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The compositional variation of glass transition exhibited a similar trend to the predicted result of thermodynamic theory for compatible polymer blends.
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As observed in Figure 2b1,b2,b3, the semiconductor-metal phase transition exhibits a characteristic thermal hysteresis which is due to latent heat evolved and absorbed during the first-order structural transition [17].
The Lumi-Ff to Meta-Fr transition exhibits a significant blue shift from 715 to 635 nm, suggesting a major structural rearrangement.
Harré and Bossomaier (2009) showed that they are indeed phase transitions, exhibiting a peak in mutual information.
In general, it is well known that π-π* and CT transitions have high molar extinction coefficients (>10,000 L/mol·cm), leading to the intense absorption bands, whereas n-π* and d-d transitions exhibit a low molar extinction coefficients, ε = 10 to 100 and ε = 5 to 500 L/mol·cm, respectively [5 8].
The LE optical transition exhibits a very long decay time which is greater than the repetition period of the laser (12 ns) and is not easily measurable with this experimental setup.
While the loss modulus was found to increase monotonically over the entire range of siloxane content, the glass transition temperature exhibited a stepwise increase upon reaching the conditions for phase co-continuity.
The brittle to ductile transition of P coincided with its glass to rubber transition, whereas SC exhibited a ductile behaviour within the glassy state.
Dichloroindigo shows absorption from the HOMO-3 to LUMO-0 transition but exhibits a different emission transition from LUMO-0 to HOMO-2.
At low strains (prior to the polydomain-to-monodomain transition) the data exhibited a final relaxed modulus of Ef=1.8 MPa.
For example, the fact that the "no transition" MAO phenotype exhibited a significantly more severe risk factor profile at baseline is suggestive for the requirement of a longer exercise intervention.
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