CAE 331/513 Building Science Fall 2013

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CAE 331/513 Building Science Fall 2013 Lecture 10: November 11, 2013 Finish cooling loads HVAC systems Energy estimation methods Advancing energy, environmental, and sustainability research within the built environment www.built-envi.com Twitter: @built_envi Dr. Brent Stephens, Ph.D. Civil, Architectural and Environmental Engineering Illinois Institute of Technology brent@iit.edu

Scheduling HW 5 graded and returned Any questions on HW 4 (IAQ) or HW 5 (heating loads)? One more HW assigned today, due next week Final exam: Monday December 2, 5-7 PM Will cover all course topics Fewer problems than mid-term Grad students Final projects and presentations due November 25 th Blog posts 1 next week, November 18: Any topic 1 the final week, November 25: Summarize your research paper 2

Grading so far Check your grades on BB and make sure they are correct Sometimes we miss HW assignments that were turned in online There is a maximum of 550 points so far 1 exam + 5 HW worth 50 points each Current distribution (not counting blog posts for grads): 15 students 90% or higher 8 students 80 to 90% 4 students 70 to 80% 3 students less than 70% 3

Last time Cooling load calculation methods CLTD/CLF Transfer functions RTS 4

Today s objectives Finish RTS cooling load example (ASHRAE HOF) Heat balance methods HVAC systems and equipment Energy estimation methods 5

Another RTSM example ASHRAE Handbook of Fundamentals RTS example Single room example, Chapter 30 in 2005 HOF 6

Software tools for load calcs These are not done by hand, sometimes by spreadsheet Many use ACCA Manual J Most use computer programs Big list of programs: http://apps1.eere.energy.gov/buildings/tools_directory/subjects.cfm/ pagename=subjects/pagename_menu=whole_building_analysis/ pagename_submenu=load_calculation 7

Last cooling load method: Heat balance method Relies on a combination of surface and air energy balances More detailed than RTS Actually used to generate the standardized profiles in RTS method Requires a computer program More time consuming than other methods Foundation of modern energy simulation programs We cover this topic in 463/524 Building Enclosure Design Will eventually have a dedicated energy simulation course also 8

Heat balance method (HBM) HBM is based on the law of conservation of energy A set of energy balance equations for an enclosed space is solved simultaneously for unknown surface and air temperatures Many fewer assumptions; more fundamental Consists of three important energy balance equations: Outside surface heat balance Inside surface heat balance Air heat balance Initiated by hourly outdoor climate conditions Design day meteorological data (or full year) 9

Heat balance method (HBM) 10

Heat balance method (HBM): Outside heat balance 11

Heat balance method (HBM): Inside heat balance 12

Heat balance method (HBM): Indoor air heat balance 13

HBM: Surface energy balance Exterior surface example: roof Once you have this equation described, you can do just about anything regarding heat transfer in building enclosure analysis, leading into full-scale energy modeling Steady-state energy balance at this exterior surface: What enters must also leave (no storage) q solar + q longwaveradiation + q convection q conduction = 0 14

HBM: Surface energy balance Exterior surface example: roof q = 0 We can use this equation to estimate indoor and outdoor surface temperatures At steady state, net energy balance is zero Because of T 4 term, often requires iteration Solar gain Surface-sky radiation Surface-air radiation Convection on external wall Conduction through wall αi solar +ε surface σ F sky (T 4 4 sky T surf ) +ε surface σ F air (T 4 4 air T surface ) +h conv (T air T surface ) U(T surface T surface,interior ) = 0 q sw,solar +q lw,surface sky +q lw,surface air +q convection q conduction = 0 15

HBM: Surface energy balance Similarly, for a vertical surface: q solar + q lwr + q conv q cond = 0 αi αi solar solar +ε surface σ F sky (T 4 4 +ε surface σ F sky (T 4 4 sky T sky T surface,ext ) ) +ε surface σ F air (T 4 4 +ε surface σ F air (T 4 4 air T air T surface,ext ) +h conv (T air T 4 +ε surface σ F ground (T surface ground ) +h conv U(T air surface T T surface,ext surface,interior ) ) = 0 U(T surface,ext T surface,int ) = 0 4 T surface,ext ) Ground 16

HBM: Combining surface energy balances For an example room like this, you would setup a system of equations where the temperature at each node (either a surface or within a material) is unknown 12 material nodes + 1 indoor air node At surface nodes: q = 0 C 1 2 3 Heat Xfer @ external surfaces: Radiation and convection At nodes inside materials: dt mc p dt = q at boundaries Based on density and heat capacity of material 1 2 L 3 Room F Convection A air node Rad iati on 3 internal surface node 2 element-inner node 1 external surface node 3 2 R 1 17

