of energy use for heating Residential buildings pren 410: Glass in building Determination of luminous and solar characterisics of glazing EN ISO 7345: Thermal insulation Physical quantities and definitions (ISO 7345:1987) pren ISO 10077-1 Windows, doors and shutters Thermal transmittance Part 1: Simplified calculation method EN ISO 13786: Thermal Performance of Building components Dynamic thermal characteristics Calculation method EN ISO 13789: Thermal Performance of Buildings Transmission heat loss coefficient Calculation method 35