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Lecture 9 Domestic Hot Water Supply

Jul 08, 2018

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    Lecture 9. Domestic

    Hot

    Water

    Supply

    Hongwei LiCivil Engineering Department

    Building 118, room 206Technical University of Denmark

    [email protected]

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    Lecture Content

    DHW Supply

    Plate heat exchanger(PHE) Heat exchanger concept and design By‐pass control

    Pipe heat transfer calculation Storage tank Flat station

    Legenella Heat pumps

    Lecture11 DHW Supply

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    DHW supply

    Lecture11 DHW Supply

    Fig. 1 DHW supply with reciruclation

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    DHW

    supply

    ComfortDanish regulation: 10 seconds waiting time, supply at 45oC for kitchen and 40oC for shower and

    hand wash Hygiene: LegionellaEHP requires the minimum DHW tempearture at 50oC, and never fall below 55oC for storagetank or DHW with recirculationGerman guideline: a DHW system with total volume less than 3 L allows temperature lowerthan 50oC without risk of Legionella (3 liters not includes HE)

    Energy efficiencyWell insulated pipe, avoid recirculation

    Low costoverall cost reduction both in ‐house substaiton and in network

    Lecture 9 DHW Supply

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    DHW load

    profile

    Lecture 9 DHW Supply

    0

    2

    4

    6

    8

    10

    12

    14

    16

    0 5 10 15 20 25 30 35 40 45 50 55 60 65

    l / m

    min

    Flow rate ShowerKitchen

    0

    5

    10

    15

    20

    25

    30

    35

    0 5 10 15 20 25 30 35 40 45 50 55 60 65

    k W

    min

    Power Shower

    Kitchen

    Bath tub Shower Kitchen wash Hand wash

    Cold water temperature [oC] 10 10 10 10

    Temperature at tapping [oC] 40 40 45 40

    Required power [kW] 26.4 17.6 14.7 7.0

    Norminal flow rate [l/min] 12.57 8.38 6.00 3.33

    Duration of draw-off [s] 600 300 150 180

    Volume of tapped water [l] 126 42 15 10

    Total number of tapping 2 4 2 4

    Delay between each tapping [min] 30 20 20 20

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    Energy demand

    for

    DHW

    Energy for taping requirement

    i is the i th unit. T s,i is the i th unit DHW supply temperature. V i,day is volume flow rate of i th unit m3 /day, n and V i,day depends on the type of buildings and activities, Q has the unit MJ/day

    Heat loss along distribution pipe:

    Lecture 9 DHW Supply

    L

    l

    e f d u ploss dlT lT U T T cmQ0

    )(182.4 ,1

    , cis

    n

    i

    dayitapping T T V Q

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    Factors affect time

    delay

    Lecture 9 DHW Supply

    q

    Ld t i

    4

    2

    Factors for time delay due to service pipe and heat exchanger(i) Service pipe diameter, length, thermal capacity and re ‐circulation.

    (ii) HE volume, primary flow rate, thermal capacity of HE and the setting of thermal by ‐pass (without by ‐pass, external by ‐pass, and internal by ‐pass).

    Transprtation delay (simplest condition)

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    DHW Distribution Systems in Small Buildings

    Anti ‐Legionella equipment in large buildings

    DHW system

    design

    No DHW recirculation Reduce transportation time Reduce total volume

    Lecture 13 Domestc hot water supply

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    ITHE in

    LTDH

    Lecture11 DHW Supply

    1. DH supply 2. DH return 3. SH return 4. SH supply

    5. DHW return 6. DHW supply 7. Heat exchanger 8. By‐pass thermostatic valve 9. Thermostatic controller

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    Recommended Design

    Parameters

    (EHP)

    Lecture11 DHW Supply

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    Plate heat exchanger in

    LTDH

    Lecture11 DHW Supply

    For lower temperature difference Improved flow pattern

    Enlarged surface area and increased heat transfer (10%) Improved control

    Low pressere drop

    T11=50oC, T12

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    Plate heat exchanger (PHE)

    Lecture11 DHW Supply

    Thin and rectangular metallic sheet with corrugated surface.

