SOLAR RADIATION AVAILABILITY FOR PLANT GROWTH IN ARIZONA CONTROLLED ENVIRONMENT AGRICULTURE SYSTEMS



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SOLAR RADIATION AVAILABILITY FOR PLANT GROWTH IN ARIZONA CONTROLLED ENVIRONMENT AGRICULTURE SYSTEMS Stephen Kania, Horticultural Engineer Gene Giacomelli, Professor & Director CEAC Controlled Environment Agriculture Center (CEAC) Department of Agricultural and Biosystems Engineering University of Arizona Tucson, Arizona Abstract: The availability of solar radiation and its daily and yearly distribution has a tremendous influence on the productivity and quality of plant growth. In controlled environment agriculture (CEA), where all other environmental factors such as air temperature, irrigation and nutrition are controlled or enhanced, the solar radiation or light is the most limiting factor for plant growth. Thirteen years of solar radiation data from AZMET (Arizona Meteorological Network) which provides meteorological data for southern and central Arizona, was downloaded and analyzed to determine the total solar radiation received in Tucson, Arizona. All data were converted into quantum units, so that the total moles m -2 per day could be calculated. Plant photosynthesis and subsequent growth are directly proportional to the moles of light received by the plant. Total moles per year, as well as the average daily moles were also calculated. The maximum for the thirteen-year dataset was 70.3 moles m -2 per day. Keywords: solar radiation, moles, quantum sensor, AZMET, PAR Introduction Plants require solar radiation for photosynthesis, and their growth rate is proportional to the amount received, assuming that other environmental parameters are not limiting. Visible light is a composite of wavelengths between 400 and 700 nanometers (nm), and this specific waveband is defined as PAR (photosynthetically active radiation). PAR consists of wavelengths that are utilized by the plant biochemical processes in photosynthesis to convert light energy into biomass. The PAR can be defined as quantum units of light energy, and expressed as the number of photons of light received on a unit area. A single photon is an extremely small amount of energy, however, with a discrete energy value that is inversely related to its wavelength. Individually each photon with their specific wavelength and energy level represents a color as perceived by the human eye. When combined, such as in sunlight, the photons between 400 and 700 nm make white light. When measuring light by quanta (or number of photons), the common unit is micromoles (one millionth of a mole) of light, where a mole of photons is 6.02 x 10 23 of them. The time (second) and area (square meter) are included to provide a rate per unit area, and thus measurements for light quanta have units of micromoles per second per square meter (µmol s -1 m -2 ). This is considered an instantaneous rate, and is measured by a quantum sensor to provide average hourly values. The total amount of the light energy received over a prescribed time period, a day for example, is the sum of the light energy and is expressed in mol m -2. It can be calculated by multiplying the average hourly value (µmol s -1 m -2 ) by the number of seconds per hour (3600 sec) and dividing by one million to obtain the mole per square meter

