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Field experiment of green roor and common roof

Dalam dokumen Welcome from the Conference 2 Contents 3 (Halaman 155-159)

Abstract

6. Acknowledgements

2.1 Field experiment of green roor and common roof

As is illustrated in Fig.1, there were two test rooms using the same building materials located at Jiading Campus of Tongji University, the dimensions were both 3m*3m*2.7m. The left roof was extensive green roof, and the right one was just common roof that was made of foam sandwich panel (75mm thick). Extensive green roof was made up of foam sandwich panel and 36 prefabri- cated greenery modules which was connected by buckles, and the size of every module was 50cm*50cm*7cm (not including the canopy layer). The greenery module was well designed, which combined plant layer, substrate layer, filtering membrane and drainage layer together (Fig.2). The plant was sedum linear, a type of succulent vegetation, which is very common in Shanghai district.

The substrate was about 4cm thick and was comprised of peat soil, powdered perlite, vermiculite aggregate and organic fertilizer. During the experiment, the windows and door were locked, and indoor temperature was controlled by air conditioner at 26℃ in summer and 24℃ in winter. A weather station was installed near the roof to record the local meteorological data, including air temperature, relative humidity, solar radiation, wind speed and precipitation. Type-T thermocou- ples were set at different heights along the vertical direction of green roof and common roof, measuring temperatures of different layers. For green roof, 28 thermocouples measured tempera- ture of seven positions, including indoor air, inner and outer surface of sandwich panel layer, drainage layer, substrate layer, canopy layer and local air temperature 15cm above vegetation.

And for common roof, 16 thermocouples measured temperatures of four positions, including in- door air, inner and outer surface of sandwich panel, air temperature 15cm above the panel. All the thermocouple were connected to a data acquisitions system which scanned all sensors every one minute and stored the data in a local computer. Four TDR (Time Domain Reflectometry) sensors were used to measure volumetric water content of substrate layer, and four humidity sensors were set above the roofs to record local relative humidity. Furthermore, six heat flux sensors were in- stalled at the inner surface of sandwich panel to measure heat flux through both roofs. And these sensors were put near the center of the roof to avoid edge effect.

Figure 1 Schematic of experimental setup Figure 2 Structure view of greenery module 2.2 Numerical model of green roof

Adopting various simplifications, researchers proposed different models of green roof system.

From the simpliest thermal resistance model to heat and moisture balance model, more and more physical phenomena were considered. And this paper takes another three factors into green roof model based on SVAT1 theory proposed by Shuttleworth (Shuttleworth, et al., 1990): (1) Multiple solar reflection was considered between different layers of plant; (2) the effect of wind profile on turbulent transfer coefficients below and above canopy surface was considered; (3) Coupled heat and mositure transfer was applied in substrage layer based on the theory of Philip & de Vries (Philip and De Vries, 1957). As is illustrated in Fig.3, the following assumptions are used based on previous study (D.J. Sailor, 2008; E.P.D. Barrio, 1998): (1) Green roof is divided into three big layers, including plant layer, substrate layer and structure layer, and its area is large enough to be assumed horizontally homogeneous. (2) The biochemical reactions and heat conduction through plantsare ignored. (3) The change of substrate water content equals to the water loss through evapotranspiration, and plant's water loss is not considered. (4) The canopy is considered as a semi-transparent medium, in which radiation obeys Beer's law. (5) The structure layer is water- proof, where moisture transfer is not involved.

Figure 3 Schematic of heat and moisture transfer of green roof system 2.2.1 Longwave radiaiton distribution

In longwave range, transmittance and reflectance of the leaf tissure are negligible. The canopy will transmit only the radiation which is not even once intercepted by a leaf. In this paper, plant layer of green roof system is divided into n parts, and the longwave transmitance of plant layer can be calculated by the following equation:

𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐

= exp⁑(βˆ’π‘˜π‘˜

𝐿𝐿𝐿𝐿

βˆ™ LAI) (1)

Where, π‘˜π‘˜πΏπΏπΏπΏ is the extinction coefficient for longwave radiation, some values of it are supplied in literatures. LAI is leaf area index of plant layer.

