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Relationship Between Negative Air Ion Generation by Plants and Stomatal Characteristics Under Stimulation of Pulsed Electrical Field
Wu Renye, Sun Yuanfen, Zheng Jingui, Deng Chuanyuan, Ye Dapeng, Wang Qingshui
Chinese Bulletin of Botany    2017, 52 (6): 744-755.   DOI: 10.11983/CBB16242
Abstract   (1317 HTML17 PDF(pc) (641KB)(1161)  

Under normal conditions, the capacity of plants to generate negative air ions (NAIs) is very weak. However, stimulation of a pulsed electrical field can result in substantial improvement of the ability for NAI generation. We examined NAI generation in Stromanthe sanguinea, Calathea zebrina, and Hippeastrum rutilum in glass chambers under the natural state and under pulsed electrical field and light stimulation and analyzed the shape of stomata. We found variation in NAI generation by plants due to the different combined parameters of the pulsed electrical field. Each plant has its own optimal pulsed electrical field with a combination of parameters for efficient NAI generation: S. sanguinea with A3B3C3 (A3, U=1.5×104 V; B3, T=1.5 s; C3, τ =65 ms), C. zebrina with A3B4C1 (A3, U=1.5×104 V; B4, T=2.0 s; C1,τ =5 ms) and H. rutilum with A4B4C1 (A4, U=2.0×104 V; B4, T=2.0 s; C1, τ=5 ms). With the application of a pulsed electrical field to plants, the higher the voltage, the greater the capacity for NAI generation. With enhanced light intensity, the ability to generate NAI significantly increased with application of a pulsed electrical field. Without the pulsed electrical field, despite the slightly increased NAI concentration with increasing light intensity, NAI concentration did not differ (P>0.05). Finally, NAI generation was closely related to the characteristics of leaf stomata. Furthermore, a greater degree of stomatal opening and stomatal density was associated with stronger capacity to generate NAI.


Treatment Factors Average of negative air ions concentration (ion·cm-3)
A B C P0 P4 P6 P7
A1B1C1 8 0.5 5 36±3 a 452644±21866 n 91±6 a 8605±983 f
A1B2C3 8 1.0 65 38±2 a 471667±21881 n 92±8 a 9581±948 f
A1B3C4 8 1.5 90 39±2 a 535311±25007 l 94±5 a 8559±874 f
A1B4C2 8 2.0 35 44±2 a 494667±27146 m 98±8 a 8832±543 f
A2B1C4 10 0.5 90 39±2 a 795822±53569 k 95±9 a 20200±1478 f
A2B2C2 10 1.0 35 38±2 a 822267±54244 j 88±8 a 22473±1381 f
A2B3C1 10 1.5 5 37±3 a 813022±50909 jk 85±7 a 23236±2467 f
A2B4C3 10 2.0 65 41±3 a 872734±55664 i 91±4 a 21801±1643 f
A3B1C2 15 0.5 35 105±2 a 1564444±119680 d 226±20 a 181311±20261 e
A3B2C4 15 1.0 90 107±2 a 1628244±191548 c 250±40 a 218444±33270 c
A3B3C3 15 1.5 65 109±3 a 1730800±195344 a 233±16 a 191867±32167 de
A3B4C1 15 2.0 5 107±2 a 1670933±187634 b 262±28 a 208067±34590 cd
A4B1C3 20 0.5 65 130±2 a 1186667±103135 f 170±39 a 301933±30237 b
A4B2C1 20 1.0 5 129±5 a 1264000±117184 e 179±18 a 330356±30322 a
A4B3C2 20 1.5 35 134±3 a 1136800±83461 g 215±33 a 322644±29865 ab
A4B4C4 20 2.0 90 140±4 a 1038133±83109 h 164±51 a 318156±36925 ab
Table 4 Analysis of negative air ions concentration generated by plants upon different combinational parameters of pulsed electrical stimulation (means±SD)
Extracts from the Article
不同强度的脉冲电场对盆土释放负离子的作用很小(36-140 ion·cm-3), 处理间均无显著差异(表4)。紫背竹芋在不同强度脉冲电场作用下, 释放负离子的能力存在差异, 浓度均值为452 644-1 730 800 ion·cm-3 (表4)。A3B3C3处理下的负离子浓度均值最高, 是常态下释放能力(未刺激)的22 773.7倍。负离子浓度最低的处理为A1B1C1, 浓度均值为452 644 ion·cm-3, 是其常态下释放能力的5 955.8倍。方差分析表明, 紫背竹芋高效释放负离子的最优处理为A3B3C3。在该强度脉冲电场作用下, 其释放负离子能力的倍增效应最为显著。
表4
绒叶肖竹芋释放负离子的浓度均值为85-262 ion·cm-3 (表4), 以A3B4C1处理下负离子的释放能力最强, 是其常态下释放能力的3.2倍。而以A2B3C1作用下的释放能力最弱, 仅为85 ion·cm-3, 与自然状态下的释放能力(81 ion·cm-3)相近。尽管各处理绒叶肖竹芋释放负离子的能力不同, 但各处理间均无显著差异。方差分析表明, 仅脉冲电压对其释放负离子的能力存在显著影响(P<0.05)。验证性实验表明, A3B4C1为绒叶肖竹芋高效释放负离子最佳脉冲电场的组合参数。
朱顶红释放负离子的浓度均值为8 559-330 356 ion·cm-3 (表4), 以A4B2C1作用下的释放能力最强, 是其常态下的4 404.7倍, 与其它各处理均呈显著差异(P<0.05)。释放负离子能力最小的是A1B3C4, 为8 559 ion·cm-3, 是其常态下的114.1倍。方差分析表明, 脉冲电压、脉冲间隔和脉冲宽度均对其释放负离子的浓度具有显著的影响(P<0.05)。验证性实验表明, A4B4- C4是其高效释放负离子的最佳脉冲电场组合参数, 浓度均值为330 356 ion·cm-3。
与自然状态下各植物释放负离子的能力相比, 施加不同强度的脉冲电场, 植物释放负离子的浓度有不同程度的提高。除绒叶肖竹芋外, 紫背竹芋和朱顶红释放负离子的能力在不同强度脉冲电场作用下均存在显著差异(P<0.05) (表4)。
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