Journal of Horticultural Science & Biotechnology (2004) 79 (5) 699-703 Measurements of net radiation absorbed by isolated acid lime trees {Citrus latifolia Tanaka) 1 1 2 3 By L . R. A N G E L O C C T , N. A . V I L L A N O V A , M . A . C O E L H O F I L H O and E R. M A R I N departamento de Ciências Exatas, Escola Superior de Agricultura "Luiz de Queiroz", Universidade de São Paulo, CP 9, CEP 13418-900, Piracicaba, SP, Brazil Centro Nacional de Pesquisa de Mandioca e Fruticultura, E M B R A P A , Cruz das Almas, BA, Brazil Centro Nacional de Pesquisa de Monitoramento de Satélite, E M B R A P A , Campinas, SP, Brazil (e-mail: lrangelo@carpa.ciagri.usp.br) (Accepted 5 April 2004) 2 3 SUMMARY B y using net radiometers mounted on a circular frame rotating around the canopy, measurements of total all-wave radiation absorbed by t w o ' T a h i t i ' acid lime trees were carried out i n an orchard in Piracicaba, S ã o Paulo State, Brazil. The rotating system around the canopy o f a tree was formerly idealized and used i n New Zealand, allowing integration o f all-wave radiation and photosynthetically active radiation absorbed. I n an experiment i n December 1997, a first device using six net radiometers mounted o n a light frame was used. A bigger device, more like the one used i n New Zealand, in terms of the number of radiometers and the frame, w i t h a different torque system, was used i n another tree on some days from July t o September 2000. The performance of b o t h devices is discussed, including the possible error sources when using the first model (1997) and the problems of torque transmission on the second. Despite the lack of a test to check the performance of the device and the problems presented i n the year 2000, the results confirm the possibility of providing reliable measurements of the net radiation absorbed by isolated trees. Relations o f the net radiation per unit area of projected canopy on the ground were determined with integrated values over different time scales (from 15 min t o 24 h ) . U n i q u e relations between net radiation and incoming solar radiation were obtained for both trees over several time scales. These relations are applicable only to high leaf density conditions and canopy geometry similar to the used i n this study. ' T ' h e net radiation absorbed by a tree canopy is a A determinant variable of transpiration and photosynthesis, w i t h application i n a g r i c u l t u r a l and environmental studies. I n tree species, it is i m p o r t a n t to determine the relations o f the radiant energy with the plants, which depend on the tree canopy geometry, leaf area density, trees spacing and o t h e r factors that d e t e r m i n e the losses and gains o f energy. The measurements as well as the estimations are complex due to the number o f factors involved. Some papers have been w r i t t e n on the determination of light interception by canopies, such as those of apple trees (Charles-Edwards and Thornley, 1973; CharlesEdwards and Thorpe, 1976; Thorpe, 1978; W ü n s c h e et al., 1995). I n New Zealand, M c N a u g h t o n et al. (1992) used a device named a " w h i r l i g i g " , formed o f net radiometers and quantum sensors mounted o n a circular frame. The frame rotated a r o u n d a Robinia pseudoacacia tree, allowing integrated measurements of net radiation ( R n ) and photosynthetically active radiation ( P A R ) fluxes passing through the surface enclosing the tree. Green (1993) used this technique to estimate net radiation and P A R absorbed by a walnut single tree. Further, Green et al. (1995, 2001) and Green and M c N a u g h t o n (1997) also used the technique i n studies with an apple tree. In the present paper, results and measurements of net •Author for correspondence. radiation absorbed by the canopy of t w o trees of 'Tahiti' acid lime (Citrus latifolia Tanaka) are presented and discussed, using the " w h i r l i g i g " technique developed in New Zealand. The relations between the canopy net r a d i a t i o n and i n c o m i n g solar r a d i a t i o n are also presented