    Two fluids alternatively passes through the plate surface and exchanges heat.

    Numbers of plate depend on required thermal ouput Corrugated surface increaes effective surface area, distrupting boundary layer, creates turbulent

    mixing and decrease fouling resistance, thus enhance the heat transfer.

    Large heat transfer surface, fast temperature change, and compact size.

    PHE is more efficient to cool DH water than stroage tank

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    Gasketed Plate heat exchanger (PHE)

    Lecture11 DHW Supply

    Gasketed plate heat exchanger

    Gasketed PHE:are made of two end plates and of form ‐pressed plates with gaskets, tightened between the end plates.

    use sealing gasket to prevent intermixingof media and leakage to outside.

    Capable for high temperature, easy to clean and maintain, plates can take apartfor expansion or contraction

    Start, left ‐hand, right ‐hand, and end plate

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    Brazed PHE

    Lecture11 DHW Supply

    The units are connected together not through the use of endplates and gaskets. Instead, all corrugated plate are brazed together at hightemperature.

    1.Reliability, lightweight, large capacity

    2.Low internal water volume. Need fast regulatingsystem to reach desired temperature within short

    timeTwo media flow through alternate channels,

    always in opposite directions (counter current flow).

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    Flow arrangement

    in

    PHE

    Lecture11 DHW Supply

    U and Z type port connection. The flow pass the same distance in the Z type connection

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    Temperature distribution

    in

    PHE

    Lecture11 DHW Supply

    Parallel flow PHECounter flow PHE

    In a condenser

    In an evaporator

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    PHE heat

    transfer

    analysis

    Lecture11 DHW Supply

    Overall energy balance in hot/cold fluid

    micoc pcohih ph T UAT T cmT T cmQ

    )()( ,,,,

    )ln()ln(2

    1

    21

    1

    2

    12

    T T

    T T

    T T

    T T T m

    Log mean temperature difference (LMTD)

    For parallel flow For counter flow

    ocoh

    icih

    T T T

    T T T

    ,,2

    ,,1

    icoh

    ocih

    T T T

    T T T

    ,,2

    ,,1

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    PHE heat

    transfer

    analysis

    Lecture11 DHW Supply

    hh and hc are heat transfer coefficient of hot and cold stream, p is plate thickness, k

    p is thermal conduction of plate material, R

    f,h and

    R f,c are fouling resistance on hot and cold side. It is an approximation as U vary along with plate.

    Overall heat transfer coefficient U

    c f h f p

    p

    ch

    R Rk hhU ,,

    111

    for the same U and inlet/outlet temperature, the meantemperature difference is smaller for parallel flow than for counter flow, thus the required surface area is smaller than parallel flow

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    ‐NTU

    method

    Lecture11 DHW Supply

    Two types of analysis: Performance calculation (determine heat transfer rate): with known flow rate, inlet/outlet temperature, U and A

    Design calculation (determine heat transfer area):

    1. With knowing Tm, use LMTD method

    2. Without knowing Tm, use ‐NTU method (only inlet temperatures are known). : Heat exchanger effectiveness

    NTU: the number of heat transfer unit (thermal length)

    Maximum possible heat transfer rate • It can be achieved in a counter flow HE with infinite length• with maximum temperature difference in HE: Thi‐Tci

    If C c

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    ‐NTU method

    Lecture11 DHW Supply

    Heat exchanger effectiveness e (ratio between actual HT rate to maximum possible HT rate )

    )(

    )(

    )(

    )(

    ,,min

    ,,

    ,,min

    ,,

    max icih

    icocc

    icih

    ohihh

    T T C

    T T C

    T T C

    T T C

    qq

    )( ,,min icih T T C q thus

    NTU is the number of heat transfer unit (thermal length):