And longwave radiation that each part receives can be derived as follows:

𝑅𝑅

𝑙𝑙,𝑓𝑓𝑓𝑓

= 𝐹𝐹

𝑓𝑓𝑖𝑖

βˆ™ πœ€πœ€

𝑓𝑓

πœ€πœ€

𝑖𝑖

𝜎𝜎(𝑇𝑇

𝑝𝑝,𝑖𝑖4

βˆ’ 𝑇𝑇

𝑝𝑝,𝑓𝑓4

) + 𝐹𝐹

𝑓𝑓𝑖𝑖

βˆ™ πœ€πœ€

𝑓𝑓

πœ€πœ€

𝑖𝑖

𝜎𝜎(𝑇𝑇

𝑖𝑖4

βˆ’ 𝑇𝑇

𝑝𝑝,𝑓𝑓4

) + 𝐹𝐹

𝑓𝑓𝑖𝑖𝑖𝑖𝑖𝑖

βˆ™ πœ€πœ€

𝑓𝑓

(𝐼𝐼

𝑖𝑖𝑖𝑖𝑖𝑖

βˆ’ πœŽπœŽπ‘‡π‘‡

𝑝𝑝,𝑓𝑓4

)⁑⁑⁑⁑⁑⁑ (2)

where, 𝑅𝑅𝑙𝑙,𝑓𝑓𝑓𝑓 is longwave radiation of each part of plant layer, 𝐹𝐹𝑓𝑓𝑖𝑖is radiation view factor, Ξ΅ is longwaver radiation absorption coefficient, 𝑇𝑇𝑖𝑖 and 𝑇𝑇𝑝𝑝 are ground surface temperature and leaf temperature of each layer.

When j<i,

𝐹𝐹

𝑓𝑓𝑖𝑖

= (1 βˆ’ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑓𝑓

) βˆ™ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,π‘“π‘“βˆ’1

βˆ™ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,π‘“π‘“βˆ’2

β‹― 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑖𝑖+1

βˆ™ (1 βˆ’ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑖𝑖

)⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (3)

When j>i,

𝐹𝐹

𝑓𝑓𝑖𝑖

= (1 βˆ’ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑓𝑓

) βˆ™ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑓𝑓+1

βˆ™ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑓𝑓+2

β‹― 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,π‘–π‘–βˆ’1

βˆ™ (1 βˆ’ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑖𝑖

)⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑(4) 𝐹𝐹

𝑓𝑓𝑖𝑖

= (1 βˆ’ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑓𝑓

) βˆ™ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑓𝑓+1

βˆ™ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑓𝑓+2

β‹― 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,nβˆ’1

βˆ™ (1 βˆ’ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,n

)⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (5) 𝐹𝐹

𝑓𝑓𝑖𝑖𝑖𝑖𝑖𝑖

= (1 βˆ’ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,𝑓𝑓

) βˆ™ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,π‘“π‘“βˆ’1

βˆ™ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,π‘“π‘“βˆ’2

β‹― 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,2

βˆ™ (1 βˆ’ 𝜏𝜏

𝐿𝐿𝐿𝐿,𝑐𝑐,1

)⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (6)

2.2.2 Solar radiation distribution

Absorptivity, reflectivity and transmissivity of each part of plant layer is defined as following equa- tions:

𝛼𝛼

𝑆𝑆𝐿𝐿,𝑐𝑐

= 1 βˆ’ 𝜌𝜌

𝑆𝑆𝐿𝐿,𝑐𝑐

βˆ’ 𝜏𝜏

𝑆𝑆𝐿𝐿,𝑐𝑐

⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (7) 𝜌𝜌

𝑆𝑆𝐿𝐿,𝑐𝑐

= (1 βˆ’ 𝜏𝜏

𝑆𝑆𝐿𝐿,𝑐𝑐

) βˆ™ 𝜌𝜌

𝑆𝑆𝐿𝐿,𝑝𝑝

(8)

