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Czech Technical University in PragueFaculty of Civil Engineering
Department of Microenvironmental and Building Services Engineering
Michal Kabrhel 12008/2009
Heating systemsApllied thermodynamics
Indoor environment
2Michal Kabrhel
Heating
n The function n Heat supply to guarantee required indoor
temperaturen Heat supply for technology n Heat supply for hot water generation
n The principle
3Michal Kabrhel
Heating - History 700 BC - 0
Hypocausta
4Michal KabrhelBEE1 - prof.Kabele
Heating - History – Middle Ages
n Fireplace, stove
5Michal Kabrhel
Heating - History 18th-19th
century - steam system
6Michal Kabrhel
Heating - History 20thcentury
7Michal Kabrhel
History 20th century warm water systems
Steam systems are replaced by warm water ones - use of electricity, pumps, control
Warm water boiler Strebl 1927
8Michal Kabrhel
1900-1945
9Michal Kabrhel
Heating nowadaysn Warm water systemsn Gas boilers operated by
electronics n Heating surface inside
floor, wall, ceilingn Computer models
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Heating nowadays
11Michal Kabrhel2008/2009
Applied thermodynamicsn Heat, heat energy
n Heat is the energy transferred between a system and its surroundings due solely to a temperaturedifference between the system and some parts of itssurroundings.
n Temperaturen State variable describing kinetics energy of the
particles of the systemn Thermodynamic /Kelvin/ T [K]n Celsius t [°C] t= T-273,15n Fahrenheit [°F] 1°F=5/9°C (°F-32).5/9=°C
12Michal Kabrhel2008/2009
Basic laws of thermodynamics
n Zeroth lawn There is a state variable TEMPERATURE. Two
systems at the same temperature are in thermodynamics equilibrium.
n The zeroth law of thermodynamics states that if forexample you have a Body (A) and a Body (B), both atthe same temperature; and then you have a Body (C) which is at the same temperature as Body (B); Therefore the temperature of Body (C) is equal to thetemperature of Body (A).
13Michal Kabrhel2008/2009
Basic laws of thermodynamics
n 1.lawn The total energy of the system plus the surroundings
is constant. (internal energy of system)n 2.law
n The second law is concerned with entropy (S), whichis a measure of disorder. The entropy of the universeincreases.
n 3.lawn It is impossible to cool a body to absolute zero
by any finite process
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Heat transfer modesn Heat Conductionn Heat is transferred between two systems
through a connecting medium, Biot-Fourier
n Heat Convection n Macroscopic movement of the matter in the
forms of convection currents. n Newton-Richman, Fourier-Kirchhof
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Heat transfer
n Transmissionconvection+conduction+convection
n Radiation nElectromagnetic waves
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Indoor environmentn Theory of the indoor environment
n Hygrothermal microclimaten Acoustic microclimaten Psychical microclimaten Light microclimaten Electrostatic microclimate
n Hygrothermal microclimaten Indoor environment state from the viewpoint of
thermal and moisture flows between the human body and surroundings
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Heat Exchange between the Human Body and the Enviroment
n Metabolic Rate Mn degree of muscular activities,n environmental conditions n body size.
