Phase-transformation kinetics in triphasic cordierite gel

2001 ◽  
Vol 16 (2) ◽  
pp. 451-458 ◽  
Author(s):  
R. Petrović ◽  
Dj. Janacković ◽  
S. Zec ◽  
S. Drmanić ◽  
Lj. Kostić-Gvozdenović

A triphasic cordierite-type gel was prepared from silica sol, boehmite sol, and an aqueous solution of Mg(NO3)2 · 6H2O. The silica sol was obtained from water glass by the ion exchange method, while boehmite sol was obtained by peptization of freshly prepared Al(OH)3. Phase transformations occurring in the gel were studied by differential scanning calorimetry, x-ray diffractometry, and Fourier transform infrared spectrometry. Spinel was observed to crystallize from the gel prior to cristobalite; their reaction subsequently yielded α-cordierite. At higher temperatures, α-cordierite transformed into modulated β-cordierite. Kinetic parameters of α-cordierite formation and α-cordierite to modulated β-cordierite transformation were determined by differential scanning calorimetry under nonisothermal conditions. Formation of a-cordierite was found to be a diffusion-controlled process, with an overall activation energy of Ea = 1242 ± 66 kJ/mol. During the α → β-cordierite transformation, a modulated phase was formed by surface transformation of α-cordierite. The overall activation energy for the formation of the modulated structure is Ea = 583±77 kJ/mol.

2014 ◽  
Vol 988 ◽  
pp. 31-35
Author(s):  
Jia Le Song ◽  
Chan Chan Li ◽  
Zhi Mi Zhou ◽  
Chao Qiang Ye ◽  
Wei Guang Li

Curing kinetics of MEP-15/593 system and MEP-15/593/660 system is studied by means of differential scanning calorimetry (DSC). Curing kinetic parameters are evaluated and the relationship between diluent 660 and the curing properties is investigated. The results show that the diluent 660 can not only reduce viscosity and activation energy, but also improve the degree of cure and conversion ratio.


e-Polymers ◽  
2006 ◽  
Vol 6 (1) ◽  
Author(s):  
Newton Luiz Dias Filho ◽  
Hermes Adolfo de Aquino

AbstractNon-isothermal dielectric analysis (DEA) and differential scanning calorimetry (DSC) techniques were used to study the epoxy nanocomposites prepared by reacting 1,3,5,7,9,11,13,15-octa[dimethylsiloxypropylglycidylether] pentaciclo [9.5.1.13,9.15,15 .17,13] octasilsesquioxane (ODPG) with methylenedianiline (MDA). Loss factor (ε”) and activation energy were calculated by DEA. The relationships between the loss factor, the activation energy, the structure of the network, and the mechanical properties were investigated. Activation energies determined by DEA and DSC, heat of polymerization, fracture toughness and tensile modulus show the same profile for mechanical properties with respect to ODPG content.


1982 ◽  
Vol 15 ◽  
Author(s):  
Dean E. Peterson ◽  
Frank W. Clinard

ABSTRACTSamples of CaPuTi2O7 were prepared by cold pressing and sintering. Plutonium was substituted for zirconium in order to characterize radiation damage effects. The energy stored in a sample which had reached saturation in swelling after storage at ambient temperature was measured with a differential scanning calorimeter. The total energy of 6.6±0.1 cal/g is released over the range 485–715° C. The activation energy of annealing of the damage is 1.22±0.05 eV. The temperature dependence of the rate constant is described by kT= 5.96E4 exp(−1.22/kBT) s−1 where kB and T are the Boltzmann's constant and temperature(K) respectively. A sample stored at 600°C was similarly evaluated and showed no release of stored energy to the precision of the apparatus (±0.1 cal/g). These results are applied to analysis of waste incorporation in Synroc and are correlated with analogous parameters for other materials.


