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1 f anthocyanin degradation was modeled by the Arrhenius equation.
2 ependent Phia values were analyzed using the Arrhenius equation.
3 onditions by first order kinetics, using the Arrhenius equation.
4 st exactly by the yields calculated with the Arrhenius equation.
5 ncrease in the thermal energy (k(B)T) in the Arrhenius equation.
6 y on binding enthalpy, in agreement with the Arrhenius equation.
7 be described with an equation similar to the Arrhenius equation.
8 a two-state Markovian process that obeys the Arrhenius equation.
9 omplicated and could not be explained by the Arrhenius equation.
10 ve reaction rate constants complied with the Arrhenius equation.
11 surrounding cavitation bubbles and using the Arrhenius equation, an effective mean temperature of 340
12 t migration rate could be represented by the Arrhenius equation and therefore can be controlled by th
13 ase the rate of dechlorination, according to Arrhenius' equation, and increase the rate of TCE desorp
14 ith temperature and formulations such as the Arrhenius equation are widely used in earth system model
15 determined to be E(a) = 25 +/- 7 kJ mol(-1) (Arrhenius equation), DeltaH(double dagger) = 23 +/- 7 kJ
17 ium triflate, 17e, were calculated using the Arrhenius equation: E(a) = 26.8 kcal/mol, Delta H(++) =
19 pressure independent and gave the following Arrhenius equation: log[(k/(cm(3) molecule(-1) s(-1))] =
21 ustrates a novel adaptation of the classical Arrhenius equation that accounts for the microscopic ori
22 action at elevated temperatures and used the Arrhenius equation to extrapolate the results to room te
23 s time decay data, and these were fit to the Arrhenius equation to give the effective barrier to rela
24 ere we present a theory that generalizes the Arrhenius equation to include static disorder of conform
25 derived from H-B relation parameters and the Arrhenius equation was applied to describe changes in co
26 ed in the range of 35 to 60 degrees C, using Arrhenius equation, was determined to be 11.32 kcal mol(
27 urfaces are traditionally described using an Arrhenius equation with energy barrier and pre-exponenti
28 out-of-phase magnetic susceptibility to the Arrhenius equation yields an effective energy barrier, U
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