n Heat loss Qn Respirationn Convectionn Radiationn Conductionn Evaporation
n Body thermal balance equationM=Q comfortM>Q hotM<Q cold
Ta
Tp
18Michal Kabrhel
n Humann Metabolic Raten Clothing Insulation
n Spacen Air Temperature (Dry-Bulb)n Relative Humidityn Air Velocityn Radiation (Mean Radiant Temperature)
2008/2009
Factors Influencing Thermal Comfort
19Michal Kabrhel
n Operative Temperature
n where tg = operative temperaturen ta = ambient air temperaturen tr = mean radiant temperaturen hc = convective heat transfer coefficientn hr = mean radiative heat transfer coefficient
2008/2009
Environmental indices
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Environmental indicesn Mean Radiant Temperature
n wheren tr = mean radiant temperaturen Ti = temperature of the surrounding surface i,
i=1,2,....,nn φrn = shape factor which indicates the fraction of
total radiant energy leaving the clothing surface 0 and arriving directly on surface i, i=1,2,...n
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Thermal comfort evaluation
n PMV index (Predicted mean vote)
n PPD index (Predictedpercentage ofdissatisfied)
Czech Technical University in PragueFaculty of Civil Engineering
Department of Microenvironmental and Building Services Engineering
Michal Kabrhel 22125BEE1_2008/2009 Michal Kabrhel
HeatingPrinciples of heating equipment
Heat emmitters
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Hot water heating
n Principlen Heating system
n Heat sourcen Distribution
networkn Heat emitter
n Heat transfer mediumn watern steamn air
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Convectors
NaturalFan-convectorsFloorWall
Michal Kabrhel
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Radiators
Michal Kabrhel
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Off-peak storage
n Staticn Dynamicn Hybrid
n Convectorn Radiator
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Air flow patterns
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Heat emittersn Design principlesn Heating outputn Locationn Covering - furnituren Connection to the pipe systemn Type
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Heater emitters design
n Covering = changes in the output
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Low - temperature radiant heating
n floor, wall and/or ceiling with embedded pipes or el.wires in concrete slabn Temperature distribution
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Underfloor heating
n History
Michal Kabrhel
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Low - temperature radiant heating
n Floor structure
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Underfloor heating - structure
TYP ATYP B
TYP C
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Low - temperature radiant heating
n Technical solutionn Pipe layout
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Low - temperature radiant heating
n Output n Limited surface temperature á limited output cca
100 W.m-2
n Energy savings n Lower air temperature á lower heat losses
n Controln Low temperature difference á autocontrol effect
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Underfloor heating - examples
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Radiant panels
n Low temperaturen heaters max 110 °C (water, steam, el. power)
n High temperaturen dark - about 350°C - radiant tube heating
system (gas)n light - about 800 °C - flameless surface gas
combustion
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Heat emitters
Czech Technical University in PragueFaculty of Civil Engineering
Department of Microenvironmental and Building Services Engineering
Michal Kabrhel 39125BEE1_2008/2009 Michal Kabrhel
HeatingHot water heating systems
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Hot-water heatingn Terminology
Boiler
Emitter
Main supply/return pipe
Branch supply/return pipe
Radiator valve
Ventcock
Drain/feed cock
Shutoff valves
Expansion vessel
Manual Control valve
Emitter
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Heating system designInitial information about the
buildingn Type
n industrial, office, dwelling
n Operationn continuous, intermittentn single, multiple
n Structuren heavy, light n new, reconstruction
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Heating system design Functional requirements
n Connection of the heat emitters with the heat source
n Deaerationn Drainingn Integration into the building
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Design parameters of hot water heating systems
n (1) Water circulationn (2) Geometry of the systemn (3) Water temperaturen (4) Expansion vessel n (5) Materials
44Michal Kabrhel125BEE1_2008/2009
Water circulation
n Natural – without pumpP1=h.ρ1 .g
P2=h.ρ2.g
ΔPF=ΔPn + ΔPP
n Forced – with pump
ΔPn=P2-P1=h.(ρ2- ρ1 ).g
P1 P2
Michal Kabrhel
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Geometry of the system
n Relative connection of the heat emittersn One-pipe, two-pipe
n Main pipe lay-outn Upper, lower, combined
n Branch pipes lay-out n vertical, horizontal , microbore
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Geometry of the system Relative connection of the heat emitters
n Two-pipe systemn One-pipe system
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Two-pipe systems
n Contraflow, parallel flow
Tichelmann
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One-pipe systemsBasic schemes of the connection
