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Study of effective factors in detection of irradiated food using thermoluminescence based on the models of reference minerals

机译:基于参考矿物模型的热致发光检测辐照食品的有效因素研究

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In the thermoluminescence (TL) detection method for irradiated foods, accurate standards have been developed for detecting irradiated foods. The standard method describes that emission maximum temperature (T1i) and TL ratio for non-heated or non-mixed sample can be in the range of 150-250 °C and more than 0.1, respectively, when it was irradiated food. But when irradiated food is heated up to 200 °C, or mixed up with non-irradiated stuffs, T1i and TL ratio would not drop in the range. Here we examined the effects of the two processes, heating and mixing with non-irradiated food, on T1i and G1/G1k ratio (ratio of G1 and average G1 for 1 -kGy-irradiated JF2, this value is modeled after TL ratio) using a model consisting of irradiated and non-irradiated geochemical standards of feldspar (JF1, JF2, PF, etc.). T1i temperatures for irradiated JF1, JF2, and PF ranged from 163 to 175 °C, while those for the non-irradiated JF2 ranged from 253 to 263 °C. T1i temperatures for 5-kGy-irradiated and preheated JF2 for 10 s, 20 s, and 30 s at 180 °C were 215, 225, and 231 °C, respectively. When JF2 was irradiated from 100 Gy to 5 kGy, the T1i was almost constant at any doses. G1/G1k ratios at 100,200, and 500 Gy were 0.15, 0.23, and 0.60, respectively. Gl/Glk ratio was proportional to the given dose at the integration temperature ranges. The TS sample, which originated from farm soil in Tanegashima Island, gave the same results as JF2. T1is for 5-kGy-irradiated and preheated JF2 for 20 s at 150,180, and 200 °C were 197, 225, and 246 °C, respectively. Longer and higher preheating resulted in higher T1i. Longer and higher preheating extremely reduced the G1/G1k ratio, and in some cases the ratio was less than 0.1. This means TL ratio is useless in determination of the standard for irradiated food. Peak temperatures for JF2 in mixture of 5-kGy-irradiated to non-irradiated (1.25-5%) were 261-263 °C (non-irradiated portion, T1n) and 177-180 °C (irradiated portion T1i). The peak positions are almost the same as those of original components and would not be affected by the mixing ratio. But TL ratio could not be used to determine irradiated food because mixing would reduce it remarkably. Some of the glow curves were simulated by a computer program. In conclusion, T1i is a key factor in an irradiated food determination practice for sample containing feldspar, rather than TL ratio.
机译:在辐照食品的热致发光(TL)检测方法中,已经开发了用于检测辐照食品的准确标准。标准方法描述了当辐照食品时,未加热或未混合样品的最高发射温度(T1i)和TL比可以分别在150-250°C和大于0.1的范围内。但是,当将辐照食品加热至200°C或与非辐照物料混合时,T1i和TL比不会在该范围内下降。在这里,我们检查了加热和与非辐照食品混合这两个过程对T1i和G1 / G1k比率(1-kGy辐照的JF2的G1与平均G1的比率,此值是根据TL比率建模的)的影响。由长石的辐照和非辐照地球化学标准品(JF1,JF2,PF等)组成的模型。辐照过的JF1,JF2和PF的T1i温度范围为163至175°C,而非辐照过的JF2的T1i温度范围为253至263°C。在180°C下进行5 kGy辐照和预热的JF2在10 s,20 s和30 s下的T1i温度分别为215、225和231°C。当从100 Gy到5 kGy照射JF2时,T1i在任何剂量下都几乎恒定。 100,200和500 Gy时的G1 / G1k比分别为0.15、0.23和0.60。 G1 / Glk比与积分温度范围内的给定剂量成比例。 TS样品来源于种子岛的农场土壤,其结果与JF2相同。在150,180和200°C下,5-kGy辐射和预热JF2在20 s时的T1是197、225和246°C。更长和更高的预热导致更高的T1i。更长的时间和更高的预热极大地降低了G1 / G1k比率,在某些情况下该比率小于0.1。这意味着在确定辐照食品标准时,TL比是无用的。在被5-kGy照射至未照射(1.25-5%)的混合物中,JF2的峰值温度为261-263°C(未照射部分,T1n)和177-180°C(照射部分T1i)。峰位置几乎与原始组分的峰位置相同,并且不受混合比例的影响。但是TL比不能用于确定辐照食品,因为混合会显着降低辐照度。一些辉光曲线是通过计算机程序模拟的。总之,对于含有长石而不是TL比的样品,T1i / n是辐照食品测定实践中的关键因素。

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