for a given hourly period (mol m -2 per hour). The sum of these hourly calculations throughout the day would provide the daily total moles per square meter (mol m -2 per day). Light energy can also be defined in radiometric units, which is measured with a pyranometer. In radiometric units, light energy is expressed in terms of the Joule. Again, the time (second) and area (square meter) are included to provide a rate per unit area, and thus radiometric measurements for light energy are Joule per second per square meter (J s -1 m -2 ). A Joule per second is also defined as a Watt, which is energy per unit time. Therefore, the radiometric measure of light energy has units of Watts per square meter (W m -2 ). Solar radiation may be measured in radiometric units (W m -2 ) to determine its total energy value, or it may be measured in quantum terms (µmol s -1 m -2 ) for calculation of the amount of the sunlight specifically available for plant growth during a specific growth period (mol m -2 ). Meteorological stations generally provide radiometric units of solar radiation, therefore a conversion factor is required to obtain quantum units. Solar radiation data from AZMET (Arizona Meteorological Network), for the Tucson, Arizona region was converted into more useful forms for the commercial plant production industry. Summaries of the intensity of solar radiation and the accumulated amount received for specific time periods throughout the year are provided in this paper. When planning a greenhouse, the available sunlight is one of the most important parameters to consider. Utilities, such as water, fuel for heating, electrical power, communications can be brought to the planned greenhouse, usually at reasonable cost. The lack of natural sunlight, however, cannot be corrected, even with artificial lighting which is expensive even as a supplement to natural light, and is prohibitively expensive as a replacement for sunlight. Evaluating meteorological data is a good option for determining the availability of natural sunlight at a specific location. Considerations for locating a greenhouse should include the total available daily light, and the intensity of the light throughout the year at the site. In addition, greenhouse designs, orientation, and types of glazings will all affect the amount of light transmitted into the structure and reaching the crop (Giacomelli and Roberts, 1993). The sun angle relative to the greenhouse structure changes each day from sunrise in the east to sunset in the west. However, it also changes throughout the year rising and setting at a much more northerly position during the longer sunlight days of summer, coming close to directly overhead, while remaining more southerly during the shorter days in the winter. Intensity is reduced by the low sun angles of the winter and increased by the higher angles of the summer. It is also reduced by the composition of the atmosphere, for example with higher moisture content (clouds), and longer travel distance through the atmosphere of the low angles of winter. One challenge is to construct a greenhouse that meets all criteria, such as the capital construction budget, local codes, compatibility with crop production system, etc, but that also transmits sufficient PAR to produce a good crop. Materials and Methods The solar radiation data was obtained from the historical records of the AZMET station at the Campus Agricultural Center in Tucson, Arizona. The data were measured using a Li-Cor Pyranometer which measured solar radiation in the 400-1100 nm waveband. Data were recorded as hourly averages with units of energy of Mega-Joules per square meter (MJ m -2 ). These radiometric data were converted to quantum data by using the conversion factor for atmospheric solar radiation (2.07 µmol s -1 m -2 per MJ m -2, Ting and Giacomelli, 1987), and then calculating mole m -2 per hour. This conversion factor is only valid for conversion of atmospheric measurements from radiometric and quantum units.

Thirteen years of data (1988 to 2000 plus 210 days of 2001) were analyzed. The Julian calendar (day of the year) was used as the time scale in the tables and graphs. By definition, January 1 st is Day 1 and December 31 st is Day 365 (or 366 if leap year) of the Julian year. Results and Discussion Table 1 contains the average daily PAR (mol m -2 ) and standard deviation for each month (and Julian Day) of the year for Tucson, Arizona. The standard deviation represents the variation in average daily PAR for each month. It is an indication of the sky conditions such as haze, dust, and cloud cover that occurred during each month of the year. The month of June had the highest average total daily PAR, at 60.0 moles per day. The angle of the sun directly affects the measured total light. Tucson is located at ~32 o North latitude, and the summer solstice (highest solar angle) occurs June 22 nd. The maximum solar radiation intensities which occurred throughout the year can be seen in Figure 1. The highest values occurred in May and June near the summer solstice and were as much as 1110 Wm -2. The lowest (daily high) values occurred in winter and were about 700 Wm -2. Converted to PAR, these values are 2300 and 1450, µmol s -1 m -2 respectively. The total PAR per day for each day within the 13-year period is displayed in Figure 2. The variability for each day from year to year can easily be seen. The seasonal variation is also clearly evident. Tables 2 and 3 provide the seasonal average PAR and total PAR in mol m -2 per day for the 13-year period. There was only a 12% difference in total PAR among all the 13 years (Table 3). The distribution of the PAR and total PAR per crop during the period of tomato production (September 1 st to May 31 st ) at the CEAC Hydroponic Greenhouse is shown in Table 3. This production period consists of 74.4% of the year. However, the average PAR per day during this period is 91.1% of the average daily PAR for the entire dataset. In Figure 3 the total inches of rain for any day of the year, for the 13-year period is presented. The vertical lines separate the year into the four seasons. The inset numbers are the total number of rainy days during each of the seasons for 13 years (115, 456, 199, and 93), and total inches of rain (38, 15.7, 71.2, and 34.1) received for winter, spring, summer and fall, respectively. On an average yearly basis, there are approximately 9, 35, 15, and 7 rainy days for winter, spring, summer and fall, respectively, and there are approximately 2.9, 1.2, 5.5, and 2.6 inches of rain received during the winter, spring, summer, and fall seasons, respectively. These data indicate a significant summer rainy period, and a less significant winter rainy period. Conclusions The purpose of this study was to utilize available solar radiation data, convert it into units of PAR, the portion of sunlight usable by plants, and to present it in a format to indicate how sunlight varies during the year in Tucson, Arizona. Evaluation of such data can support decisions on crop production. Acknowledgements Paper # P-125933-08-01. Supported by CEAC, the Controlled Environment Agricultural Center, College of Agriculture and Life Sciences, The University of Arizona. (ASPsk01.doc)

