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Maximum sintering rate is achieved at 1350 °C.
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The basic mechanism and activation energy (Q) of diffusion at the initial sintering stage were estimated using the sintering rate equations that are applicable to the CRH data.
Equation (4) corresponds to the sintering rate equation derived by J Wang and R Raj.
Sintering rate at the initial sintering stage is expressed by the equation: frac{d}{dt}left[{left(frac{varDelta L}{L_0}right)}^{frac{1}{n}}right]=frac{Kgamma varOmega D}{kTaP} (2).
In heat microscope measurements, maximum sintering was recorded at 1138 °C.
Depending on their nature, they can either accelerate or slow down the sintering rate.
Due to high sintering rate and narrow temperature range, the fuel path will be clogged/blocked in a few seconds.
We can conclude that in samples 3Y-TZP (DIPE), mass transfer process is more intensive than in samples TZ-3Y (TOSOH), which was confirmed by higher sintering rate at the initial stage of sintering.
Similarly, ionic substitutions in hydroxyapatite or in tricalcium phosphate create lattice defects that modify the sintering rate.
Higher heating rate leads to a higher mechanical strength due to accelerated sintering rates.
Particle shape imposes a strong effect on the viscous sintering rates in so far as sintering timescales are dependent on curvature of the surface in contact with the substrate in a jet engine.
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