Environmental Engineering. Family of heating appliances

Similar documents
Project: Underfloor and wall heating example

FUNDAMENTALS OF HVAC

TREES Training for Renovated Energy Efficient Social housing

Environmental Engineering

Chapter 1: 20, 23, 35, 41, 68, 71, 76, 77, 80, 85, 90, 101, 103 and 104.

BUS5 Building structures 5: Fire safety

1/54 Circulation pump, safety valve, expansion vessel

Cooling of Electronics Lecture 2

Examination Heat Transfer

Thermal behavior and Energetic Dispersals of the Human Body under Various Indoor Air Temperatures at 50% Relative Humidity

Radiant Heating Panel Thermal Analysis. Prepared by Tim Fleury Harvard Thermal, Inc. October 7, 2003

New correlations for the standard EN 1264

Study on Thermal Load Calculation for Ceiling Radiant Cooling Panel System

Determination of heat losses of a concrete silo for sugar and a fan project

INVESTIGATION OF THE PERFORMANCE OF COOLING PANELS: CEILING AND FLOOR PANElS.

Available online at ScienceDirect. Procedia Engineering 121 (2015 )

Coolant. Circuits Chip

If there is convective heat transfer from outer surface to fluid maintained at T W.

Principles of Food and Bioprocess Engineering (FS 231) Problems on Heat Transfer

Building Envelope Requirements Overview Page 3-4

COVENANT UNIVERSITY NIGERIA TUTORIAL KIT OMEGA SEMESTER PROGRAMME: MECHANICAL ENGINEERING

EXPERIMENTAL AND SIMULATION TEMPERATURE EVALUATION WHICH DETERMINE THERMAL COMFORT

Examination Heat Transfer

University of New Mexico Mechanical Engineering Spring 2012 PhD qualifying examination Heat Transfer

Ceiling Radiant Cooling Panels Employing Heat-Conducting Rails: Deriving the Governing Heat Transfer Equations

Determination of installed thermal resistance into a roof of TRISO-SUPER 12 BOOST R

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

industry hall : highbay luminaire NJ700 LED Project number : sample system Customer : Processed by : Siteco Light Consulting Date : 07/2013

Response function method

PROBLEM 9.3. KNOWN: Relation for the Rayleigh number. FIND: Rayleigh number for four fluids for prescribed conditions. SCHEMATIC:

Iterative calculation of the heat transfer coefficient

S.E. (Chemical) (Second Semester) EXAMINATION, 2012 HEAT TRANSFER (2008 PATTERN) Time : Three Hours Maximum Marks : 100

PHOS 25 Downlight LED PROJECTOR

Heat Tracing Basics. By: Homi R. Mullan 1

1. Basic state values of matter

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 3 August 2004

CFD as a Tool for Thermal Comfort Assessment

It is easiest to create a table of values and calculate the energy consumption piece by piece.

TankExampleNov2016. Table of contents. Layout

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

Vincent Barraud SOPREMA BASICS OF THERMAL INSULATION

SECONDARY SCHOOLS ANNUAL EXAMINATIONS 2005 Educational Assessment Unit Education Division. FORM 4 PHYSICS Time: 1 hr. 30 min.

MEASUREMENT OF THE AIRFLOW AND TEMPERATURE FIELDS AROUND LIVE SUBJECTS AND THE EVALUATION OF HUMAN HEAT LOSS

Numerical simulation of human thermal comfort in indoor environment

Arc welding Arc theory. CTU in Prague Faculty of Mechanical Engineering

Calculating the heat transfer coefficient of frame profiles with internal cavities

Natural convection heat transfer around a horizontal circular cylinder near an isothermal vertical wall

Anna Majchrzycka THERMAL COMFORT

( )( ) PROBLEM 9.5 (1) (2) 3 (3) Ra g TL. h L (4) L L. q ( ) 0.10/1m ( C /L ) Ra 0.59/0.6m L2

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

Radiation Heat Transfer. Introduction. Blackbody Radiation. Definitions ,

Thermal Unit Operation (ChEg3113)

Numerical Analysis of Comfort and Energy Performance of Radiant Heat Emission Systems

EVALUATION OF THERMAL ENVIRONMENT AROUND THE BLIND ON NON-UNIFOM RADIANT FIELDS A CFD SIMULATION OF HEAT TRANSFER DISTRIBUTION NEAR THE BLINDS

tel.: , fax: , mobile:

Simplified Collector Performance Model

True/False. Circle the correct answer. (1pt each, 7pts total) 3. Radiation doesn t occur in materials that are transparent such as gases.

