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Here, we use a simple approach [20] by calculating the thermal conductivity at different tube lengths and then using a linear fitting according to the formula 1 κ p = a + b l.
The decaying amplitude of the extracted modal responses is then used to identify the modal damping ratios using a linear fitting function on modal response data.
For biases below 0.60 V, were the inversion layer describing the n-type conductivity can be found, an electron concentration of 5.6 × 10 cm−3 was calculated using a linear fitting of the experimental points presented in Fig. 5b.
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For the four methods, all of the slopes were determined using a linear fit.
The agreement between model and experiment is determined using a linear fit to ordered pairs of data.
The transverse relaxivities (R2, 1/T2) were determined using a linear fit of 1/T2 as a function of the Fe concentration of the particles.
By using a linear fit to the two different sets of measurements, the S values of 804.7 μV/K for the 20 mK/s heating rate and 791.2 μV/K for the 0.8 mK/s heating rate were obtained.
In Fig. 5b, the ΔV versus ΔΤ curve is plotted, from which S is extracted using a linear fit to the data (see Fig. 5b) (red line), from which the value of S = 916.9 μV/K is obtained.
When using a linear fit, the correlation is r2 = 0.73 with these parameters.
The rate of each reaction was determined using a linear fit to the first 10% of substrate consumption.
The rate of each assay was determined using a linear fit to the first 10% of substrate consumption.
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