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Towards Prediction of Artificial Monolayer Performance for Water Conservation

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Warm surface film thermally stable, no eddies increase RL. IMPACT OF MICROMETEOROLOGY ON RESISTANCE TO EVAPORATIVE LOSS Liquid thermal boundary layer ... – PowerPoint PPT presentation

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Title: Towards Prediction of Artificial Monolayer Performance for Water Conservation


1
Towards Prediction of Artificial Monolayer
Performance for Water Conservation
  • Pam Pittaway Nigel Hancock
  • National Centre for Engineering in Agriculture
  • University of Southern Queensland, Toowoomba.

2
ARTIFICIAL MONOLAYER TECHNOLOGY
  • Potential for cost-effective water saving BUT
  • Averaged daily data indicates highly variable
    performance.

THIS PRESENTATION
  • Understand the cause of highly variable
    performance to predict optimal conditions for
    cost-effective monolayer application.

3
ARTIFICIAL MONOLAYER TECHNOLOGY IN PRACTICE
4
VARIATION IN MONOLAYER FIELD TRIAL PERFORMANCE
(Craig et al 2005)
Location Storage size (km2) Trial monitoring period (days) Evaporation Reduction ()
University of Southern Queensland, Toowoomba, Qld 0.0001 1- 6 days 2- 8 days 3- 6 days 4- 7 days 5- 7 days 38 17 10 38 40
Capella Qld 0.042 1- 9 days 2- 8 days 3- 7 days 4- 8 days 0 0 0 0
Cubby Station, Dirranbandi, Qld 1.2 1- 5 days 2- 10 days 3- 8 days 31 27 0
5
ARTIFICIAL MONOLAYERS FOR EVAPORATION REDUCTION
  • Monomolecular fatty alcohol films compressing at
    water surface to retard evaporative loss
  • Long-chain, saturated fatty alcohols form
    continuous condensed film
  • Condensed film retards molecular transfer across
    liquid thermal and gaseous boundary layers
  • Wind speeds gt6 m sec-1 disrupt films

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8
  1. IMPACT OF ARTIFICIAL MONOLAYER AT MONO-MOLECULAR
    SCALE

(Figure 7.1 Davies and Rideal 1963)
GAS PHASE
Liquid thermal boundary layer (LTBL)
  • Damping capillary waves reduces wind shear RG
    reduced and eddies (Rayleigh-Benard convection)
    RL reduced.

A condensed monolayer increases RG , RI RL
9
  1. IMPACT OF MICROMETEOROLOGY ON RESISTANCE TO
    EVAPORATIVE LOSS

(Figure 7.1 Davies and Rideal 1963)
GAS PHASE
Liquid thermal boundary layer (LTBL)
  • Cold surface film thermally unstable, strong
    eddies reduce RL.
  • Warm surface film thermally stable, no eddies
    increase RL.

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11
  1. METEOROLOGICAL DRIVERS AT THE MICRO SCALE

If ?a ?wgt 0 induces a cold surface film
(?0?wlt0), small RL induces evap
loss. Increasing wind speed to 1.5 m sec-1
increases the cold surface film, reducing RG
RL, increasing evap loss.
Fig 2.5, Gladyshev (2002)
12
METEOROLOGICAL DRIVERS AT THE MICRO SCALE
concluded
  • Airsubsurface water (?a ?w) is a surrogate of
    QH
  • Surfacesubsurface water (?0 ?w) is a surrogate
    of Liquid Thermal Boundary Layer resistance
  • (?0 ?w) lt0 cold surface film (thin LTBL, lt
    RL)
  • (?0 ?w) gt0 warm surface film (thick LTBL, gt
    RL)

13
TRIALS IMPACT OF PHYSICAL COVERS ON
MICROMETEOROLOGY RESISTANCE TO EVAPORATIVE LOSS
Trial 1 black Atarsan cover on x2 tanks,
monolayer on x1 tank
Trial 2 white shade cloth cover on x2 tanks,
monolayer on x1 tank
14
INSTRUMENTATION ABOVE AND UNDER PHYSICAL COVERS
NOT TO SCALE
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16
DIURNAL ENERGY BALANCE FOR SHALLOW WATER (Fig
3.15 Oke 1987)
Shallow water Japan (QG is soil heat flux)
17
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18
(?0 ?w)
(?0 ?w)
(?a ?w)
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21
CONCLUSIONS
  • Monomolecular films increase R in liquid thermal
    (RL) gaseous (RG) boundary layers
  • Calm conditions with thermally stable LTBL (warm
    surface film),
  • RL gt Rmonolayer (no effect)
  • Light wind, thermally unstable LTBL,
  • RL lt Rmonolayer (water savings)
  • Hourly analysis is ESSENTIAL to interpret R and
    drivers of evaporation (QH, QE, Q)

22
THANK YOU
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