Field evaluation of the performance of a radiant heating/cooling ceiling panel system

PROBLEM 1.2 ( ) 25 C 15 C dx L 0.30 m Ambient air temperature, T2 (C)

An ion follows a circular path in a uniform magnetic field. Which single change decreases the radius of the path?

CHAPTER 5 CONVECTIVE HEAT TRANSFER COEFFICIENT

Fundamentals of light

Fundamentals of light

CIBSE Guide A: corrigenda

Solar Flat Plate Thermal Collector

ENSC 388. Assignment #8

PHOS 15 LED PROJECTOR

MODULO DIAGRAMMA-FOTO Instructions for the correct disposal of waste

ABSTRACT INTRODUCTION. flow rate on the load variation was not given.

Convection Heat Transfer of Nanofluids in Commercial Electronic Cooling Systems

4D11 Building Physics LECTURE 1. 1 Introduction 2 HEAT TRANSFER IN BUILDINGS

Analysis of radiant characteristics of electric panels FENIX for heating.

Characterisation of Deposits on Membrane Walls of Steam Generators by Heat Flux Density Measurement

Air Diffusion Designing for Comfort

BSE Public CPD Lecture Numerical Simulation of Thermal Comfort and Contaminant Transport in Rooms with UFAD system on 26 March 2010

UNIVERSITY OF HONG KONG Faculty of Engineering M.Sc.(Eng) in Building Services Engineering MEBS6002 LIGHTING ENGINEERING

ME 305 Fluid Mechanics I. Part 8 Viscous Flow in Pipes and Ducts. Flow in Pipes and Ducts. Flow in Pipes and Ducts (cont d)

On the Emissivity of Silver Coated Panels, Effect of Long Term Stability and Effect of Coating Thickness

Transient natural ventilation of a room with a distributed heat source

FLOOR VIBRATIONS FREQUENTLY ASKED QUESTIONS AND MORE. Frequently Asked Question. Questions Concerning Design for Walking Excitation

Computer Evaluation of Results by Room Thermal Stability Testing

ROOM AVERAGE VELOCITY EQUATION A TOOL TO IMPROVE DESIGN OF THERMAL COMFORT CONDITIONS

IDA ICE CIBSE-Validation Test of IDA Indoor Climate and Energy version 4.0 according to CIBSE TM33, issue 3

TRANSMISSION OF HEAT

Chartered Institute of Building Service Engineers (CIBSE) code for interior lighting design

Radiative Equilibrium Models. Solar radiation reflected by the earth back to space. Solar radiation absorbed by the earth

Standard Test Method for Measuring the Steady-State Thermal Transmittance of Fenestration Systems Using Hot Box Methods 1

ME 305 Fluid Mechanics I. Chapter 8 Viscous Flow in Pipes and Ducts

The energy performance of an airflow window

PROBLEM Node 5: ( ) ( ) ( ) ( )

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

Chapter 2: The Law of Conservation of Mass

EN 10211:2007 validation of Therm 7.4. Therm 7.4 validation according to EN ISO 10211:2007

EXPERIMENT AND SIMULATION OF RADIANT/CONVECTIVE SPLIT FROM PASSENGER IN AIRCRAFT CABINS

MATERIAL PROPERTIES test methods comment

Geometrical diameter, height = m = m. Geometrical diameter, height = m = m CIE code =

Case Study in Reinforced Concrete adapted from Simplified Design of Concrete Structures, James Ambrose, 7 th ed.

