3 .結(jié)果和討論
3.1 .水的吸收和擴散系數(shù)
重量結(jié)果圖.1是壓裂性的水量是陰謀反對t1 / 2為.圖.2 ,水分含量測定傅里葉變換近紅外的不同樣品還介紹.
從最初的線性部分的曲線,水彌散系數(shù)可以計算的后續(xù)性方程:
其中重,w0和W ∞是重量的樣品浸泡時間中t ,t = 0和飽和平衡,電子商務(wù)是厚度的樣品,和D的水擴散系數(shù).在表1中,D和平衡水含量介紹.沒有太大的差異觀察功能的固化程度.
3.2 .體積變化在吸水
從傅里葉變換近紅外光譜在不同的浸泡時間是有可能的獲取信息的數(shù)量變化如下吸水.根據(jù)朗伯一比爾定律,吸光度在某波,阿,被吸收發(fā)生數(shù)目成正比吸收物種perunit節(jié).因此,一個3月2日應(yīng)的數(shù)量成正比,其中吸收物種分布.如果我們選擇一些具體的波紅外光譜的整潔樹脂,充分遠離吸收水分子,我們可以衡量分數(shù)體積變化使用以下表達式:
有在A0和吸光度的綜合參考頻帶4623厘米- 1 ,浸泡時間噸= 0和T ,ΔV/V0the分數(shù)體積變化下列吸水.圖.3 ,體積變化的分數(shù)是陰謀反對浸泡時間.
英語翻譯
英語翻譯
3.Results and discussion
3.1.Water uptake and diffusion coefficients
Gravimetric results are presented in Fig.1 were the frac-tional amount of water is plotted against t1/2.In Fig.2,the water content measured by FT-NIR for the different samples is also presented.
From the initial linear portion of the curves,water diffu-sion coefficients can be calculated according to the follow-ing equation:
where wt,w0 and w∞ are the weights of the samples at immersion time t,t=0 and at the saturation equilibrium,e is the thickness of the sample,and D the water diffusion coefficient.In Table 1,D and the equilibrium water content are presented.No great differences are observed in function of curing degree.
3.2.Volume change during water uptake
From FT-NIR spectra at different immersion times it is possible to obtain information on the volume change following water uptake.According to the Lambert–Beer law,absorbance at a certain wavenumber,A,were absorption takes place is proportional to the number of absorbing species perunit section.Therefore,A−3/2 should be proportional to the volume in which the absorbing species are distributed.If we select some wavenumber specific of the IR spectrum of the neat resin,sufficiently far away from absorption of water molecules,we can measure the fractional volume change using the following expression:
were A0 and At are the integrated absorbances of the reference band at 4623 cm−1 at immersion times t=0 and t,ΔV/V0the fractional volume change following water uptake.In Fig.3,the fractional volume change is plotted against immersion time.
別用翻譯軟件。那我也會
3.Results and discussion
3.1.Water uptake and diffusion coefficients
Gravimetric results are presented in Fig.1 were the frac-tional amount of water is plotted against t1/2.In Fig.2,the water content measured by FT-NIR for the different samples is also presented.
From the initial linear portion of the curves,water diffu-sion coefficients can be calculated according to the follow-ing equation:
where wt,w0 and w∞ are the weights of the samples at immersion time t,t=0 and at the saturation equilibrium,e is the thickness of the sample,and D the water diffusion coefficient.In Table 1,D and the equilibrium water content are presented.No great differences are observed in function of curing degree.
3.2.Volume change during water uptake
From FT-NIR spectra at different immersion times it is possible to obtain information on the volume change following water uptake.According to the Lambert–Beer law,absorbance at a certain wavenumber,A,were absorption takes place is proportional to the number of absorbing species perunit section.Therefore,A−3/2 should be proportional to the volume in which the absorbing species are distributed.If we select some wavenumber specific of the IR spectrum of the neat resin,sufficiently far away from absorption of water molecules,we can measure the fractional volume change using the following expression:
were A0 and At are the integrated absorbances of the reference band at 4623 cm−1 at immersion times t=0 and t,ΔV/V0the fractional volume change following water uptake.In Fig.3,the fractional volume change is plotted against immersion time.
別用翻譯軟件。那我也會
英語人氣:438 ℃時間:2020-04-06 07:14:16
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