•With mixing valve•Two-point•One-point
• With By-Pass–“Horse Rider“ – Controlled by-pass
•Serial
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One-pipe systemsMixing valves
Two-point valves
One-point valves
Ventil compact
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Relative connection of the heat emitters
Conclusion
Two-pipe X one-pipe system
n Length of the pipesn Water circulationn Measuring and controln Pressures in the system
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Geometry of the systemMain-pipe layout
Upper
Lower
Combined
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Branch pipes layout
Vertical
Horizontal
Microbore
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Temperature Operational temperature
n Design temperature
t2
t1
tw1
tw2
tTp,max
tw
Temperature difference - emitter = tw1 - tw2
Temperature difference system = t1 - t2
System supply t1
System return t2
Emitter supply tw1
Emitter return tw2
Maximal emitter surface temperature tTp max
Mean emitter temperature tw
54Michal Kabrhel125BEE1_2008/2009 Michal Kabrhel
Temperature in the system
n Heat transferred by the system
n Heat transferred by the emitter
t2
t1
tw1
tw2
tp1,max
tw
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Temperatures Design Criterions
• Economical criterions
• Physical properties of the medium
• Hygiene requirements
• Technical properties of the heat source
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TemperatureParameters design
n Heating system supply temperature• Low- temperature t1 <=65°C• Medium - temperature 65°C< t1 <= 115°C• High temperature t1 > 115°C
n Temperature difference n 10K - 25K, high temperature 40K - 50K. n 90/70 °C, 80/60°C, 75/55°C, 55/45°C
57Michal Kabrhel125BEE1_2008/2009 Michal Kabrhel
Temperature Parameters Design
n Emitter n Maximal surface temperature (85 - 90°C)
n Temperature differencen Two-pipe = system temperature difference (15 - 25
K) n one-pipe < system temperature difference OS (5 -
10 K)
58Michal Kabrhel125BEE1_2008/2009 Michal Kabrhel
Piping materials
n The material should be selected at the beginning of the design process
n Used materialsn steeln coppern plastic
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Piping materialsSteel
n Traditional materialn Welding, flanges
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Piping materialCopper
n Lower material usagen Chemical reaction with water pH min7n Electrochemical corrosion (Al)n soldering , torch brazing
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Piping materialPlastic
• Materials• Netted polyethylene (PEX, VPE),• polybuten (polybutylen, polybuten-1,PB),• polypropylen (PP-R, PP-RC,PP-3),• Chlorided PVC (C-PVC, PVC-C)• Multilayer pipes with metal
n Life-cycle !!!n Oxygen barierre ?
62Michal Kabrhel
Heating systemhydraulic calculation
Heating systemhydraulic calculation
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Calculation
n Temp difference setupn Transferred outputn Circulation moden Hydraulic scheme,
sections, circuitsn Water flow rate
64Michal Kabrhel
Design of the pipe diameter
n Forced circulationn method economical specific pressure loss
60 - 200 Pa.m-1
n method optimal velocityn 0,05 - 1,0 m.s-1 (!!! Noise)
– method given pressure differencen buoyancy + pump headn 10-70 kPa
n Natural circulation– method given pressure difference
n buoyancy
65Michal Kabrhel
Pressure loss calculationn Pressure lossn frictionn local resistance
n Pressure loss of the circuit compare with the pump head
nPressure excess is reduced by the control valves
nPressure lack – must be changed the pump or redesigned the system
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n boiler plantsn combustion process in the
boilers
n heat-exchanger plantsn district heating
n renewable sourcesn utilization of solar, wind,
geothermal energy, co-generation, heat pumps
Heat sources
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Boiler plants classificationn Fuel
n solid, gas, liquid
n Burnern atmosphericn pressurized
n Operating temperature
n steam n hot watern low temperature -
condensing boilers
Czech Technical University in PragueFaculty of Civil Engineering
Department of Microenvironmental and Building Services Engineering
Michal Kabrhel 682008/2009 68
District heating
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Boiler plants classificationn Output
n I.category n >3500 kW
n II.categoryn >500 <3500 kW
n III.categoryn >50 <500 kW
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Boiler rooms function
n Fuel supplyn solid, liquid, gas (natural x propane)
n Heat distributionn heatingn hot water generationn air-condition heatern technology
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n Safety devicesn Expansion vessel, pressure relief valves
n Control of the boiler outputn Electronic control
n Requirements to the building constructionn Supports of the piping, foundation below heavy
elements (hw tanks, boiler)
n Operation
Boiler rooms function
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Boiler rooms function
n Air supplyn combustionn ventilationn heat gains removal
n Air outletn ventilationn heat gains removal
n Waste gases removaln atmosphericn pressurizedn “turbo” boilers
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District heating
n Heat sourcen Distribution networkn Transfer plantn Heating system
Heat source
DistributionPrimary network
DistributionSecondary network
Transfer plant
