Optimal Designs for a Modified Exponential Model
Juan M. Rodr´ ıguez-D´ ıaz Mar´ ıa Teresa Santos-Mart´ ın 1 Historical notes
From the middle of the 19th century on several equations relating the rate constant k of a chemical reaction to the temperature T have appeared in literature. All of them were developed experimentally and the most popular ones try to fit linearly ln(k) against T, 1/T or ln(T). The fact that this different plots gave reasonably good linear fits with the same data was due to the narrow temperature ranges usually employed in kinetic studies (see [Laidler (1984)]), but after the controversy on the models maintained during several decades all these equations were gradually dropped out but two of them: the Arrhenius and Modified-Arrhenius ones. The main reason for the rejection of the remaining equations was the lack of theoretical justification for them, while the Arrhenius ones were well explained theoretically. 1.1 The Arrhenius equation The Arrhenius equation is widely accepted as the right tool to describe the influence of temperature on the rates of chemical processes. It was first used by Svante Arrhenius in 1884 in his studies of dissociation of electrolytes, but later on applied to describe the relationship between temperature and the rates of chemical reactions and many other physical processes such as diffusion, thermal and electrical conductivity, viscosity, etc. The integrated form of the equation is ln(k) = A′ − β T , where β = E/R, with E the activation energy and R the gas constant. By taking expo- nentials and making the change T = 1/X it comes to be the exponential model E[k] = Ae−βx + ε (1) where A = eA′ > 0 is the frequency factor, and β > 0. The optimal designs for this model have been studied in [Han and Chaloner (2003)] for independent and normally-distributed errors with constant variance and in [Rodr´ ıguez-Torreblanca and Rodr´ ıguez-D´ ıaz (2007)] for different variance structures. Also optimal and compound designs specifically for the Arrhenius equation as well as a study of the efficiency of some designs used in literature can be found in [Rodr´ ıguez-Arag´
- n and L´
- pez-Fidalgo (2005)].
However, for the analysis of more precise rate-temperature data, particularly in studies covering a wide temperature range, it is usual to allow A′ to be temperature-dependent, proportional to ln(T), or equivalently A proportional to X raised to a power m producing E[k] = axme−βx + ε (2) where a > 0 is now temperature independent and β > 0, the so called Modified-Arrhenius (MA) model. Nowadays (see [Laidler (1984)]), the procedure often employed is to use
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