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研究生:王贊森
研究生(外文):Wang, Tsan-Sen
論文名稱:稠溶液之黃豆11S球蛋白受溫度剪力及超音波作用後物化特性之影響
論文名稱(外文):The physico-chemical changes of soy 11S globulin in concentration solution after heating, shearing and ultrasonic treatments.
指導教授:陳榮輝陳榮輝引用關係
指導教授(外文):Chen Rong-Huei
學位類別:碩士
校院名稱:國立海洋大學
系所名稱:水產食品科學系
學門:農業科學學門
學類:食品科學類
論文種類:學術論文
論文出版年:1997
畢業學年度:85
語文別:中文
論文頁數:114
中文關鍵詞:稠溶液黃豆11S球蛋白溫度剪力超音波物化特性
外文關鍵詞:concentration solutionsoy 11S globulintemperatureshearultrasonicphysico-chemical
相關次數:
  • 被引用被引用:3
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本研究探討稠溶液黃豆 11S 球蛋白經不同條件之熱、剪力、超音波單獨
或合併作用後對其物化特性之影響。物化特性之探討包括表面疏水性、平
均粒徑大小、二級結構和動黏彈性質。黃豆 11S 球蛋白磷酸鹽緩衝液(
pH 7.6, μ﹦0.5)之稠溶液定濃度為 10%。結果顯示:稠溶液之黃豆
11S 球蛋白經過加熱處理後,其表面疏水性、平均粒徑大小會隨加熱溫度
的上升及加熱時間的增加而變大,經長時間 60分鐘的 70、80、90℃ 加
熱處理者其二級結構之 α-螺旋的含量由原本(未加熱處理)的 11 %
分別增加至約 24、25、29 %,而動黏彈性之損失因子則隨加熱溫度和作
用時間的增加而下降。剪力處理會使稠溶液之黃豆 11S 球蛋白之表面疏
水性及平均粒徑大小隨剪力作用時間及剪速率上升而增加,且經過掬力處
理之後,二級結構之 α-螺旋及 β-褶板的含量皆有增加的現象,且以
越大之剪速率作用越久,黃豆 11S 球蛋白中規則之二級結構的比例變成
愈高,而動黏彈性質之損失因子亦會隨剪率和作用時間的增加而下降。超
音波處理亦會使稠溶液之黃豆 11S 球蛋白之表面疏水性隨超音波作用時
間及超音波輸出功率的上升而增加,而平均粒徑大小在功率180、300
Watt 之超音波作用 5 分鐘時會有下降的趨勢,但 420 Watt 之超音波作
用 5 分鐘則會上升,經過超音波作用後之黃豆 11S 球蛋白的二級結構之
α-螺旋及 β-褶板之含量均較未作用者高,且超音波功率越高、作用
時間越久者,二級結構中規則的比例變得愈高,而動黏彈性中之損失因子
則亦隨超音波輸出功率和作用時間的增加而下降。 合併剪力與加熱處理
,會使稠溶液之黃豆 11S 球蛋白之表面疏水性及平均粒徑大小隨剪速率
及溫度的上升而增加,但單獨受剪力處理者之表面疏水性大於剪力合併加
熱處理者大於單獨加熱處理者。而平均粒徑則為單獨加熱 60 分鐘處理者
最大,剪力合併加熱處理 5 分鐘者次之,單獨剪力處理 10 分鐘者最小
。且經剪力合併加熱處理後,其二級結構之 α﹣螺旋及 β﹣褶板之含量
有增加的現象,且於越高的溫度下受愈高之剪速率作用者,二級結構中之
規則的比例亦越高。而動黏彈性之損失因子則隨剪速率和加熱溫度的增加
而下降。 合併超音波與加熱處理,會使稠溶液之黃豆 11S 球蛋白之表面
疏水性及平均粒徑大小隨超音波功率及溫度的上升而增加,超音波合併加
熱處理者之表面疏水性約略等於單獨超音波處理者大於單獨加熱處理者。
而平均粒徑則為單獨加熱處理 60 分鐘者最大,超音波合併加熱處理 10
分鐘者次之,單獨超音波處理 10 分鐘者最小。且經超音波合併加熱處理
後,其二級結構之 α﹣螺旋及 β﹣褶板之含量有增加的現象,且於越高
的溫度下施行愈高功率之超音波處理,黃豆 11S 球蛋白中規則之二級結
構比例亦變成越高。而動黏彈性之損失因子則隨超音波功率和加熱溫度的
增加而下降。
The objective of this study is to elucidate the effect of
single or combined physical treatments on the physical property
changes of the concentration soy 11S globulin solution. The
physical treatments include heating, shearing and ultrasonic
radiation whereas the physical properties interested are surface
hydrophobicity, average particle size , secondary structure and
dynamic properties. The concentration of soy 11S globulin
solution is 10%soy 11S globulin dispersion in phosphate buffer
pH 7.6, μ﹦0.5. The results show surface hydrophobicity,
average particle size of soy 11S globulin increased with
increased heating temperature and heating time. α-helix
content increased from 11% for unheated to 24, 25 and 29% for
those heated at 70, 80 and 90℃for 30 min, respectively. Loss
tangent angle, one of the dynamic properties, decreased with
increasing heating temperature and heating time. Shear treatment
resulted in increasing surface hydrophobicity, and increasing
average particle size of soy 11S globulin in concentration
solution. The increase was proportional to the increase of shear
