李文采, 田寒友, 白京, 王辉, 邹昊, 乔晓玲. 采用压汞法研究不同冷冻羊肉冰晶结构特征[J]. 农业工程学报, 2019, 35(20): 280-287. DOI: 10.11975/j.issn.1002-6819.2019.20.034
    引用本文: 李文采, 田寒友, 白京, 王辉, 邹昊, 乔晓玲. 采用压汞法研究不同冷冻羊肉冰晶结构特征[J]. 农业工程学报, 2019, 35(20): 280-287. DOI: 10.11975/j.issn.1002-6819.2019.20.034
    Li Wencai, Tian Hanyou, Bai Jing, Wang Hui, Zou Hao, Qiao Xiaoling. Investigation of ice crystal structure characteristics of different frozen lamb by using mercury intrusion[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2019, 35(20): 280-287. DOI: 10.11975/j.issn.1002-6819.2019.20.034
    Citation: Li Wencai, Tian Hanyou, Bai Jing, Wang Hui, Zou Hao, Qiao Xiaoling. Investigation of ice crystal structure characteristics of different frozen lamb by using mercury intrusion[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2019, 35(20): 280-287. DOI: 10.11975/j.issn.1002-6819.2019.20.034

    采用压汞法研究不同冷冻羊肉冰晶结构特征

    Investigation of ice crystal structure characteristics of different frozen lamb by using mercury intrusion

    • 摘要: 为研究不同冷冻羊肉冰晶结构特征,该文以空气冷冻和液浸冷冻2种不同冷冻方式以及冻贮3和90 d不同时间的冷冻羊肉为研究对象,采用真空冷冻干燥法将冷冻羊肉体内冰晶升华,用压汞法对冰晶升华留下的孔隙结构进行测定,并观察解冻复温后肌肉微观组织结构。研究结果表明,压汞法可有效测定冷冻羊肉冰晶升华后留下的孔隙分布特征,以此来表征冰晶结构特征。通过比较空气冷冻和液浸冷冻后冻贮不同时间羊肉的孔隙结构以及解冻复温后肌纤维组织结构变化特点,发现不同冷冻羊肉冰晶升华后孔隙分布特征存在差异,空气冷冻后冻贮3和90 d以及液浸冷冻后冻贮3和90 d的冷冻羊肉最大累计进汞量分别为2.16±0.08、2.33±0.07、1.76±0.01和2.29±0.05 mL/g,孔隙平均直径为10.09±0.30、25.73±0.91、3.21±0.46和14.45±0.64 µm,存在显著差异(P<0.05),迂曲度分别为2.27±0.05、3.88±0.05、3.15±0.08和4.41±0.16,存在显著差异(P<0.05)。该研究结果可为压汞法在冷冻肉冰晶结构参数的测定应用中提供一定的理论依据。

       

      Abstract: In order to prove the feasibility of measuring the structure of ice crystal based on mercury intrusion, in this study, fresh lamb were either stored for 3 and 90 days after air freezing or stored for 3 and 90 days after immersion freezing. Ice crystal formed in the frozen meat wasare characterized as indicators for selectingof optimalthe fitness of the freezing methods and storing time on lamb., Ttherefore, the drop rate of central temperature during freezing, the characteristics of ice crystals, and the morphology of muscle fibers were recorded during different freezing processes and different frozen and stored times, and the microstructures of ice crystals formed were analyzed for cross-section area, equivalent diameter, roundness and elongation, ice size, shape, and location., Tthese factors were evaluated and compared with cumulative intrusion, distribution of pores and tortuosity that were measured by mercury intrusion. The mean (±standard deviation) cross-section area of ice crystals were 2 076.15±1 756.22, 555.41±526.72, 637.63±556.58 µm2 for the lamb samples subjected to stored 90 days after air freezing and stored for 3 and 90 days after immersion freezing, respectively. Aas compared with the muscle fibers (1 978.12±1 092.27µm2) that stored 3 days after air freezing. The roundness of the ice crystals formed in frozen lamb that stored 90 days after air freezing and stored for 3 and 90 days after immersion freezing was 0.65±0.17, 2.47±0.78 and 1.92±0.61, respectively, while the roundness of the frozen lamb that stored for 3 days was 0.73±0.14. The elongation of the ice crystals formed in frozen lamb that frozen and stored 90 days after air freezing and stored for 3 and 90 days after immersion freezing was 2.70±1.39, 2.47±0.78 and 1.92±0.61, respectively, while the roundness of the frozen mutton that stored for 3 days was 1.95±0.70. Air freezing, which finished the ice formation process within 549.5 min, created larger and irregular ice crystals, which resulted in severe and irreversible damage to lamb muscles. Immersion freezing produced smaller ice crystals than air freezing and finished the freezing process at a higher speed within 80.5 min. The quick process and short storage created finer ice crystals than long storage and air freezing, while the integrity of muscle fibers remained intact relatively. Because the pores left in the muscle that correspond to the space of the original ice crystals, therefore, the cumulative intrusion, aperture of pores, log differential intrusion and tortuosity of mutton samples were also recorded during different freezing processes after vacuum and freeze-drying. The mean (±standard deviation) maximum cumulative intrusion of pores were 2.16±0.08, 2.33±0.07, 1.76±0.01, 2.29±0.05 mL/g for the mutton samples subjected to be stored for 3 and 90 days after air freezing and stored for 3 and 90 days after immersion freezing, respectively. The distribution of pores showed that the large pores and middle holes were the main pores among different frozen muttons, and the frozen lamb samples that were stored long time have more large pores, middle holes and small holes than the frozen lamb samples that were stored short time. The average aperture dimension of pores were 10.09, 25.73, 3.21 and 14.45µm for the mutton samples subjected to be stored for 3 and 90 days after air freezing and stored for 3 and 90 days after immersion freezing, respectively. The tortuosity of pores were 2.27±0.05, 3.88±0.05, 3.15±0.08 and 4.41±0.16 for the lamb samples subjected to be stored for 3 and 90 days after air freezing and stored for 3 and 90 days after immersion freezing, respectively. The variation trend of maximum cumulative intrusion, distribution of pores and tortuosity were basically consistent with analysis of ice crystals of freeze-sectioning. Results achieved in this research provide mercury intrusion is a useful technical support for ice crystals.

       

    /

    返回文章
    返回