and discussed. MATERIAL A N D METHODS Data were obtained for two periods. The first was 12 days in December, 1997 and the other with a further 6 d from the end o f July to September of 2000, in a 'Tahiti' acid lime orchard, with tree spacing of 8.0 m x 7.0 m , g r o w i n g i n the " L u i z de Q u e i r o z " Campus o f the University of S ã o Paulo, Piracicaba, S ã o Paulo State, Brazil (latitude 2 2 ° 4 2 ' , longitude 4 7 ° 3 8 ' W, altitude 540 m above mean sea level).The orchard, surrounded in the west and in the north by an eucalyptus windbreak 20 m tall, was irrigated by mini-sprinklers.To the south, there was a mango orchard and l o w vegetation to the east. In 1997, a six year old tree was used with a total leaf area of 39.9 m , located about 25 m from the windbreak to the west. The canopy was pruned just before the system installation to eliminate branches exceeding the limits of the frame, allowing its free movement. I n 2000, a nine year o l d tree was used, located 14 m from the east border o f the orchard, 38 m from the windbreak, with a total leaf area o f 51.2 m , after the p r u n i n g to allow the 2 2 Acitl lime net rndiutioii absorption by I wo vertical circles ami two horizontal ones (Figure la), manufactured with a l u m i n u m tubes of I ) m m outside diameter (Figure l a ) , rotated by a 0.25HP electric motor, with direct transmission of the movement by a reduction system attached directly to the upper pole of the frame. The motor was held by an horizontal bar attached to a mast from which the frame was suspended. The mast was positioned so as to minimize shading the tree. 1 The measurements in 2000 were performed using a frame whose structure was composed o f two concentric circles of mild steel lubes o f 40 m m outside diameter (Figure l b ) . Hie circles were interconnected by small bars of similar material and the outer tube was flattened where the radioniclers were mounted. Pie circular frame was mounted on a horizontal turntable, composed o f one mild steel stationary circle mounted in I luce levelling jacks. A b o v e this stationary circle, there was another circle of flat-section steel fitted with nylon wheels resting on the stationary circle.The upper circle and the vertical frame rotated, powered by a I I I I * motor, with a reduction gearbox. Torque was transmitted by a belt drive from the driven pulley of the gearbox to the upper, rotating circle. In both devices, the rotation speed of the frame was about three revolutions per minute, as used by McNaughton ci <;/. (1992). In December 1997. six net radiometers R E B S (Radiation and l.ncrgv Balance Systems. Seattle. W A , USA) model 0 * 7 were used, two fewer than the number used in the New Zealand experiments. In 2000, eight net radiometers were used. Hie radiometers used in l'W7 were used i m m e d i a t e l y after purchase, so the calibrations factors supplied by the manufacturer were used. In 2000. the net radiometers were calibrated against a C N R I net radiometer ( K i p p & Z o n e n . Delft, The Netherlands). McNaughton <•/ .//. (1992) found that placing the sensor plate of the net radiometers in non-horizontal positions in which the) were calibrated did nol affeel theit calibration factors, FIG. 1 Top: view of ihc rut.ilinir Ir.imc (without ihc ncl radiometers) used in December 1997. Bottom:device used in 2000. frame 10 rotate. The drip-line leaf area index (canopy leaf area per ground area w i t h i n the plant's d r i p line) was 4.