The remaining term in the equation, G, is the gravitational constant, which has to be measured by experiment and, as of 2007, US scientists have measured it at 6.693 × 10−11 cubic metres per kilogram second squared.
Some natural frequencies and their corresponding mass normalized mode shapes of physical structures may be measured by experiment.
The variables were measured by experiments performed on different frequency channels.
The static torque values of the rotor have been measured by experiments and calculated by numerical analysis, and finally they have been compared.
Flammability limits of the burner were measured by experiments, and longitudinal temperature distributions of air and burned gas flowing in the passes of the burner were determined by means of both experimental measurements and numerical simulations.
The performance of the correction methods under such conditions is measured by experiment 6.
These association constants are too high to measure by direct titration, but they can be measured by competition experiments, by displacing the templates with monodentate ligands, such as pyridine or quinuclidine.
The identification cost can be measured by either the experiment time, the performance degradation during experimentation due to the added excitation signal, or a combination of both.
S k, i, r can be obtained from the regulatory sequences, SI k stands for the splicing index of the k-th exon, which will be measured by the exon array experiment, and calculated based upon Equation 1.
The homogenization temperatures (Tc) of the one-phase carbonic inclusions (CH4) were measured by cooling experiments with samples E1 and W4 (Figure 4f).