2008 ◽  
Vol 570 ◽  
pp. 120-125
Author(s):  
R.M. Ribeiro ◽  
R.S. de Biasi ◽  
D.R. dos Santos ◽  
Dílson S. dos Santos

Crystallization of the amorphous metallic alloy Fe73.5 Cu1Nb3 Si8.5 B14 was investigated by ferromagnetic resonance (FMR), small angle in situ X-ray scattering (SAXS/WAXS) and differential scanning calorimetry (DSC). Only one crystalline phase was observed by WAXS and only one peak was observed by DSC. The activation energies, calculated from FMR and DSC data, were 287 kJ.mol-1 and 313.4 kJ.mol-1, respectively. The values calculated for the Avrami exponent were 0.98 (FMR) and 1.4 (DSC). These values correspond to different mechanisms of nucleation and growth; however, the SAXS /WAXS results suggest that the dominant mechanisms are nucleation and growth of crystals from small dimensions.


2014 ◽  
Vol 508 ◽  
pp. 110-113
Author(s):  
Rong Hua Zhang ◽  
Biao Wu ◽  
Xiao Ping Zheng

The temperature and duration of β1→α+β2 transformation of Ti-6Al-4V alloy in cooling process were measured by differential scanning calorimetry, and transformation activation energy and Avrami exponent of β1→α+β2 were also calculated. The results show that the cooling rate is in the range of 在5~20°C/min, the transformation temperature and the transformation duration β1→α+β2 transformation of Ti-6Al-4V alloy decreased with the increasing cooling rate, its transformation activation energy decreased with the increasing phase transformation volume fraction, and Avrami exponent was between 1 and 2 at 660°C.


2011 ◽  
Vol 688 ◽  
pp. 180-185
Author(s):  
Yu Zhang ◽  
Wei Lu ◽  
Biao Yan ◽  
Yu Xin Wang ◽  
Ying Yang

The nanocrystallization kinetics of the Fe81Si3.5B13.5C2amorphous alloy was investigated by differential scanning calorimetry (DSC). The apparent activation energy Ea, as well as the nucleation and growth kinetic parameters has been calculated by Kissinger and Ozawa methods. The changeable activation energy Eawith crystalline fraction α was obtained by the expended Friedman method without assuming the kinetic model function, and the average value of Eawas 364±20 kJ/mol. It was shown that the crystallization mechanism of initial stage (0<α<0.7) of the transformation was bulk crystallization with two and three dimensional nucleation graining growth which was controlled by diffusion. For the middle stage (0.7<α<0.9), the crystallization mechanism is surface crystallization with one dimensional nucleation graining growth at a near-zero nucleation rate. In the final stage(α>0.9),the local Avrami exponents rose anomalously from 1.4 to about 2.0.


2001 ◽  
Vol 16 (8) ◽  
pp. 2399-2407 ◽  
Author(s):  
S. O. Kasap ◽  
D. Tonchev

We have studied the glass transition behavior of vitreous As2Se3 by carrying out temperature-modulated differential scanning calorimetry (TMDSC) and conventional differential scanning calorimetry (DSC) experiments to measure the glass transition temperature Tg. In TMDSC experiments we have examined the reversing heat flow (RHF), that is the complex heat capacity CP in the glass transition region as the glass is cooled from a temperature above the glass transition temperature (from a liquidlike state) and also as the glass is heated starting from room temperature (from a solidlike state). The RHF, or CP versus T, in TMDSC changes sigmoidally through the glass transition region without evincing an enthalpic peak which is one of its distinct advantages for studying the glass transformations. The Tg measurements by TMDSC were unaffected by the amplitude of the temperature modulation. We have determined apparent activation energies by using Tg-shift methods based on the Tg-shift with the frequency (ω) of temperature modulation in the TMDSC mode and Tg-shift with heating and cooling rates, r and q, respectively, in the DSC mode. It is shown that the apparent activation energies ∆h* obtained from ln ω versus 1/Tg and ln q versus 1/Tg plots are not the same, but nonetheless, they are approximately the same as the apparent activation energy ∆hn of the viscosity over the same temperature range where the empirical Vogel expression of Henderson and Ast, η = 12.9 exp[2940/(T - 335)], was used for the viscosity. The latter observation is in agreement with the assertion that the structural relaxation time Ʈ is proportional to the viscosity h. The apparent activation energy ∆hr obtained from the ln r versus 1/Tg plot during heating DSC scans is lower than ∆h* observed during cooling scans. The results are discussed in terms of a phenomenological Narayanaswamy type relaxation time. It was observed that Tg obtained from TMDSC cooling experiments did not depend on the underlying cooling rate for q ≤ 1 °C min-1; and for temperature amplitudes 0.5–5 °C. The transition due to the temperature modulation was well separated from the transition due to the underlying cooling rate. Further, the apparent activation energies obtained from ln ω versus 1/Tg during cooling and heating scans for q and r ≤ 1 °C min−1 are approximately the same as expected from Hutchison's calculations using a single relaxation time model of TMDSC experiments.