MNFFY 221/SIF 4082 Energy and Environmental Physics. 2002

3mm Advanced Super Flux LEDs B84-YSC-A1T1U1DH-AM

CRYOGENIC CONDUCTION COOLING TEST OF REMOVABLE PANEL MOCK-UP FOR ITER CRYOSTAT THERMAL SHIELD

Transcription:

Fakulta strojní Ústav techniky prostředí Family of heating appliances Ing. Ondrej Hojer, Ph.D. Table of contents: A) Design of Floor heating B) Design of a safety valve and an expansion vessel C) Introduction to large space heating 2

Design of Floor heating Characteristic floor number m = 2 Λ + Λ a b π 2 k d d [/m] Heat distribution layer (the one with tubes) where: Λ a [W/m 2.K] Λ b [W/m 2.K] k d [W/m.K] d [m] heat transfer coefficient upwards from the tubes (on the fig. red arrows) heat transfer coefficient downwards from the tubes (on the fig. yellow arrows) thermal conductivity of heat distribution layer material (the layer with the tubes) external tube diameter partial heat transmissivity upwards from the tubes Λ = a d i + k h i where : d [m] particular thicknesses of layers above the tubes, k i [W/m.K] thermal conductivities of layers above the tubes, h = h + h = 4, 80 + 5, 25 = 0, 05 W / m 2.K R C partial heat transmissivity downwards from the tubes Λ [W/m 2.K] = = b d i + R + ceil k h h i summary heat transfer coefficient on the floor heat transfer coeff. by convection and by radiation where : R ceil [m 2.K/W] thermal resistance of the ceiling, h [W/m 2.K] summary heat transfer coefficient on the bottom side of the heated floor (standard - in case there is another room this coefficient is chosen as h = 8 W/m 2.K) 2

Floor surface temperature is calculated from equation l Λ tgh m 2 t t = a ( t t ) s i h m i l m 2 [ C] where : t m [ C] mean water temperature (t w +t w2 )/2 t i [ C] indoor design temperature m [m - ] characteristic floor number Λ a [W/m 2.K] heat transfer coefficient upwards from the tubes h [W/m 2.K] summary heat transfer coefficient by convection and radiation upwards l [m] tubes distance Principle of the calculation is to keep surface temperature bellow the hygienic limits (floor heating = 29 C). Hence maximal thermal output is limited. Mean surface temperature t s shall not from physiological point of view exceed the value: t s = 27 to 29 C at room for permanent stay (rooms for living, offices,...), t s = 30 to 32 C at service rooms, where people are just temporary (halls, corridors, stairs,...), t s = 32 to 34 C at rooms, where people are mainly walking barefooted (swimming pools, spa, bath rooms...). At given water temperatures t m... (t w +t w2 )/2 and internal design air temperature t i, the mean surface temperature t s depends mainly on distance between tubes l. Other values are either almost constant or they have just small influence on results. The specific thermal heat flux to the room is than defined: q = h t t s i [W/m 2 ] and specific heat flux of the floor surface downwards when both air design temperatures in rooms upwards and downwards are the same h q = Λ t t b Λ s i [W/m 2 ] a 3

We the design temperatures up and down are different t i t i downward is calculated q = Λ h b Λ t t + Λ t t s i b i i a [W/m 2 ], specific heat flux This heat flux represents heat loss that has to be minimized as possible. In case there is an unheated room bellow the floor it is necessary to choose for the layers located bellow the tubes materials with lower thermal conductivity than in cases when there is another heated room. Mostly it is required that heat flux downwards shouldn t be higher than approx. 0 up to 5 % of the total heat output of the floor For rooms located below other heated rooms the total heated surface is calculated A P ΦHL,i = q + q [m 2 ] whereϕ HL,i is total heating load of the room (EN 283). In rooms at ground floor or on the highest floor the heated surface is calculated from an equation: A P = φ HL,i q [m 2 ] and total thermal power needϕ PN is for both cases given by equation φ = (q + q ).A P PN [W] 4

Design of an Expansion vessel 9 B EV NP M PR PR PR h PR B EV NP M h V et Panel radiator Boiler Expansion vessel Neutral point Manometer Height of water column between highest point of system and neutral point NP =,3 V n o η 0 5

t max = t max t min feed water temperature (mostly 0 C) maximal operation temperature η = p p h,max,a p h,max,a d,min,a 2 6

3 p =, ρ g h 0 + d,dov,a p B 3 Pressure of the dry air or nitrogen is set to the value: p et,set. = (, až,3).ρ.g.h.0-3 [ kpa ]. 4 7

Central air distr. system Floor heating Local air distr. system Radiant Strips Plaque radiant heaters Tube radiant heaters Floor (panel) heating 8

Radiant strips (panels) Tube radiant heaters 9

Plaque (luminous) radiant heaters Local air-distribution systems 0

Central air-distribution systems Vertical space characterization A Occupancy zone B Neutral zone C Roof zone