欢迎登录材料期刊网

材料期刊网

高级检索

合成了高固体含量(〉85%)的线性酚醛树脂,经凝胶渗透色谱/多角度激光光散射(SEC/MALLS)联用仪测定其数均分子量为1577,且分子量分布范围较窄,-Mw/-Mn仅为1.127。采用差示扫描量热(DSC)分析技术在50℃~300℃温度范围内,以不同的升温速率(2.5℃/min、5℃/min、7.5℃/min和10℃/min)研究了该酚醛树脂的固化反应过程。结果表明,该高固体含量线性酚醛树脂的凝胶化温度Tgel=110.61℃,固化温度Tcure=129.14℃,后处理温度Ttreat=146.96℃;根据Kissinger方程、Ozawa方程和Crane方程以及n级动力学模型确定该树脂的固化动力学方程为dα(t)/dt=2.09×1017(1-α)0.95exp(-2.10235×104/T)。

Novolac-type resin with high solid content(85%) was synthesized,of which number average molecular weight is 1577 and distribution is narrow.The curing process was studied by differential scanning calorimetry(DSC) at different heating rates of 2.5 ℃/min,5 ℃/min,7.5 and 10 ℃/min between 50 ℃~300 ℃.The gelation temperature,curing temperature and post processing temperature of the resin are 136.68 ℃,163.16 ℃ and 197.39 ℃ respectively.According to Kissinger equation,Ozawa equation,Crane equation and the n-level kinetic model,the curing kinetic equation is dα(t)/dt=2.09×1017(1-α)0.95exp(-210235×103/T).

参考文献

[1] 高月静,李郁忠,寇晓康,郑宏军.高固体含量酚醛树脂的固化特征及动力学研究[J].高分子材料科学与工程,1999(03):45-47.
[2] 周大鹏.DSC法研究不同邻对位比值酚醛树脂的固化行为[J].高分子材料科学与工程,2008(10):131-133,137.
[3] Lee YK.;Kim DJ.;Kim HJ.;Hwang TS.;Rafailovich M.;Sokolov J. .Activation energy and curing behavior of resol- and novolac-type phenolic resins by differential scanning calorimetry and thermogravimetric analysis[J].Journal of Applied Polymer Science,2003(10):2589-2596.
[4] Perez, JM;Oliet, M;Alonso, MV;Rodriguez, F .Cure kinetics of lignin-novolac resins studied by isoconversional methods[J].Thermochimica Acta: An International Journal Concerned with the Broader Aspects of Thermochemistry and Its Applications to Chemical Problems,2009(1/2):39-42.
[5] de Medeiros ES.;Agnelli JAM.;Joseph K.;de Carvalho LH.;Mattoso LHC. .Curing behavior of a novolac-type phenolic resin analyzed by differential scanning calorimetry[J].Journal of Applied Polymer Science,2003(6):1678-1682.
[6] 程广文,范晓东,周志勇,田威.凝胶渗透色谱-多角度激光散射测定聚乙二醇分子量[J].高分子材料科学与工程,2008(10):127-130.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%