    ),,( ement flowarrang R NTU f

    minC

    UA NTU

    max

    min

    C C

    R

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    ‐NTU method

    Lecture11 DHW Supply

    Parallel flow PHE:

    Counter flow PHE:

    R

    NTU R

    1)1(exp1

    NTU R R NTU R )1(exp.1 )1(exp1

    When C h or C c tend to be infinite as in evaporator or condenser, R=0, e becomes independent of flow direction

    NTU exp1

    Parallel (top) and counter (bottom) PHE

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    Example

    Lecture11 DHW Supply

    An instantaneous heat exchanger is used to heat up the cold water to the desired DHW supply temperature. The overall heat transfer coefficient for the PHE is 4000 W/m 2.oC. The primary side water inlet temperature is 60oC, with flow rate 15 L/m. The secondary water inlet temperature is 10 oC, with flow rate as 11 L/m. To get the desired secondary water outlet temperature as 55 oC. 1) what will be the heat transfer area for the PHE? 2). What will be the primary return temperature?

    NTU method

    As =765 W/ oC

    , , =3.8 E4 W

    , , =3.4 E4 W

    The effectiveness is

    0.9 0.73

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    Example

    Lecture11 DHW Supply

    The NTU can be found from the figure as

    4.6

    Thus 0.88 2

    8.9

    )ln( )

    10275560

    ln(

    )1027()5560(

    1

    2

    12

    T T

    T T T m

    LMTD

    W E T UA m 44.3

    Thus 0.87 2

    isos pso pi p p p T T cmT T cmq ,,,,

    Thus ,

    27

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    Thermal by ‐pass

    Lecture11 DHW Supply

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    Without by‐pass: water cool down

    Initial water temperature is 50oC and insulation is 15oC

    Test between 0 ‐720 min. Three ground tempeature 3, 8, 14 From 50oC to 20oC requires 3 and 4

    hours for ground temperature at 8 and 14.

    At ground 14oC, 1.0 hours to cool down from 50 to 35oC.

    Lecture11 DHW Supply

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    Without by‐pass: transport delay

    Transport delay due to thermal capacity.

    Temperature at outlet of service pipe

    (inlet of HE) Aluflex 20/20/110 , 10 m long Ground temeprature 8oC Different initial temperature and flow

    rates.

    For Ti=20oC,

    17.3

    l/min:

    6.1

    s inlet

    hot

    water (50oC) reach the outlet, but cooled to 39oC due to pipe thermal capacity, need additional 2 s to reach 45oC.

    For Ti=35oC, 17.3l/min: 7 s to reach

    45oC

    Lecture11 DHW Supply

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    1‐D pipe heat loss

    Lecture11 DHW Supply

    r 1, h f

    h ar 2, k 2

    0)(1

    dr dT

    kr dr d

    r

    1‐D pipe temperature distribution

    Heat transfer across the cylinder

    dr dT

    rLk q r )2(

    T f

    T aT s,1

    T s,2 T s,3T s,4

    T f

    T s,1 T s,3 T s,4 T a

    f hr 121 2

    12

    2)/ln(

    k

    r r

    ahr 421 3

    23

    2)/ln(

    k

    r r

    T s,2

    4

    34

    2)/ln(

    k

    r r

    a f a f

    r T T U R R R R R

    T T q

    54321

    R2R1 R3 R4 R5

    [W/m]

    a f hr k r r

    k r r

    k r r

    hr

    U

    44

    34

    3

    23

    2

    12

    1

    1)/ln()/ln()/ln(12

    [W/m.K]

    R: [K.m/W]

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    Example 1 ‐D pipe heat loss

    Lecture11 DHW Supply

    Calculate pipe line heat transfer coefficient based on the properties given in the table. Pipe is made of PEX, casing is HDPE and insulation is PUR foam