𝜏𝜏

𝑆𝑆𝐿𝐿,𝑐𝑐

= 𝑒𝑒𝑒𝑒𝑒𝑒⁑(βˆ’π‘˜π‘˜

𝑆𝑆𝐿𝐿

βˆ™ 𝐿𝐿

𝑐𝑐

πœ‚πœ‚

𝐿𝐿𝐿𝐿𝐿𝐿

) (9) π‘˜π‘˜

𝑆𝑆𝐿𝐿

= [(1 βˆ’ 𝜏𝜏

𝑆𝑆𝐿𝐿,𝑝𝑝

)

2

βˆ’ 𝜌𝜌

𝑆𝑆𝐿𝐿,𝑝𝑝2

]

1/2

βˆ™ π‘˜π‘˜

𝐿𝐿𝐿𝐿

⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (10)

Where, π‘˜π‘˜π‘†π‘†πΏπΏis the extinction coefficient for solar radiation,πœπœπ‘†π‘†πΏπΏ,𝑝𝑝 and πœŒπœŒπ‘†π‘†πΏπΏ,𝑝𝑝 are transmittance and reflectance of the leaf tissue respectively.

After multiple reflection, absorption and transmittance, the total absorptivity can be derived as follows:

𝛼𝛼

1Μ…2⋯𝑛𝑛

= 𝛼𝛼

1

(1 +

1βˆ’πœŒπœŒπœπœ1𝜌𝜌23⋯𝑛𝑛

1𝜌𝜌23⋯𝑛𝑛

)⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (11) ⁑⁑⁑⁑⁑⁑⁑⁑⁑

𝛼𝛼

12⋯𝑖𝑖̅⋯𝑖𝑖

= 𝛼𝛼

12⋯𝑖𝑖⋯𝑛𝑛̅̅̅̅̅̅

βˆ’ 𝛼𝛼

12⋯𝑖𝑖+1⋯𝑛𝑛̅̅̅̅̅̅̅̅̅̅

⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (12) 𝛼𝛼

12⋯𝑗𝑗̅

=

1βˆ’πœŒπœŒπœπœ12β‹―π‘—π‘—βˆ’1𝛼𝛼𝑗𝑗

π‘—π‘—βˆ’1β‹―21πœŒπœŒπ‘—π‘—

⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (13)

Where,

𝜏𝜏

12⋯𝑖𝑖

=

1βˆ’πœŒπœŒπœπœ12β‹―π‘—π‘—βˆ’1πœπœπ‘—π‘—

π‘—π‘—βˆ’1β‹―21πœŒπœŒπ‘—π‘—

⁑⁑ (14)

𝜌𝜌

𝑖𝑖⋯21

= 𝜌𝜌

𝑖𝑖

+

1βˆ’πœŒπœŒπœπœπ‘—π‘—2πœŒπœŒπ‘—π‘—βˆ’1β‹―21

π‘—π‘—πœŒπœŒπ‘—π‘—βˆ’1β‹―21

⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (15)

𝛼𝛼

12⋯𝑖𝑖⋯𝑗𝑗̅̅̅̅̅

=

1βˆ’πœŒπœŒπœπœ12β‹―π‘–π‘–βˆ’1𝛼𝛼𝑖𝑖⋯𝑗𝑗

π‘–π‘–βˆ’1β‹―21πœŒπœŒπ‘–π‘–β‹―π‘—π‘—

⁑⁑⁑⁑⁑⁑⁑ (16)

𝛼𝛼

𝑓𝑓⋯𝑖𝑖

= 1 βˆ’ 𝜏𝜏

𝑓𝑓⋯𝑖𝑖

βˆ’ 𝜌𝜌

𝑓𝑓⋯𝑖𝑖

⁑⁑⁑⁑

(17)

Then solar radiation of each part of plant layer can be calculated by multiplying incident solar radiation above green roof by total absorptivity𝛼𝛼12⋯𝑖𝑖̅⋯𝑖𝑖:

𝑅𝑅

𝑖𝑖,𝑓𝑓𝑓𝑓

= 𝛼𝛼

12⋯𝑖𝑖̅⋯𝑖𝑖

Γ— 𝑅𝑅

𝑓𝑓𝑛𝑛

⁑

(18)

2.2.3 Energy balance of plant layer

(𝜌𝜌𝐢𝐢

𝑝𝑝

)

𝑓𝑓

𝑑𝑑

𝑓𝑓

𝐿𝐿𝐿𝐿𝐿𝐿

𝑖𝑖𝑑𝑑𝑑𝑑𝑑𝑑𝑑𝑑𝑓𝑓𝑓𝑓

= 𝑅𝑅

𝑠𝑠,𝑓𝑓𝑖𝑖

+ 𝑅𝑅

𝑙𝑙,𝑓𝑓𝑖𝑖

+ 𝐻𝐻

𝑓𝑓𝑖𝑖

+ 𝐸𝐸

𝑓𝑓𝑖𝑖

⁑⁑⁑⁑

(19) 𝐻𝐻

𝑓𝑓𝑖𝑖

= 2𝐿𝐿𝐿𝐿𝐿𝐿

𝑖𝑖

(𝜌𝜌𝐢𝐢

𝑝𝑝

)

π‘Žπ‘Ž(𝑑𝑑𝑓𝑓𝑓𝑓(π‘Ÿπ‘Ÿβˆ’π‘‘π‘‘π‘π‘)

𝑏𝑏)

(20) 𝐸𝐸

𝑓𝑓𝑖𝑖

= 2𝐿𝐿𝐿𝐿𝐿𝐿

𝑖𝑖(πœŒπœŒπΆπΆπ›Ύπ›Ύπ‘π‘)π‘Žπ‘Ž(𝑒𝑒(π‘Ÿπ‘Ÿπ‘“π‘“π‘“π‘“βˆ’π‘’π‘’π‘π‘)

𝑠𝑠𝑠𝑠+π‘Ÿπ‘Ÿπ‘π‘)

(21)

where (ρ𝐢𝐢𝑝𝑝)𝑓𝑓is volumetric heat capacity of plant layer, 𝑑𝑑𝑓𝑓 is leaf thickness, 𝑇𝑇𝑓𝑓𝑖𝑖 is average tempera- ture of each part of plant layer, 𝜏𝜏 is time, 𝐻𝐻𝑓𝑓𝑖𝑖 and 𝐸𝐸𝑓𝑓𝑖𝑖 are sensible heat and latent heat transfer of each part of plant layer respectively, π‘Ÿπ‘Ÿπ‘π‘ is leaf boundary layer resistance, π‘Ÿπ‘Ÿπ‘ π‘ π‘ π‘  is leaf stomatal re- sistance, 𝑇𝑇𝑐𝑐 is average temperature of canopy space.𝑒𝑒𝑓𝑓𝑖𝑖 is saturated vapor pressure of plant tem- perature, 𝑒𝑒𝑐𝑐 is vapor pressure of canopy space.𝛾𝛾 is psychometric constant.(ρ𝐢𝐢𝑝𝑝)π‘Žπ‘Ž is volumetric heat capacity of air.

2.2.4 Energy and moisture balance of substrate surface

βˆ’πœ†πœ†

π‘”π‘”πœ•πœ•π‘‘π‘‘πœ•πœ•πœ•πœ•π‘”π‘”

|

πœ•πœ•=0

βˆ’ π‘Ÿπ‘Ÿ

𝑣𝑣

(𝐷𝐷

π‘£π‘£π‘£π‘£πœ•πœ•π‘£π‘£πœ•πœ•πœ•πœ•

+ 𝐷𝐷

π‘£π‘£π‘‘π‘‘πœ•πœ•π‘‘π‘‘πœ•πœ•πœ•πœ•π‘”π‘”

) = 𝑅𝑅

𝑛𝑛,𝑔𝑔

+ 𝐻𝐻

𝑔𝑔

+ 𝐸𝐸

𝑔𝑔

⁑⁑

(22) 𝜌𝜌

𝑀𝑀

βˆ†π‘§π‘§

𝑑𝑑𝑣𝑣𝑑𝑑𝑑𝑑

= βˆ’