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Distribution network
n ductn ductlessn collectorn surface
a) b) c) d)
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Heat exchangersn Tubular n U-tubesn Kit
n Platen sealed and screwedn soldered
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Heat transfer plantn Pressure dependent, water-water
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Heat transfer plantn Pressure independent - water - water
Consumer network
Heat exchager
Secondary network
manifold
Safety and expansion device
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Heat transfer plantn Pressure dependent - steam - steam
Condensate meter
Secondary network manifold
Reduction valve
Condensate tank
Repumping of the condensate
Steam trap
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Example of heat transfer plant water-water
79
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Example of transfer plant
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Electric energy - utilisation
n Direct heatingn Infra red heatersn radiatorsn Convectors, warm air
heatingn Radiant heating
n panelsn curtainsn sheetsn cables
n Warm water (electric boiler)
n Storage heatingn Off-peak storage
n staticn dynamicn hybrid
n warmwater (boiler)n Resistant cables
Appliances
Czech Technical University in PragueFaculty of Civil Engineering
Department of Microenvironmental and Building Services Engineering
Michal Kabrhel 822008/2009 82
HeatingRenewable heat sources
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Electric energy – productionSituation in CZ•70% coal 7,5 GW tj cca 51 000 ton of coal daily, •18% water 1,8 GW•17% nuclear 1,7 (2,7) GW 47,6 ton uranium anually (130 kg daily)•0,5 % other (wind, solar)
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Biomass
² wood² wood residue² straw
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Biomass sources
v Cultivation
v Waste product
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Manufactured biomass
ØBriquettes
ØPellets
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Fuel value
vWood 16 MJ/kg
v Briquettes, Pelets 19 MJ/kg
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Biomassv Renewable sourcev Local source – not related to
global politicsv Balanced production CO2 – no
greenhouse effect
• Water content – fuel value• Fuel storage• Ash• Lower operation comfort
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Biomass combustion boiler - gasification
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Scheme of gasification boiler connection
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Pellets boiler
n = gasification boiler + fuel storage + screw conveyor
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Pellets transport - pneumatic
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Pellets delivery
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Pellets transport
Michal Kabrhel 94
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Solar energyn SUN – sky move
n Difusse and direct radiation
n Solar constant 1360 W/m2
n Clouds
n Real radiation max 1000 W/m2
Global radiation ČR [MJ . m-2 .a]
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Renewable heat sourcesn Solar Energyn Passive Systems
n solar windown greenhousen accumulation wall
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Renewable heat sourcesn Solar architecturen location in the countryn building plann thermal insulationn balanced accumulation of the structuren additional heating systemn minimizing of heat gains in summer by
shading
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Renewable heat sourcesn Active solar systemsn Thermal solar systemn water, air collectors
Water solar system
• Direct• Undirect
• Natural • Forced close
Water solar system
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Renewable heat sourcesn Active solar systemsn Photovoltaics cells
Cell Panel Field
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Renewable heat sources
n Grid-onn Grid-off
Inverter Appliance
Appliance
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Renewable heat sourcesGeothermal energy - Heat pumpsn Evaporator, compressor,
condenser, reducing valven Evaporator
n air, water, soil
n Condensatorn low temperature heating, hot
water, swimming pool
n Efficiency -n Output/Input= avg.2,4
http://www.geoexchange.org/frames/case_studies.htm
Energy ofenvironment
Utilisation: heating, hot water
Compressor
Medium vapour
Compressed hot vapour
Liquid mediumCooled medium
Evaporator
Condenser
Reducing
valve
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Heat pumps - alternatives of heat sources
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Combined heat and power generation (CHP)
n gas engine with el.powergenerator
n cooling of the engine is the heat source
n output e.g. 42 kW heat 25 kW electric
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Fuel CellsIn principle, a fuel cell operates
like a battery. Unlike a battery, a fuel cell does not run down or require recharging. It will produce energy in the form of electricity and heat as long as fuel is supplied.
A fuel cell consists of two electrodes sandwiched around an electrolyte. Oxygen passes over one electrode and hydrogen over the other, generating electricity, water and heat.
n http://www.esru.strath.ac.uk/EandE/Web_sites/00-01/fuel_cells/
Michal Kabrhel
Wind energy
Wind energyn Wind+building
Geothermal energy