References Giacomelli, G.A. and W.J. Roberts. 1993. Greenhouse Glazing Systems. HortTechnology 3(1):50-58 Thimijan, R.W., Royal D. Heins. 1983. Photometric, Radiometric, and Quantum Light Units of Measure: A Review of Procedures for Interconversion. HortScience 18(6):818-822. Ting, K.C., G. A. Giacomelli. 1987. Availability of Solar Photosynthetically Active Radiation. Transactions of the ASAE. 30(5):1453-1457. Table 1. Average and Standard Deviation of Daily PAR (moles m -2 ) for Each Month in Tucson, Arizona. Month (Julian Day) Ave. Daily Ave. Daily Month (Julian Day) Ave. Daily Ave. Daily moles m -2 Std. Dev. moles m -2 Std. Dev. January (1 31) 25.4 2.90 July (182-212) 52.2 2.77 February (32-59) 31.5 3.03 August (213-243) 48.6 1.99 March (60-90) 42.3 3.23 September (244-273) 44.6 2.08 April (91-120) 52.9 3.90 October (274-304) 37.2 2.99 May (121-152) 58.9 4.03 November (305-334) 28.2 1.89 June (153-181) 60.0 3.29 December (335-365) 23.4 2.70 Table 2. Average Daily PAR (moles m -2 ) for Each Season in Tucson, Arizona. Season and Julian Day Average Moles per Day Winter, December 22 to March 21 (356-80) 30.3 Spring, March 22 to June 21 (81-172) 55.9 Summer, June 22 to September 21 (173-264) 50.1 Fall, September 22 to December 21 (265-355) 31.8 Winter Tomato Production, October through March (274 90) 31.4 Table 3. Average Daily PAR (moles m -2 ) and Total Seasonal PAR for the Tomato Production Season (September to May) in Tucson, Arizona from 1988 to 2000. Year Ave. Daily Total Year Ave. Daily Total Moles Moles Moles Moles 1988 37.7 10,244 1989 39.2 10,730 1990 37.9 10,395 1991 37.6 10,312 1992 35.3 9,698 1993 36.1 9,887 1994 37.4 10,245 1995 38.8 10,633 1996 40.3 11,072 1997 38.8 10,639 1998 38.5 10,562 1999 42.1 11,495 2000 39.7 10,909 Overall Ave 38.4 10,525

Maximum Solar Radiation in Tucson, AZ (1988-2001) 1200 Watts per Square Meter 1000 800 600 400 200 0 0 50 100 150 200 250 300 350 Julian Day Figure 1. Maximum solar radiation (W m -2 ) for each day of the year in Tucson AZ, from 1988 to 2001. * Total Daily PAR for Tucson AZ (1988-July 2001) Moles per Square Meter 70 60 50 40 30 20 10 0 0 50 100 150 200 250 300 350 Julian Day Figure 2. Total PAR (moles m -2 ) for each day of the year for Tucson, AZ (1988 to 2001).

Rain (Inches) 3.5 3.0 2.5 2.0 1.5 1.0 Winter 115 days 38.0 inches Spring 45 days 15.7 inches Sum m er 199 days 71.2 inches Fall 93 days 34.1 inches 0.5 0.0 80 172 264 355 0 50 100 150 200 250 300 350 Julian Day Figure 4. Total rain for all days in Tucson, AZ (1988 2001).