Analysis of Incoherent Scatter Radar(ISR)data collected during an experiment involving alternating O/X mode pumping reveals that the high-frequency enhanced ion line(HFIL)and plasma line(HFPL)did not appear immediatel...Analysis of Incoherent Scatter Radar(ISR)data collected during an experiment involving alternating O/X mode pumping reveals that the high-frequency enhanced ion line(HFIL)and plasma line(HFPL)did not appear immediately after the onset of pumping,but were delayed by a few seconds.By examining the initial behaviors of the ion line,plasma line,and electron temperature,as well as ionosphere conditions,we find that(1)the HFIL and HFPL were delayed not only in the X mode pumping but also in the O mode pumping and(2)the HFIL was not observed prior to enhancement of the electron temperature.Our analysis suggests that(1)leakage of the X mode to the O mode pumping may not be ignored and(2)spatiotemporal uncertainties and spatiotemporal variations in the profiles of ion mass and electron density may have played important roles in the apparent failure of the Bragg condition to apply;(3)nevertheless,the absence of parametric decay instability(PDI)cannot be ruled out,due to our inability to match conditions caused by the spatiotemporal uncertainties.展开更多
CO2和H2O气体浓度是农田小气候的2个重要指标,一般采用CO2/H2O分析仪进行测定,为减少人为干扰,需使用气管将待测区域气体传输至分析器,而气管的材质及其长度会影响CO2/H2O测定时读数稳定所需的时间。本研究采用8种常用材质的气管及5种...CO2和H2O气体浓度是农田小气候的2个重要指标,一般采用CO2/H2O分析仪进行测定,为减少人为干扰,需使用气管将待测区域气体传输至分析器,而气管的材质及其长度会影响CO2/H2O测定时读数稳定所需的时间。本研究采用8种常用材质的气管及5种气管长度进行双因素随机区组试验,以筛选CO2/H2O测定所需的最佳气管材质及长度。结果表明:不同材质气管测定CO2浓度的稳定时间为9.20~11.47s,测定H2O气体浓度的稳定时间为9.67~18.93s。利用主效可加互作可乘(Additive main effects and multi-plicative interaction,AMMI)模型对CO2/H2O气体浓度达到稳定的时间进行方差分析和稳定性分析发现,在CO2浓度观测过程中,气管长度的固定效应导致的变异最大,材质次之,材质与长度互作效应较小;各材质中,CO2读数稳定时间最短的为蠕动泵管;在H2O气体浓度观测过程中,存在显著的材质和长度间的互作效应,其中材质的固定效应导致的变异最大,长度次之,PVC管的读数稳定时间最短。不同材质与不同长度的交互作用不同,每种材质对不同长度都有其特殊的适应性。因此,应根据测定指标,选择稳定时间短的材质和长度,以提高农田CO2和H2O气体浓度的测定效率。展开更多
文摘Analysis of Incoherent Scatter Radar(ISR)data collected during an experiment involving alternating O/X mode pumping reveals that the high-frequency enhanced ion line(HFIL)and plasma line(HFPL)did not appear immediately after the onset of pumping,but were delayed by a few seconds.By examining the initial behaviors of the ion line,plasma line,and electron temperature,as well as ionosphere conditions,we find that(1)the HFIL and HFPL were delayed not only in the X mode pumping but also in the O mode pumping and(2)the HFIL was not observed prior to enhancement of the electron temperature.Our analysis suggests that(1)leakage of the X mode to the O mode pumping may not be ignored and(2)spatiotemporal uncertainties and spatiotemporal variations in the profiles of ion mass and electron density may have played important roles in the apparent failure of the Bragg condition to apply;(3)nevertheless,the absence of parametric decay instability(PDI)cannot be ruled out,due to our inability to match conditions caused by the spatiotemporal uncertainties.
文摘CO2和H2O气体浓度是农田小气候的2个重要指标,一般采用CO2/H2O分析仪进行测定,为减少人为干扰,需使用气管将待测区域气体传输至分析器,而气管的材质及其长度会影响CO2/H2O测定时读数稳定所需的时间。本研究采用8种常用材质的气管及5种气管长度进行双因素随机区组试验,以筛选CO2/H2O测定所需的最佳气管材质及长度。结果表明:不同材质气管测定CO2浓度的稳定时间为9.20~11.47s,测定H2O气体浓度的稳定时间为9.67~18.93s。利用主效可加互作可乘(Additive main effects and multi-plicative interaction,AMMI)模型对CO2/H2O气体浓度达到稳定的时间进行方差分析和稳定性分析发现,在CO2浓度观测过程中,气管长度的固定效应导致的变异最大,材质次之,材质与长度互作效应较小;各材质中,CO2读数稳定时间最短的为蠕动泵管;在H2O气体浓度观测过程中,存在显著的材质和长度间的互作效应,其中材质的固定效应导致的变异最大,长度次之,PVC管的读数稳定时间最短。不同材质与不同长度的交互作用不同,每种材质对不同长度都有其特殊的适应性。因此,应根据测定指标,选择稳定时间短的材质和长度,以提高农田CO2和H2O气体浓度的测定效率。
