Sentence examples for both the models are from inspiring English sources

Both the models are solved by kinetic Monte Carlo methods.

Parameters of both the models are obtained based on the available results of experimental tests carried out at different temperatures and strain rates.

Both the models are trained on the data set obtained from experiments carried out in Marine Structures Laboratory, Department of Applied Mechanics and Hydraulics, National Institute of Technology Karnataka, Surathkal, India.

At the pixel level, a couple of BG models is maintained for each pixel independently: both the models are based on a 40-coefficients, one-step Wiener filter, where the (past) values taken into account are the predicted values by the filter in one case, and the observed values in the other.

While both the models are able to reproduce the experimentally observed global spray and combustion characteristics, predictions using the KH-ACT model exhibit closer agreement with measurements in terms of liquid penetration, cone angle, spray axial velocity, and liquid mass distribution for non-evaporating sprays.

Both the models are shown as follows q_{e} = frac{{q_{m}K_{text{L}} C_{e} }}{{1 + K_{text{L}} C_{e} }} (6) q_{e} = K_{text{F}} C_{e}^{1/n} (7 where q m is the maximum uptake capacity (mg/g), KL (L/mg) the Langmuir adsorption constant, KF the Freundlich constant related to adsorption capacity (mg/g) and C e the concentration of metal ions at equilibrium (mg/L).

Both the models were developed by the authors.

The non-linear plot for both the models is shown in Fig. 3.

The expected number of transmissions for both the models were computed.

Both the models were found equally suitable to describe the measured data.

It may be noted that 'Time to Peak discharge' as estimated by both the models was found to be identical for the event of 23/6/1999.