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100 Hz~3.98 MHz下蘋果虎皮病果實(shí)電特性研究
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Dielectric Properties of Fuji Apple Superficial Scald in the 100Hz~3.98MHz Range
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    摘要:

    為了研究富士蘋果虎皮病病果電特性的變化規(guī)律,,探討利用電特性參數(shù)的變化來(lái)反映蘋果內(nèi)部的物理化學(xué)變化,,運(yùn)用LCR型電子測(cè)量?jī)x測(cè)定了100Hz~3.98MHz頻率,、(20±1)℃恒溫條件下貯藏1,、8,、15,、22和29d的虎皮病果實(shí)復(fù)阻抗,、電抗,、電導(dǎo),、電容和介質(zhì)損耗系數(shù)等電學(xué)參數(shù),。結(jié)果顯示:在同一貯藏時(shí)間下,,隨著頻率的增加,果實(shí)的復(fù)阻抗,、電抗值在減小,,電導(dǎo)值則在增加;而電容和果實(shí)的介質(zhì)損耗系數(shù)變化則沒有規(guī)律性,。統(tǒng)計(jì)分析顯示,,感病果實(shí)和正常果實(shí)電容值村在極顯著差異(P<0.01)。結(jié)果表明:電容值基本可以正確反映蘋果的實(shí)際品質(zhì)情況,。

    Abstract:

    The change law of dielectric properties on Fuji apple superficial scald which stored at constant temperature was investigated. The mechanisms that reflected internal quality of fruit using dielectric properties were discussed so as to provide a new theoretical basis for nondestructive inspection and research methods to distinguish between diseased and normal fruits based on electrical properties. The fruits’ dielectric properties, which embraced the impedance, reactance, conductance, capacitance and loss coefficient, were determined with going up frequency from 100Hz to 3.98MHz at (20±1)℃ by applying LCR electronic measure instrument. The results showed that with the frequency increasing, fruit impedance and reactance were decreased; the capacitance and dielectric loss coefficient were changed irregularly, while the conductance was increased in spiral form under same storage times. There was a significantly positive correlation between impedance and reactance, the value of capacitance were significantly different (P<0.01) between the diseased and normal fruits from 100Hz to 3.98MHz. The research revealed that the capacitance could reflect the quality of apples in some extent. 

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馬海軍,馮美,張繼澍.100 Hz~3.98 MHz下蘋果虎皮病果實(shí)電特性研究[J].農(nóng)業(yè)機(jī)械學(xué)報(bào),2010,41(11):105-109. Dielectric Properties of Fuji Apple Superficial Scald in the 100Hz~3.98MHz Range[J]. Transactions of the Chinese Society for Agricultural Machinery,2010,41(11):105-109.

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