HBM: Air energy balance To get the impact on indoor air temperature (and close the system of equations) Write an energy balance on the indoor air node Air impacted directly only by convection (bulk and/or surface) (V room ρ air c p,air ) dt air,in dt n = h i A ( i T i,surf T ) air,in + mc p T out T air,in i=1 ( ) +Q HVAC In plain English: The change in indoor air temperature is equal to the sum of convection from each interior surface plus outdoor air delivery (by infiltration or dedicated outdoor air supply), plus the bulk convective heat transfer delivered by the HVAC system L 3 C 3 F 3 A air node EQ i HVAC R 3 Q infiltration 18

Using HBM to calculate peak loads 19

Using HBM to calculate peak loads 20

Energy simulation basics http://energy.concord.org/energy2d/solar-heating-convection.html 21

HVAC SYSTEMS What do they look like? 22

HVAC systems Once we know our peak heating and cooling loads, we will need to select equipment HVAC = Heating, Ventilating, and Air-Conditioning Primary systems Vapor compression systems (i.e., chillers and condenser units) Electrically driven Thermally driven Cooling towers Secondary systems Distribution systems (air and water) 23

HVAC system design options We can rely on central HVAC systems One system per building May control all zones similarly or different zones differently Depends on system type Or we can rely on distributed HVAC systems for every zone Motels, strip malls, apartment buildings Need to figure out what medium we will use for heat transfer Air, steam, water? Need to determine what capacity and efficiency we want 24

Typical central residential system 25

Typical large commercial systems: Central Heating option 1: Steam boiler AHU serves all rooms Heating option 2: Hot water boiler Cooling option 1: Air cooled chiller chilled water Cooling option 2: Cooling tower chilled water 26

Typical large commercial systems: Central Packaged central system 27

Typical large commercial systems: Central 28

Typical small commercial systems: Distributed 29

Packaged roof top units (RTU) 30

Slab installation 31

Central vs. distributed systems Central Large equipment has higher quality, efficiency, and durability Maintenance is concentrated Noise is removed from zone Diversity allows lower installed capacity Can use thermal storage Distributed Easy to provide zoning Direct control by occupants Easier independent scheduling for energy savings Generally lower capital costs and shorter lead time for equipment Don t need dedicated maintenance staff Can often install on roof (saves room in the building) 32

All air air handling systems Constant air volume (CAV) Constant zone airflow rates Meets varying loads by varying supply air temperature Variable air volume (VAV) Constant zone supply air temperature Meets varying loads by varying supply airflow rates Dual duct (DD) Mix hot and cold air at each zone Use constant or variable supply airflow rate Multizone (MZ) Mix hot and cold air for each zone at the air handler 33

Typical CAV 34

Typical VAV 35

Typical DD 36

Typical MZ 37

Air supply and diffusers Mixed versus displacement ventilation Diffuser selection 38

Air-water systems Many commercial buildings use a combination of conditioned air and zone water coils Ventilation requires air movement But zone heating and cooling loads can be met with fan coils 39

One or two coils Thermostat controls water flow Ventilation is met with conditioned or unconditioned outdoor air Fan coils 40

HVAC SYSTEMS How do they actually work? 41

Typical central residential systems How a furnace works https://www.youtube.com/watch?v=vbso23tnpue How your AC works https://www.youtube.com/watch?v=_lfula1pz8u Other parts of heating and cooling systems https://www.youtube.com/watch?v=y972runhyve Learn HVAC for commercial systems https://www.youtube.com/watch?v=fjzidb4n5vc 42

Vapor compression cycle: AC units Expansion valve Indoor 75 F Outdoor 105 F 43

Enthalpy, h [J/kg, Btu/lb] Temperature change, ΔT Thermodynamics for HVAC Δh = CpΔT only for the same phase (e.g. air or water) What if we have change of the phase? Evaporation or condensation Entropy, s [J/kgK, Btu/lb F] Δh = TΔs for evaporation or condensation 44

Vapor compression cycle: AC units High P, lower T Saturated liquid High P, high T Superheated vapor Low P, low T Saturated vapor Low P, low T Liquid + vapor mix 45

Question: What is the COP? A. Congressional Observer Publications B. California Offset Printers C. Coefficient of Performance D. Slang for a policeman COP = Provided cooling energy [W] Used electric energy [W] = η Equivalent to the efficiency of an air-conditioning unit 46

What is the efficiency of a typical residential AC unit? A. 10% B. 50% C. 80% D. 100% E. 300% For an ideal refrigeration cycle: COP = Q cool W elec = h 1 h 4 h 2 h 1 * h = Ts 47

Chillers Chillers use vapor compression or absorber system to produce chilled water for cooling spaces Air-cooled chiller Chiller Water 52 F Building Outside air 95 F Water 42 F Inside 75 F 48

