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VO2, as a promising material for its thermochromic characteristics, is widely used for various thermal and optical applications due to the presence of multiple thermal hysteresis loops resulting in various fabrication conditions.
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Thermal hysteresis behavior and CTE of multiple-reprocessed polypropylene films are measured and discussed.
Above a certain stress level the phase transformations, even in a multiple interface mode, can be driven in such a way that the thermal hysteresis loops have a rectangular part, from which T0 can be determined via the well-known relation: T0 = (Ms + Af)/2, where Ms and Af are the martensite start and austenite finish temperatures, respectively.
The compounds display large thermal hysteresis.
Figure 4 The thermal hysteresis loop for system with random external action and applied pressure.
The thermal hull contains one or multiple thermal zones.
A large thermal hysteresis of ∼7 K discloses the first-order feature for its phase transition.
The thermal hysteresis effect was minimized at the composition of 2.5 wt.% Li2CO3.
If the intermolecular interactions are large enough, the thermal transition between the two stable states is associated with a first-order phase transition and is accompanied by a hysteresis loop which is called thermal hysteresis.
One can note that a first-order phase transition accompanied by a thermal hysteresis can take place.
The width of the thermal hysteresis Δ T is calculated by (Delta T=T_{text {up}}^{eq}-T_{text {down}}^{eq}).
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