rate and shear time. The proportion of orderly secondary
structureα-helix andβ-sheet increased with increasing shear
rate and treatment time. Loss tangent angle decreased with
increasing shear rate and shearing time. Ultrasonic radiation
treatment resulted in increased surface hydrophobicity of soy
11S globulin in concentrated solution. The increase was
proportional to the power and duration of ultrasonic radiation.
Average particle size of soy 11S globulin in concentrated
solution decreased after ultrasonic treatment at 180 Watt or 300
Watt for 5 min, however average particle size increased after
ultrasonic at 420 Watt for 5 min. Orderly secondary structure of
α-helix orβ-sheet of soy 11S globulin increased with
increasing power and duration of ultrasonic treatment. However
loss tangent angle decreased in proportion to the increase of
power and duration of ultrasonic treatment. Combined heating and
shearing treatment on concentrated soy 11S globulin solution
resulted in increasing its surface hydrophobicity and average
particle size. The increase were proportional to the heating
temperature and shear rate employed . The magnitude of increase
in surface hydrophobicity of soy 11S globulin subjected to
difference treatments were in order of shear treatment alone
larger than combined heating and shearing in turn larger than
heating treatment alone. The order of increasing in average
particle size were in order of heating alone for 60 min higher
than combined shear and heating for 5 min in turn larger than
shear alone for 10 min. Orderly secondary structure increased
after combined heating and shearing. The increase were higher
for those subjected to higher temperature and higher shear rate
treatment. The loss tangent angle decreased with increasing
shear rate and heat temperature employed. Combined heating and
ultrasonic radiation treatment resulted in increasing surface
hydrophobicity and average particle size of treated soy 11S
globulin in concentrate solution. The increase was proportional
to the increase in temperature and ultrasonic radiation power.
Increase in surface hydrophobicity resulted from combined
heating and ultrasonic radiation was almost equal to ultrasonic
treatment alone but higher that or than heat treatment alone.
Increase in average particle size resulted from treatments were
in order of heating alone for 60 min larger than combined
heating and ultrasonic for 10 min in turn larger than ultrasonic
treatment alone for 10 min. Increase in orderly secondary
structure α-helix andβ-sheet were proportional to heating
temperature and ultrasonic radiation power used. The higher the
temperature and the higher the power of ultrasonic radiation,
the higher proportion of orderly secondary structure in soy 11S
globulin resulted so as the decease in loss tangent angle after
combined treatment.
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