Water cooled chiller Chiller Cooling tower Water 120 F Outside air 95 F Water 52 F Building Water 100 F Water 42 F Inside 75 F 49

Evaporative cooling Wet media/water spray direct Raise absolute humidity, lowers temperature of conditioned air 50

Heat pumps 1) Compressor 2) Condenser 3) Evaporator 4) Air handler 5) Reversing valve and expansion valve Air-conditioner run in reverse 51

Heat pumps Cooling Heating Outside 95 F Outside 55 F Inside 75 F Inside 75 F Air-conditioner run in reverse 52

What do we need to know about cooling systems? Equipment selection example Need 1.2 tons Of water cooling 1 ton = 12000 Btu/hr 1.2 tons = 14,400 Btu/hr Capacity is 1.35 ton only for: 115 F air condenser temp 50 F of water temperature 53

Capacity and efficiency changes with outdoor T, indoor T/RH, and airflow rates 54

Capacity and efficiency changes with outdoor T, indoor T/RH, and airflow rates 55

EER = energy efficiency ratio EER and SEER Same as COP but in weird mixed units: (Btu/hr)/W Example from previous page: COP = 8.5 [kw] 2.48 [kw] = 3.43 EER = 29.0 [kbtu/hr] 2.48 [kw] =11.7 EER = COP 3.41 SEER = seasonal energy efficiency ratio, units: [Btu/Wh] Cooling output during a typical cooling season divided by the total electric energy input during the same period Represents expected performance over a range of conditions EER 0.02 SEER 2 +1.12 SEER 56

EER and SEER AC units must be 14 SEER (or 12.2 EER) beginning on January 1, 2015 if installed in southeastern region of the US 57

Using EER to estimate energy consumption If you know the load and you know the EER, you can estimate the instantaneous electric power draw required to meet the load: P elec = Q cooling,load COP Multiply by the number of hours and sum over period of time and get energy consumption: E = P elec Δt Can break into bins if COP/EER changes with varying conditions 58

FLUID FLOWS For distribution systems 59

Fluid flows in buildings We use liquids and gases to deliver heating or cooling energy in building mechanical systems Water, refrigerants, and air We often need to understand fluid motion, pressure loses, and pressure rises by pumps and fans in order to size systems We can use the Bernoulli equation to describe fluid flows in HVAC systems Static pressure p 1 + 1 2 ρ v 2 1 1 + ρ 1 gh 1 = p 2 + 1 2 ρ v 2 2 2 + ρ 2 gh 2 + K v2 2 Velocity pressure Pressure head Friction 60

Pressure losses We often need to find the pressure drop in pipes and ducts Most flows in HVAC systems are turbulent Δp friction = f " $ # L D h % & ' " $ 1 # 2 ρv2 % ' & D h = 4A P = hydraulic diameter K = f! # " L D h $ & % In a straight pipe K = f " $ # L D h + fittings K f % ' & In a straight pipe with fittings 61

Friction factor 62

Reynolds number Reynolds number relates inertial forces to viscous forces: Kinematic viscosity ν = µ m 2 ρ =1.5 10 5 s (for air at T=25 C) Re = VL ν L = D h in a pipe or duct 63

Pressure losses and rises Return side: Negative pressure Supply side: Positive pressure Energy input into system by fan 64

Duct friction charts 65

Fan curves System curves Fan and system pressures 66

Fan and system curves: Ideal W fan = ΔP V η fan 67

Fan and system curves: Real W fan = ΔP V η fan 68

ENERGY ESTIMATION METHODS Annual heating and cooling energy requirements 69

Simple energy estimation methods Two methods: Degree-day methods (simplest) Constant equipment efficiency Bin methods Accounts for varying efficiencies or indoor conditions 70

Degree-day method The simplest method of estimating energy use is the Degree- Day Method (DDM) The DDM makes uses the concept of the degree-day (DD) to estimate energy used for heating or cooling The method is better for estimating heating requirements than cooling requirements since solar gain is essentially ignored Works best where the efficiency of the HVAC equipment is constant 71

DDM The basic idea is that the energy use of a building is directly related to the temperature difference between outdoor and indoor air Heating equipment is assumed to run when the outdoor temperature drops below the balance temperature The balance temperature is the outdoor air temperature at which the internal heat gains balance the heat loss to the outside This is less than the interior temperature set point Cooling equipment is assumed to run when the outdoor temperature is above the balance temperature The balance temperature might not be the same for heating and cooling because the interior temperature, interior heat gain, and building heat loss usually differ in summer and winter 72