(>ft for the first and 3.09 for the second tree. Estimation of c r o w n porosity, by the use o f frontal canopy photographs taken from the four cardinal points with a white sheet suspended vertically behind the canopy and their image processing, showed the low average porosity on a vertical plane traversing the canopy, 2% on the first and 5% on the second tree. The windbreak started to project shadows on the trees between 1700 and 1730 hours (local lime). Measurements in December I W 7 used a modified rotational system based o n the one proposed I n McNaughton el al. (1992). It consisted of a frame formed The t e r m i n o l o g y and the calculation procedures described by M c N a u g h t o n el al. (1992) were adopted. The sensing sphere radius was 1.65 in lor the tree used in 1997 and 1 3 1 in in 2000. In 1997. the sensors were mounted at equi-latitudinal intervals, at latitudes +75'. +45". +15". -15 . —45 . -75 (positive: sensor above the equatorial circle of the sphere: negative: below I . In 2000. the equi-latitudinal disposition was adopted exactly as used by M c N a u g h t o n el al. (1992) at latitudes of +78.75°, +56.25°. +33.75°. +11.25°. -11.25°. -33.75°. -56.25°. -78.75°. The integration method proposed bv McNaughton el al. (1992) to calculate the value of Rn over the sensing sphere, was adopted, with weighting factors considering ihc m o u n t i n g positions (fable 11. C R - 1 0 X Dataloggers (Campbell Scientific. Logan. U T . I I S A ) were used in 1997, and model 21-X in 2000. IAIU I I Prtunul UWC7I//MC ftiiiors tor etich mounting position itwil in the intetrillion itiUiilu\. \l. \2 YN* M-ipiential inountinv position for the ncl radiometers, \ l being the upper h. I \ n.134 O.IK.7 \ 0.365 (1.221 \ 0.501 D.326 \ : \- 0.501 0.386 0.365 0.38ft V 0.134 0.32ft \~ \- 0.221 n.oh7 1.. R. A M ii I I I I c I , N . A . V I L I \ N O V A . M . A . C O B L H O F l L l l o and mounted on platforms fixed w> the rotating pari of the turntable recorded signals from the sensors at a sample rale of I 11/ and calculated averages every 15 m i n . R l SI I I S A M ) D I S C U S S I O N Figure 2 shows examples of the daytime course of net radiation for each measurement position of the two trees, w i t h averages every 15 m i n . A l t h o u g h the measurements were also carried out at night, they are not show n, because the net r a d i a t i o n differences among the different measurement positions around the canopy in the day were much more pronounced than at night, due to the fact that daytime net radiation is dominated I n short-wave r a d i a t i o n , which depends on atmospheric t u r b i d i t y and the incidence angle o f the sunbeam on the sensor plates, which explain the high positive values of Rn a r o u n d midday at more positive latitudes and slightly positive or negative at more negative latitudes. On the first tree with six net radiometers, values during the course of the day varied around zero at - 4 5 ° . becoming more negative at - 7 5 ° . O n the second tree, with more sensors, values close to zero or slightlv negative occurred at position 7 (latitude: -56.25 ) and negative at position S (latitude: -7S.75 ). In a general way. the variation patterns observed in each position can he compared to those found by M c N a u g h t o n end. (1992) for a single Robinia pseudoacacia tree on a sunny day. with differences between the two cases related to the number of sensors used, to geographical location, to season, to leal density and to the canopy geometry. A s affirmed by McNaughton el til. (1992), it is difficult to evaluate the accuracy of the measurements by the " W h i r l i g i g " system. In the present study, tests were not done when the sensing sphere was totally empty to check if the radiometers had matched characteristics. Theoretically, if they are matched, record zero should occur when the sensing sphere is empty, but it depends on the structure used and on the net r a d i o m e t e r placemen! and performance. McNaughton <•/ ul. (1992) concluded that in their F. R. M \ K I N 701 system, the zero deviation was smaller than 5".. of the radiation absorbed d u r i n g midday, lite type o l structure used m 2000 had little change in relation to the one used in New Zealand, which is w i n we can also admit thai in our case the zero deviation could have the same value. The structure used in 1997 was mounted with steel tubes of a smaller diameter w h i c h could p r o b a b l y have interfered less for net radiation than the one used in New Zealand and in our 2000 experiment. In 1997. the presence of an additional circular tube in the horizontal plane and another in the vertical could have increased the