Kensuke Kimura, D. Yasutake, Yuta Miyoshi, Atsushi Yamanami, Kaoru Daiou, Haruo Ueno, M. Kitano
{"title":"Leaf Boundary Layer Conductance in a Tomato Canopy under the Convective Effect of Circulating Fans in a Greenhouse Heated by an Air Duct Heater","authors":"Kensuke Kimura, D. Yasutake, Yuta Miyoshi, Atsushi Yamanami, Kaoru Daiou, Haruo Ueno, M. Kitano","doi":"10.2525/ECB.54.171","DOIUrl":null,"url":null,"abstract":"In greenhouses, ventilation systems and circulating fans are generally employed to improve air currents in crop canopies and to produce spatial uniformity across crop environments. Low efficiency and inadequate management of these air control systems result in poor control over the crop microclimate, which significantly affects yield and the quality of crop production (Katsoulas et al., 2007). Therefore, a method to design the optimal air currents is required to facilitate optimal control over the crop microclimate, i.e., heat and mass exchange between the plant canopy and the environment. Leaves play a dominant role in heat and mass exchange between crop canopies and the environment as they comprise the majority of the plant surface (Defraeye et al., 2013). As the primary organs of photosynthesis and transpiration, leaves are considered the most important sources or sinks of heat and mass in the canopy (Schuepp, 1993). The balance of heat and mass on leaf surfaces is strongly influenced by the convective exchange between leaves and the environment through the leaf boundary layer. A key factor in the convective exchange is leaf boundary layer conductance (GA), which represents the transfer coefficient of convection on leaf surfaces. Thus, for optimal design of air currents in crop canopies, GA, which is regulated by the convective airflow adjacent to leaves, must be evaluated. Due to the difficulty of directly measuring the air currents adjacent to leaves (Boulard et al., 2002), GA is generally estimated using the semi-empirical formulae of forced convection (e.g., Monteith and Unsworth, 1990). However, such formulae cannot be applied under the lower air velocity in crop canopies within greenhouses, which requires consideration of both free and forced convection (i.e., mixed convection) (Kitano and Eguchi, 1989). Leaf boundary layer conductance can be measured using the heat balance of electrically heated artificial leaves, and many researches have evaluated GA by using various types of artificial leaves (Grace et al., 1980; Dixon and Grace, 1983; Kitano and Eguchi, 1990; Leuning and Foster, 1990; Brenner and Jarvis, 1995; Grantz and Vaughn, 1999; Stokes et al., 2006; Katsoulas et al., 2007; Kimura et al., 2016). Profiles of GA in a greenhouse under ventilated conditions have been reported by Katsoulas et al. (2007). However, there is little information on GA in closed conditions, which are typical of heated greenhouses during winter nights. Under such conditions, circulating fans are employed to maintain uniformity in air conditions and convective heat transfer in the crop canopies. In this study, continuous and multipoint measurements of GA in a tomato canopy were carried out using electrically heated artificial leaves. In addition, the vertical and horizontal distributions of GA in the canopy within the green-","PeriodicalId":11762,"journal":{"name":"Environmental Control in Biology","volume":"28 1","pages":"171-176"},"PeriodicalIF":0.0000,"publicationDate":"2016-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Environmental Control in Biology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2525/ECB.54.171","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"Agricultural and Biological Sciences","Score":null,"Total":0}
引用次数: 5
Abstract