    Terms Values

    Pipe outer diameter [mm] 20

    Pipe wall thickness [mm] 2

    Casing outer diameter [mm] 80

    Casing thickness [mm] 2.5Thermal conductivity of PEX [W/m.K] 0.38

    Thermal conductivity of PUR[W/m.K] 0.023

    Thermal conductivity of HDPE [W/m.K]

    0.43

    Water flow velocity [m/s] 2

    Water temperature [oC] 47

    Air temperature [oC] 20

    Pipe length [m] 5

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    Internal flow heat transfer coefficient

    Lecture11 DHW Supply

    For turbulent flow

    Determine flow status

    6932465771000/20*2*1000

    Re E Du m

    Flow is in turbulent region

    7.29177.369324*023.0Pr Re023.0 4.08.05/4 n D D Nu

    4.93302.064.0

    *7.291 Dk

    Nuh D

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    External flow heat transfer coefficient

    Lecture11 DHW Supply

    External heat transfer coefficient is calculated based on natural convection:

    Assume pipe surface tempeature is 40oC to start calculation,

    resulting average temperature as 30oC (for thermal properties)

    13933694.22*619.16

    02.0)2040()30273/(8.9)( 33

    E E

    DT T g Ra as D

    RaD is Rayleigh number in free convection, is vometric thermal expansion coefficient, v is kinematic viscosity, a is thermal diffusivity. Air properties are evaluated at average temperature

    )(1K T a

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    External flow heat transfer coefficient

    Lecture11 DHW Supply

    Calculate heat resistance

    2

    27/816/9

    6/1

    Pr)/559.0(1

    387.06.0 D D

    Ra Nu

    27.6

    )706.0/559.0(1

    13933*387.06.0

    3200265.0

    2

    27/816/9

    6/1

    e Nu

    Dk

    h D

    R1=0.84; R2=3.68; R3=361; R4=0.94; R5=25.

    mW R R R R R

    T T U q a f r /06898.0)2047(

    54321

    Calculate back to the surface temperature. It is an iteration process

    s f r T T U q ' 7.21)(06898.047 4321' R R R RU q

    T T r f s

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    Simplifcation

    Lecture11 DHW Supply

    ahr k

    r r U

    43

    23 1)/ln(2

    R1 ,R2 and R4 are orders of magnitude lower than R 3 and R5. Thus expression of U can be simplified as (k 3> ha ). The difference is only 1.4%

    mW R R

    T T U q a f r /06996.0)2047(

    53

    a f hr k

    r r

    k

    r r

    k

    r r

    hr

    U

    44

    34

    3

    23

    2

    12

    1

    1)/ln()/ln()/ln(12

    mW R R R R R

    T T U q a f r /06898.0)2047(

    54321

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    Flat station

    Lecture 8 DHW Supply

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    Flat station

    Lecture 8 DHW Supply

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    Legionella

    Lecture 9 DHW Supply

    A fatal disease named as Legionellapneumophila.

    First discovered in 1976, USA, due to a

    outbreak of pneumonia caused 34 death. Infected by inhaling legionella bacteria

    through aerosols (tiny water droplet), or droplet nuclei contaminated with Legionella, or with ingestion of contaminated water

    Legionella proliferation/death rate vs. temperature

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    Chemical treatment

    Thermal treatment Member

    filtration

    UV sterilization

    Lecture 8 DHW Supply

    Legionella treatment

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    Heat pump

    Lecture 13 Domestc hot water supply

    Condenser

    Evaporator

    Expansionvalve

    Compressor

    House heatingdemand

    Coldenvironment

    , /

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    Heat pump as thermal booster

    Lecture 13 Domestc hot water supply

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    Lecture 13 Domestc hot water supply

    Twin Pipe Triple Pipe

    Heat Pump COP 3.3 3.3

    System COP 5.7 10.2

    Heat pump as thermal booster

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    End of lecture

    Lecture11 DHW Supply