structural effect on the record zero. Rut. based on the results of McNaughton ct til. (1992). we assume thai the total absorption o l all-wave radiation of our devices was not a serious problem. In relation to the net r a d i a t i o n measurements. McNaughton ft til. (1992) did not obtain reliable results when Ihey used sensors of several ages ami different manufacturers, but in 1997 we used brand-new equipment of a single manufacturer. In 2000. all the sensors useil were re-calibrated. The use of six net radiometers in December 1997 is another factor that may have increased the measurement errors lor the canopy, when compared with the use of eight sensors. The tact of the sensing sphere railius of the " W h i r l i g i g " of 1997 was a little smaller than Ihe one used in New Zealand could have slightlv minimized the problems caused by Ihe use o f only six net radiometers, but the difference between the radii o f the sensing sphere (0.20 m ) of the two devices was too small. The sensing sphere radius of the " W h i r l i g i g " used in 2000 was almost (1.5 m bigger than Ihe one used in New Zealand, so the calculation procedure used for integrating net radiation values can result in more errors than those obtained in thai country. M o r e net radiometers would improve the performance of the devices, mainly in 199" TTie frame used in 1997 was lighter and different from Ihe one used in 2000. which helped its installation, but the suspended system can oscillate a little when the wind is strong. However, most of the time winds were more gentle, excepting on December 14. 15. Hi and 19. when strong winils happened at short time intervals, reaching speed between 30 k m h and 45 km h . Illis first " W h i r l i g i g " functioned continuously for several days without problems. Nevertheless, to avoid the problem of oscillation, a turntable would be preferable. : DEC 14,1987 C~ 1 400 IK 600 500 400 130« LOCAL On the other hand, the device used in 2000 showed problems of torque transmission, caused by chain slip. Sometimes, tension applied to stop slippage resulted in stressing and failure o f the gearbox. In consequence, there were many incomplete days of measurement and time loss to r e p a i r the system, w i t h a worse performance than that obtained using Ihe New Zealand transmission system. A c c o r d i n g to M c N a u g h t o n ct al. (1992). t h e i r system showed adequate mechanical performance allowing continuous measurements for periods up to two weeks. 12CC 1433 1t00 1M« TMEim JUL36.200C - W I \ L 3 V ,00 a o 103 200 300 Daily BOC 10UJ 1200 S400 1600 1S00| LOCAL TIME (ht> course 800 10O0 1J00 I4C0 1600 1600 LOCAL TIME irif, Flo. 2 measured net r a d i a t i o n h\ ( l i e s e n s o r s l o r s e v e r a l days i n l<W7 (top) a n d 2(100 of the inounlinc. posiiion. in each (below). N u m b e r s following Ihe lines represent (he m o u n l i u c posiiion. from (he up|>cr l o t h e l o w e s t r a d i o m e t e r . Although the problems mentioned and the lack of a better test, in our o p i n i o n the results confirm the conclusion ol McNaughton et al. (1992) thai the devices can give reliable and accurate measurements of net radiation, with the possibility of testing models for all-wave radiation and I ' A R absorbed by trees and their application in studies of transpiration and < 10 el's a 5 Kt.yvr »w -. J r = 0.930 10 2 30 25 15 20 Rs (MJ m" d" ) 1 -0.2 2 Rs(MJ m" 15min"') -0.3 2 30 m i n , 1 h and for the whole daytime penou. A number o f f i t t i n g curves were tested using the p r o g r a m " T a b l e c u r v e " . A s t h e t w o t r e e canopy dimensions were different, w h i c h affects the integrated values o f net r a d i a t i o n for each tree, we used the value of R n divided by the projected canopy area ( P A ) on the g r o u n d ( R n / P A ) as t h e y-variable. G o o d relations between R n / P A and Rs, were f o u n d i n the 24 h and i n the d a y t i m e periods, w i t h significant linear f i t t i n g (Figure 3 ) . I t is k n o w n that Rs is the m a i n variable which determines the a m o u n t