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poster - International Conference of Agricultural Engineering

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• The effectiveness <strong>of</strong> the crop coefficient method to determine water requirements <strong>of</strong><br />

the orange orchard and to verify the suitability <strong>of</strong> the K c value proposed for a generic<br />

citrus crop.<br />

2. Materials and methods<br />

2.1. Site information and field measurements<br />

The trial was carried out during the monitoring period 2010-2011 within an orange orchard<br />

located in Sicily, Southern Italy (Lentini, lat. 37°16’N, long. 14°53’E). This area has a<br />

Mediterranean semi-arid climate (annual mean air temperature 17°C and rainfall less than<br />

600 mm). The experimental field was planted with 15-25 year old orange trees, grown in an<br />

orchard <strong>of</strong> about 120 ha. The mean canopy height was 3.75 m. Leaf area index (LAI, m 2 m -2 )<br />

was found to be in the range 4.0-4.7. For the dominant wind direction (the main were W and<br />

NW), the fetch was larger than 550 m. The crop was maintained in a well-watered conditions<br />

by irrigation supplied every day during hot months (May-October). Water was supplied by<br />

drip irrigation, with on-line labyrinth drippers, in a number <strong>of</strong> four per plant, spaced at 0.80 m,<br />

with discharge rate <strong>of</strong> 4 l/h at a pressure <strong>of</strong> 100 kPa.<br />

Continuous energy balance measurements were made from January 2010 until December<br />

2011. Net radiation (R n , W m -2 ) was measured with two CNR 1 Kippen&Zonen net radiometer<br />

at height <strong>of</strong> 8 meter. Soil heat flux density (G, W m -2 ) was measured with three soil heat flux<br />

plates, which were placed horizontally 0.05 meter below soil surface. The air temperature<br />

and the three wind speed components were measured at two heights, 4 and 8 meter, using<br />

fine wire thermocouples (76 µm diameter) and sonic anemometers (CSAT, Campbell Sci.). A<br />

gas analyzer (CSAT, Campbell Sci.) operating at 10 Hz was deployed at 8 meter. The raw<br />

data were recorded at a frequency <strong>of</strong> 10 Hz using two synchronized data loggers.<br />

Low frequency measurements were taken for air temperature and humidity, wind speed and<br />

direction, and atmospheric pressure at 4 and 8 meter. Rainfall was measured nearby.<br />

2.2. Energy closure at the orange orchard and correction <strong>of</strong> measured sensible and latent<br />

heat fluxes<br />

Neglecting the amount <strong>of</strong> available energy at the land surface that is used for photosynthesis<br />

(typically less then 1% <strong>of</strong> net radiation), the surface energy balance can be expressed at<br />

hourly or longer time scale as:<br />

R n = H + λE<br />

+ G<br />

(1)<br />

R n -G is commonly termed available energy and the surface heat storage (G) at daily or<br />

longer time scales is negligible.<br />

The EC method, applied at the site selected for this study, allows for estimates <strong>of</strong> H and λE<br />

from direct measurements <strong>of</strong> fluctuations in the vertical wind velocity and the scalar<br />

concentration. The lack <strong>of</strong> closure in the energy budget is commonly quantified by the<br />

relative difference between (R n -G) and (H+λE), expressed as a percentage: 100×[((R n -<br />

G)/(H+λE))-1]. Figure 1 shows the hourly data on (H+λE) plotted against (R n -G). Assuming<br />

that R n and G measurements are rather accurate, Fig. 1 shows that during both the<br />

monitored years (H+λE) is underestimated at the site. This may arise from an<br />

underestimation <strong>of</strong> H or λE, or both. The mean annual energy imbalance is 29.3% during<br />

2010 and 31.1% in 2011, showing peaks during winter and a variation <strong>of</strong> about 30%.<br />

The BR approach assumes that the EC technique provides correct estimates <strong>of</strong> the Bowen<br />

ratio (β=H/λE) even though it underestimates H and λE, as some studies tend to confirm (El<br />

Maayar et al., 2008). Thus rearrangement <strong>of</strong> eq. 1 yields:<br />

Rn − G<br />

λE<br />

=<br />

(2)<br />

1+ β

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