πœ•πœ•(π‘žπ‘žπœ•πœ•πœ•πœ•π‘™π‘™+π‘žπ‘žπ‘£π‘£)

βˆ’

πΈπΈπ‘Ÿπ‘Ÿπ‘”π‘”

𝑣𝑣

βˆ’ 𝑆𝑆 + 𝑃𝑃 ⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑

(23) 𝐻𝐻

𝑔𝑔

= (𝜌𝜌𝐢𝐢

𝑝𝑝

)

π‘Žπ‘Ž(𝑑𝑑(π‘Ÿπ‘Ÿπ‘”π‘”βˆ’π‘‘π‘‘π‘π‘)

π‘Žπ‘Žπ‘ π‘ )

⁑⁑⁑⁑⁑

(24) 𝐸𝐸

𝑔𝑔

=

(πœŒπœŒπΆπΆπ›Ύπ›Ύπ‘π‘)π‘Žπ‘Ž(π‘Ÿπ‘Ÿ(π‘’π‘’π‘”π‘”βˆ’π‘’π‘’π‘π‘)

𝑔𝑔𝑠𝑠+π‘Ÿπ‘Ÿπ‘Žπ‘Žπ‘ π‘ )

⁑⁑⁑⁑⁑⁑⁑⁑

(25)

where πœ†πœ†π‘”π‘”is thermal conductivity of substrate layer, 𝑇𝑇𝑔𝑔 is temperature of substrate layer, π‘Ÿπ‘Ÿπ‘£π‘£ is latent heat of moisture, 𝐷𝐷𝑣𝑣𝑣𝑣 and 𝐷𝐷𝑣𝑣𝑑𝑑 are transfer coeffcients of water vapor under gradient of moisture and temperature, πœƒπœƒ is volumetric water ratio of substrate layer, 𝑅𝑅𝑛𝑛,𝑔𝑔is net radiation of substrate surface, 𝐻𝐻𝑔𝑔 and 𝐸𝐸𝑔𝑔is sensible heat and latent heat transfer of substrate surface, πœŒπœŒπ‘€π‘€ is density of liquid water, βˆ†π‘§π‘§ is grid step of substrate layer, π‘žπ‘žπ‘™π‘™ and π‘žπ‘žπ‘£π‘£ are liquid water and gas water transfer, S and P are evaporation wate loss and precipitation. π‘Ÿπ‘Ÿπ‘”π‘”π‘ π‘  and π‘Ÿπ‘Ÿπ‘Žπ‘Žπ‘ π‘  are water vapor resistance of sub- strate surface and canopy space. 𝑒𝑒𝑔𝑔 is saturated water vapor of substrate surface.

2.2.5 Energy balance of canopy air

(𝜌𝜌𝐢𝐢

𝑝𝑝

)

π‘Žπ‘Ž

(𝐿𝐿 βˆ’ 𝑑𝑑

𝑓𝑓

𝐿𝐿𝐿𝐿𝐿𝐿)

𝑑𝑑𝑑𝑑𝑑𝑑𝑑𝑑𝑐𝑐

= βˆ’π»π»

𝑓𝑓

βˆ’ 𝐻𝐻

𝑔𝑔

βˆ’ 𝐻𝐻

π‘Žπ‘Ž

⁑⁑⁑⁑⁑⁑

(26) 𝐻𝐻

π‘Žπ‘Ž

= (𝜌𝜌𝐢𝐢

𝑝𝑝

)

π‘Žπ‘Ž(𝑑𝑑(π‘Ÿπ‘Ÿπ‘Ÿπ‘Ÿβˆ’π‘‘π‘‘π‘π‘)

π‘Žπ‘Ž)

⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (27) (𝐿𝐿 βˆ’ 𝑑𝑑

𝑓𝑓

𝐿𝐿𝐿𝐿𝐿𝐿)