o f net radiation falling on plant canopies i n the d a y t i m e , explaining the best correlations f o u n d i n this p e r i o d . A l t h o u g h the linear f i t t i n g was good i n all integration scales for the pooled values o f the t w o trees, the linear f i t t i n g was advantageously replaced by a sigmoid curve in the hourly, 30 m i n and 15 m i n scales (Figure 3 ) , w h i c h allowed a better f i t t i n g for lower values o f i n c o m i n g solar r a d i a t i o n i n the beginning as well as at the end of the daytime, when R n shows l o w values, negative or positive ones. F u r t h e r m o r e , the sigmoid curve fits better for h i g h values at midday. Such results indicate the possibility of estimating net radiation intercepted by trees o n these time scales from two simple measurements, that is, i n c o m i n g solar radiation and the projected canopy area o n the ground. For the smaller tree here used, Angelocci et al. (1999) found good linear relations for the daily and daytime values between the integrated net radiation and the net radiation measured over grass. B u t , contrary to what was observed here, these relations were seasonally dependent; so, the unique relations for both trees and different seasons here reported represent an advantage. 1 Rs (MJ m" 30 min" ) However, we should emphasize that the relation found in the present study can be applied only to trees w i t h (jfld growth conditions observed i n this jfyrjjj mih very dense" ll expl-(x-0.816)/0.753] tree studied in M were twice astyi!M ( f a i tree used in 1997, and almost identical to (lie tehtk h •0.5 ^ o T o ! , 2.0 3.0 40 2 Rs (MJ m" hr"') e T° P y a r e a p r o j e c t e d o n , h e ground (or also, the lateral area o f the crown) o f both trees T h i an -nd.cat.on that the foliage density led to a verZ h h and equivalent a t t e n u a t i o n ( p r o b a b l y almost he m a x i m u m ) o f solar radiation by the two c L 2 2 such e FIG 3 the geometric relations mentioned above Iea?a rl r?nH r a v o i d t h e p r o b , e m s o b s e r v e d in °- torL V ^ r . m e n t s we intend to modify the torque transm.ss.on system of the bigger ••Whirhgig" r Witl ! g e ° m C , r i e s a n d W drip-line L . R . A N G E L O C C I , N . A . V I L L A N O V A , M . A . C O E L H O F I L H O and F. R . M A R I N density different from those observed in this study. But it seems that the observed relations may be applied t o lhe other similar trees of the studied orchard. 703 The first two authors thank lhe Consilho Nacional di Desenvolvimento C i e n t í f i c o e T e c n o l ó g i c o f o r their fellowship. REFERENCES ANGELOCCI, L. R., V I L L A NOVA, N . A.and SENTELHAS, P. C. (1999). GREEN, S. R. and MCNAUGHTON, K . G . (1997). Modelling effective Medida do saldo de energia radiante na copa de lima ácida "Tahiti' e sua relação com a medida sobre gramado. Anais do XI Congresso Brasileiro de Agromeleorologia, Florianópolis, 1999. stomatal resistance for calculating transpiration from an apple tree. Agricultural and Forest Meteorology, 8 3 , 1 - 2 6 . C D - R O M , 1292-98. CHARLES-EDWARDS, D . A . and THORNLEY, J. H . M . (1973). Light interception by an isolated plant: a simple model. 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Agriculture and Forest Meteorology, 62, 87-107. THORPE, M. R. (1978). Net radiation and transpiration of apple trees in rows. Agricultural Meteorology, 19,41-57. WUNCHE.J. N„ LAKSO, A . N. and ROBINSON.T L . (1995). A compar- ison of four methods for estimating total light interception by apple trees of various forms. HortScience, 30, 272-6. Pesquisa Periódicos ragina i ae i PESQUISA DE PERIÓDICO POR TÍTULO Titulo: Relação de Periódicos - Classificação relativa a dados de 2003 ISSN 0022-1589 Critérios de Classificação do Qualls por Área \ Area de Avaliação Classificação Circulação Título Journal of Horticultural Science & Biotechnology A ^rH o o §? ' » — L 0 N L H T CULTURALSCIENCEi http://qual i s. capes.gov.br/pesqui sa/Servl etPesqui sa Internacional — ZOOTECNIA / RECURSOS PESQUEIROS MULTIDISCIPLINAR 4/11/2004