胡优, 李敏, 任姮烨, 司炳成. 基于加热光纤分布式温度传感器的土壤含水率测定方法[J]. 农业工程学报, 2019, 35(10): 42-49. DOI: 10.11975/j.issn.1002-6819.2019.10.006
    引用本文: 胡优, 李敏, 任姮烨, 司炳成. 基于加热光纤分布式温度传感器的土壤含水率测定方法[J]. 农业工程学报, 2019, 35(10): 42-49. DOI: 10.11975/j.issn.1002-6819.2019.10.006
    Hu You, Li Min, Ren Hengye, Si Bingcheng. Measurement of soil water content using distributed temperature sensor with heated fiber optics[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2019, 35(10): 42-49. DOI: 10.11975/j.issn.1002-6819.2019.10.006
    Citation: Hu You, Li Min, Ren Hengye, Si Bingcheng. Measurement of soil water content using distributed temperature sensor with heated fiber optics[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2019, 35(10): 42-49. DOI: 10.11975/j.issn.1002-6819.2019.10.006

    基于加热光纤分布式温度传感器的土壤含水率测定方法

    Measurement of soil water content using distributed temperature sensor with heated fiber optics

    • 摘要: 为探讨加热光纤分布式温度传感技术测量土壤含水率不同方法的可行性,通过室内土槽试验,加热埋设于砂土的碳纤维光纤,利用分布式温度传感器测量不同含水率下沿光纤的温度变化,建立最大升温值、累积升温值和热导率与土壤含水率的关系,并比较这3种方法推求土壤含水率的测量精度。结果表明,光纤的温度波动随采样间距的增大或时间间隔的增大均减小,合理的采样间距和时间间隔设置能控制温度波动小于±0.1 ℃。在低(0~0.1 m3/m3)、中(>0.1~0.2 m3/m3)和高(>0.2~0.35 m3/m3)3个含水率水平,热导率法的测量精度均高于最大升温值法和累积升温值法,并且3种方法的测量精度均随含水率增加而降低;热导率法的均方根误差为0.015 m3/m3,低于最大升温值法(0.038 m3/m3)和累积升温值法(0.050 m3/m3)。研究对高时空分辨率精确获取田间尺度土壤墒情信息发展精准农业具有重要意义。

       

      Abstract: Abstract: Soil water content has great spatial-temporal variability, so accurate field-scale soil water content acquisition with high spatial-temporal resolution is of grave significance for precision agriculture. The distributed temperature sensing (DTS) technology combined with the principle of heat pulse probe is expected to achieve this goal; however, there isn't research to compare and evaluate the advantages and disadvantages of different methods to estimate soil water content using heated DTS technology. In this study, the indoor soil tank tests were carried on to heat the carbon-fiber optical cable embedded in sand, and the temperature variations along the fiber optics at different water content were measured by the DTS. The relationship between soil water content and maximum temperature rise, cumulative temperature rise and thermal conductivity were established, and the measurement accuracies of soil water content derived from the above mentioned 3 estimated methods were compared. The results showed that the temperature fluctuation of the fiber optics decreased with the increase of the sampling spacing or the time interval, and the reasonable sampling spacing and time interval could control the temperature fluctuation within a range between -0.1 and 0.1 ℃. The temperature rise value of fiber optics decreased with the increase of soil water content. The temperature rise was the highest for the dry sand and was the smallest when the soil was saturated. The maximum temperature rise and cumulative temperature rise had a similar trends with the change of water content, and decreased exponentially with the increase of water content. The slope of curve decreased gradually with the increase of water content, and the sensitivity to water content gradually reduced. However, there was an increased exponential relationship between thermal conductivity and water content. With the increase of water content, the slope of curve did not decrease obviously. In the whole range of water content of sand, thermal conductivity had a good sensitivity to water content. For thermal conductivity method, at the all range of water content, the scatter points between measured and predicted values were on or near the 1:1 line, showing good predictions. For the maximum temperature rise and cumulative temperature rise methods, the scatter points were all around the 1:1 line when the water content range was in the 0-0.1 m3/m3, which had better prediction results, while the water content range was in the 0.1-0.25 m3/m3, where the scatter points were below the 1:1 line, which wound underestimate the moisture content. When the water content range was greater than 0.25 m3/m3, the scatter points were mostly above the 1:1 line, which overestimated the moisture content. The measurement accuracy of the thermal conductivity method was higher than that of the maximum temperature rise method and of the cumulative temperature rise method regardless of the low (0-0.1 m3/m3), medium (>0.1-0.2 m3/m3) and high (>0.2-0.35 m3/m3) water content ranges. The measurement accuracies of the 3 methods decreased with the increase of water content. The root mean square error of the thermal conductivity method was 0.015 m3/m3, which was lower than that of the maximum temperature rise method (0.038 m3/m3) and the cumulative temperature rise method (0.050 m3/m3). All of the 3 methods could measure soil water content accurately, but the accuracy of thermal conductivity method was the highest. However, although the maximum temperature rise and cumulative temperature rise methods could achieve certain accuracy, they had no physical meanings, the relationships between those 2 and water content were influenced by many factors, such as fiber optics characteristics and physical properties of soil. The thermal conductivity method had physical significance and was only related to the physical properties of soil. Moreover, the relationship between thermal conductivity and water content had been studied, and a lot of thermal conductivity models have been developed, which provided a simple and feasible method for estimating water content through soil thermal conductivity. Therefore, it was very attractive to measure water content by the active heating fiber optics-DTS using thermal conductivity method. This study provides guidance for water content measurement methods using DTS. It is of great significance to develop high-time-resolution in-situ monitoring techniques for soil water content at different spatial scales, and the ultimate goal is to accurately understand the water content dynamics in the field to guide the precision irrigation.

       

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