π‘‘π‘‘π‘žπ‘žπ‘‘π‘‘π‘‘π‘‘π‘π‘π‘“π‘“

=

πΈπΈπ‘Ÿπ‘Ÿπ‘“π‘“

𝑣𝑣

+

πΈπΈπ‘Ÿπ‘Ÿπ‘”π‘”

𝑣𝑣

+

(πœŒπœŒπΆπΆπ›Ύπ›Ύβˆ™π‘Ÿπ‘Ÿπ‘π‘)π‘Žπ‘Ž

𝑣𝑣

(π‘’π‘’π‘π‘βˆ’π‘’π‘’π‘Ÿπ‘Ÿ)

π‘Ÿπ‘Ÿπ‘Žπ‘Ž

⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (28)

Where 𝐻𝐻𝑓𝑓 and 𝐻𝐻𝑔𝑔 are sensible heat transfer from plant and substrate surface to canopy space, and π»π»π‘Žπ‘Ž is sensible heat transfer from reference height to canopy space. π‘‡π‘‡π‘Ÿπ‘Ÿ is temperature of refer- ence height, 𝑇𝑇𝑐𝑐 is temperature of canopy space, π‘’π‘’π‘Ÿπ‘Ÿ is water vapor pressure of reference height, L is height of canopy space, and π‘žπ‘žπ‘π‘π‘–π‘– is absolute humidity of canopy space.

2.2.6 Coupled hygrothermal transfer of substrate layer

𝜌𝜌

𝑀𝑀

βˆ†π‘§π‘§

πœ•πœ•π‘£π‘£πœ•πœ•π‘‘π‘‘

= βˆ’

πœ•πœ•(π‘žπ‘žπœ•πœ•πœ•πœ•π‘™π‘™+π‘žπ‘žπ‘£π‘£)

βˆ’ 𝑆𝑆 ⁑⁑⁑⁑⁑

(29) (𝜌𝜌𝐢𝐢

𝑝𝑝

)

π‘”π‘”πœ•πœ•π‘‘π‘‘π‘”π‘”

πœ•πœ•π‘‘π‘‘

+ (𝜌𝜌𝐢𝐢

𝑝𝑝

)

𝑀𝑀

π‘žπ‘ž

π‘™π‘™πœ•πœ•π‘‘π‘‘π‘”π‘”

πœ•πœ•πœ•πœ•

= βˆ’

πœ•πœ•π‘žπ‘žπœ•πœ•πœ•πœ•β„Ž

⁑⁑⁑

(30) π‘žπ‘ž

𝑙𝑙

= (βˆ’ (𝐷𝐷

π‘™π‘™π‘£π‘£πœ•πœ•π‘£π‘£πœ•πœ•πœ•πœ•

+ 𝐷𝐷

π‘™π‘™π‘‘π‘‘πœ•πœ•π‘‘π‘‘πœ•πœ•πœ•πœ•π‘”π‘”

) βˆ’ 𝐾𝐾) ⁑

(31) π‘žπ‘ž

𝑣𝑣

= βˆ’(𝐷𝐷

π‘£π‘£π‘£π‘£πœ•πœ•π‘£π‘£

+ 𝐷𝐷

π‘£π‘£π‘‘π‘‘πœ•πœ•π‘‘π‘‘π‘”π‘”

) ⁑⁑⁑

(32)

π‘žπ‘ž

β„Ž

= βˆ’πœ†πœ†

π‘”π‘”πœ•πœ•π‘‡π‘‡π‘”π‘”

πœ•πœ•πœ•πœ•

βˆ’ π‘Ÿπ‘Ÿ

𝑣𝑣

𝜌𝜌

𝑀𝑀

(𝐷𝐷

π‘£π‘£π‘‡π‘‡πœ•πœ•π‘‡π‘‡π‘”π‘”

πœ•πœ•πœ•πœ•

+ 𝐷𝐷

π‘£π‘£π‘£π‘£πœ•πœ•π‘£π‘£

πœ•πœ•πœ•πœ•

) ⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑⁑ (33)

Dalam dokumen Welcome from the Conference 2 Contents 3 (Halaman 155-159)