2010 ◽  
Vol 654-656 ◽  
pp. 2398-2401 ◽  
Author(s):  
Ludovic Charpentier ◽  
Patrick J. Masset

The thermal decomposition of pyrite was investigated under reducing atmosphere, e.g. p(O2)~10-6 bar. Thermogravimetric measurements were coupled with differential scanning calorimetry and mass spectrometry. Multi-scan method was used to calculate the values of the activation energy of the reaction of thermal decomposition of the pyrite. It was shown that the value of the activation energy of the decomposition of pyrite into pyrrhotite varies with the reaction progress. The values of activation energy vary from 250 to 350 kJ.mol-1.


2010 ◽  
Vol 22 (1) ◽  
pp. 255
Author(s):  
J. T. Aaltonen ◽  
S. Singh ◽  
L. R. Fogueri ◽  
N. S. Mulla ◽  
N. M. Loskutoff

Current administration of FSH for the purpose of superovulation of tigers is achieved through serial injections or subcutaneous osmotic pump (Blevins B et al. 2009 J. Reprod. Fertil. 21, 153 abst). Both have limitations, which are pulsatile hormone fluctuations and multiple anesthesia events for pump insertion and removal, respectively. In vivo attempts to superovulate tigers using aluminum hydroxide gel [Al(OH)3] proved unsuccessful by fecal hormone enzyme immunoassay. In addition, Al(OH)3 raises the potential for an immune response to foreign FSH. An inert, biodegradable, and FDA-approved polylactide-co-glycolide polymer-based in situ gel forming system eliminates the problems above with a single injection delivery, allowing a more natural sustained release of FSH. Polymer solutions were made using a solvent mixture of benzyl benzoate (BB), or benzyl alcohol (BA), or both. Porcine FSH (Folltropin®-V, Bioniche, Belleville, Ontario, Canada) was incorporated into the polymer solution via sonication, which gelled upon contact with interstitial fluid. Polymer composition (ratio of lactide to glycolide) and concentration and ratio of BB to BA parameters can be manipulated to achieve a desired release profile. Two formulations (F1 and F2) were created with differing percentages of composition for the purpose of recreating a controlled release rate of 100 NIH-FSH-P1 reference standard mg/day (pump output). The FSH polymer was injected into 15 mL of PBS (pH 7.4 in a 37°C shaker bath at 30 rpm), which instantly formed a gel. One milliliter of PBS was sampled every 24 h and replenished with fresh PBS. The amount of FSH was determined by measuring UV absorbance at 290 nm (Shimadzu 1600 UV-visible spectrophotometer; Shimadzu Scientific Instruments, Columbia, MD, USA). Formulation F1 showed a higher initial burst release than F2 (61.5% v. 35.8% of total incorporated hormone) as a result of the use of 100% BA as a solvent. Benzyl alcohol is more hydrophilic than BB, leaching out of the polymer-FSH solution faster and leading to a greater release of the hydrophilic FSH. Both formulations showed a biphasic release pattern in which the first phase was relatively faster than the second phase. Although F2 (80% BA-20% BB solvent) was successful in reducing the burst release by half, the day-to-day profile is below target. Our results indicate that F2 has a better release profile than F1 for inducing folliculogenesis and can be improved by manipulating formulation parameters such as increasing the polymer concentration and BA:BB ratio of the solvents. Using Fourier transform infrared spectrometry and differential scanning calorimetry, hormones before gel incorporation were compared to those released. Fourier transform infrared spectrometry and differential scanning calorimetry data suggest that the gel does not affect the conformational stability of FSH. It is therefore possible to manipulate a gel to mimic the release rate of a proven osmotic pump without compromising the functionality of the protein hormone, potentially reducing the number of surgeries or injections to superovulate tigers.


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