Heating degree days and cooling degree days In many codes, standards, references and literature, you will see references to Heating Degree Days (HDD) or Cooling Degree Days (CDD) In particular, the main energy code, ASHRAE 90.1 makes reference to HDD and CDD throughout HDD and CDD are design-days used to estimate the energy demand for heating and cooling using the DDM 73

Calculating HDD and CDD A degree-day is the sum of the difference between the average outside temperature and a base temperature (often 65 F or 18 C) for a fixed time frame Add up the product of time and temperature difference below the reference for heating (and the product of time and temperature difference above for cooling) The most accurate estimates use minute-by-minute weather data ( Tbase Tout ) HDD = when T < T 24 h REF out REF i ( Tout Tbase) CDD = when T > T 24 h REF out REF i Units: degree-days = F-days or C-days We can convert between HDD in F to HDD in C by multiplying by 5/9 74

Selecting a base temperature HDD 65F and CDD 50F are common HDD/CDD levels that are used regularly in industry, so you might use those regardless of your true base temperature If your building has a different base temperature, then you should immediately know that your estimates using DDM will not be accurate The best base temperature is the balance point temperature where internal gains balance the heat loss to outside 75

Finding the balance point temperature We find the balance point temperature by setting the heat gain/loss of the building to zero and solving for the outside temperature Q h # $ ( UA) + V! total inf ρc p at T out = T bal, Q h + Q int = 0, so % &( T T ) in out T bal = T in Q int ( UA) + V! total inf ρc p 76

Understanding balance point temperatures T bal = T in Q int ( UA) + V! total inf ρc p As the insulation increases, T bal drops As infiltration decreases, T bal drops As internal gains increase, T bal drops As a result, most modern buildings have a T bal well below 65 F (usually closer to 55 F) 77

Balance point example A 10000 ft 3 building has an overall UA of 250 Btu/hr, an infiltration rate of 0.7 ACH, and an internal gain of 5 kbtu/hr What is its balance point temperature? 78

Balance point example A 10000 ft 3 building has an overall UA of 250 Btu/hr, an infiltration rate of 0.7 ACH, and an internal gain of 5 kbtu/hr What is its balance point temperature? V inf = ACH ( )V = 0.7 ( )10000 = 7000 ft3 hr Assume ρ 0.075 lb ft 3, C p 0.24 Btu lb F, T in = 68 F: T bal = 68 5000 250 + 7000(0.075)(.24) = 68 13.3 = 54.7 F 79

Online CDD/HDD calculators There are a number of online calculators that use TMY (typical meteorological year) data http://www.degreedays.net/ http://www.cpc.ncep.noaa.gov/products/analysis_monitoring/cdus/ degree_days/ http://pnwpest.org/cgi-bin/usmapmaker.pl 80

HDD65F maps 81

HDD 65F maps 82

CDD 65F maps 83

CDD 65F maps 84

Chicago Area HDD/CDD (Fahrenheit) HDD65 = 6280 and CDD65 = 1115 HDD60 = 5080 and CDD60 = 1740 HDD55 = 4220 and CDD55 = 2500 HDD50 = 3080 and CDD50 = 3400 HDD45 = 2280 and CDD45 = 4420 All units are in F-days 85

Estimating energy use with HDD Now that we know how to get HDD, we can calculate the heating energy, E, required to keep the building heated Using hourly values: E heating = (UA) total η [T bal T out (t)]dt when T out < T bal Where η = heating system efficiency (-) Using HDD: E heating = (UA) total η HDD *Convert HDD to degree-seconds 86

Estimating energy use with HDD Example problem 8.1 Find the annual heating bill for a house in New York under the following conditions: UA total = 205 W/K Heat gain = 569 W T in = 21.1 degrees C Heating system is 75% efficient Fuel prices is $8/GJ HDD = 2800 K-days Find balance temperature Estimate energy requirements Estimate costs 87

Estimating cooling energy use Estimates for cooling energy are not as accurate but we can still use them E cooling = (UA) total COP [T bal T out (t)]dt when T out > T bal E cooling = (UA) total COP CDD *Make sure time units align 88

Bin method The Bin Method is another variation of the degree-day method where we break down the year into temperature ranges or bins and compute the energy use in each of the bins 5 degree temperature ranges are usually used In this method, we can easily account for: Varying loads Varying heating/cooling systems Varying system efficiencies This is especially important for air-conditioner units and heat pumps where the efficiency depends greatly on the temperature at which it is working 89

Bin method We need to find the number of hours (N bin ) that the outdoor temperature (t o ) is in a temperature bin 90

Bin method 91

Annual energy consumption While these methods are good for rough estimates, it is best to perform annual energy simulations using software to get better estimates EnergyPlus equest IES-VE TRNSYS Many others 92

Next time Energy efficiency Building diagnostic methods 93