In greenhouses, ventilation systems and circulating fans are generally employed to improve air currents in crop canopies and to produce spatial uniformity across crop environments. Low efficiency and inadequate management of these air control systems result in poor control over the crop microclimate, which significantly affects yield and the quality of crop production (Katsoulas et al., 2007). Therefore, a method to design the optimal air currents is required to facilitate optimal control over the crop microclimate, i.e., heat and mass exchange between the plant canopy and the environment. Leaves play a dominant role in heat and mass exchange between crop canopies and the environment as they comprise the majority of the plant surface (Defraeye et al., 2013). As the primary organs of photosynthesis and transpiration, leaves are considered the most important sources or sinks of heat and mass in the canopy (Schuepp, 1993). The balance of heat and mass on leaf surfaces is strongly influenced by the convective exchange between leaves and the environment through the leaf boundary layer. A key factor in the convective exchange is leaf boundary layer conductance (GA), which represents the transfer coefficient of convection on leaf surfaces. Thus, for optimal design of air currents in crop canopies, GA, which is regulated by the convective airflow adjacent to leaves, must be evaluated. Due to the difficulty of directly measuring the air currents adjacent to leaves (Boulard et al., 2002), GA is generally estimated using the semi-empirical formulae of forced convection (e.g., Monteith and Unsworth, 1990). However, such formulae cannot be applied under the lower air velocity in crop canopies within greenhouses, which requires consideration of both free and forced convection (i.e., mixed convection) (Kitano and Eguchi, 1989). Leaf boundary layer conductance can be measured using the heat balance of electrically heated artificial leaves, and many researches have evaluated GA by using various types of artificial leaves (Grace et al., 1980; Dixon and Grace, 1983; Kitano and Eguchi, 1990; Leuning and Foster, 1990; Brenner and Jarvis, 1995; Grantz and Vaughn, 1999; Stokes et al., 2006; Katsoulas et al., 2007; Kimura et al., 2016). Profiles of GA in a greenhouse under ventilated conditions have been reported by Katsoulas et al. (2007). However, there is little information on GA in closed conditions, which are typical of heated greenhouses during winter nights. Under such conditions, circulating fans are employed to maintain uniformity in air conditions and convective heat transfer in the crop canopies. In this study, continuous and multipoint measurements of GA in a tomato canopy were carried out using electrically heated artificial leaves. In addition, the vertical and horizontal distributions of GA in the canopy within the green-
在温室中,通常采用通风系统和循环风扇来改善作物冠层的气流,并在作物环境中产生空间均匀性。这些空气控制系统的低效率和管理不足导致对作物小气候的控制不力,从而严重影响作物生产的产量和质量(Katsoulas et al., 2007)。因此,需要一种设计最佳气流的方法来促进对作物小气候的最优控制,即植物冠层与环境之间的热量和质量交换。叶片在作物冠层与环境之间的热量和质量交换中起主导作用,因为它们占植物表面的大部分(Defraeye et al., 2013)。叶片作为光合作用和蒸腾作用的主要器官,被认为是冠层最重要的热量和质量的来源或汇(Schuepp, 1993)。叶片表面的热量和质量平衡受到叶片与环境之间通过叶片边界层的对流交换的强烈影响。对流交换的一个关键因素是叶片边界层电导(GA),它代表了叶片表面对流的传递系数。因此,对于作物冠层气流的优化设计,必须对叶片附近对流气流调节的遗传系数进行评估。由于难以直接测量叶片附近的气流(Boulard et al., 2002),一般采用强制对流的半经验公式估算总风量(例如,Monteith and Unsworth, 1990)。然而,在温室内作物冠层空气流速较低的情况下,该公式不适用,需要同时考虑自由对流和强制对流(即混合对流)(Kitano and Eguchi, 1989)。叶片边界层电导率可以通过电加热人工叶片的热平衡来测量,许多研究已经通过使用各种类型的人工叶片来评估GA (Grace et al., 1980;Dixon and Grace, 1983;Kitano and Eguchi, 1990;Leuning and Foster, 1990;Brenner and Jarvis, 1995;Grantz and Vaughn, 1999;Stokes et al., 2006;Katsoulas et al., 2007;木村等人,2016)。Katsoulas等人(2007)报道了通风条件下温室中GA的分布。然而,很少有关于封闭条件下GA的信息,这是冬季夜间加热温室的典型情况。在这种情况下,使用循环风机来保持空气条件的均匀性和作物冠层内的对流换热。在本研究中,利用电加热人工叶片对番茄冠层内的GA进行了连续和多点测量。绿化带内冠层GA的垂直和水平分布