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However, the response function cannot be measured by experiments quantitatively.
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 variables were measured by experiments performed on different frequency channels.
Applicability of the proposed formulation is assessed by comparing moment-rotation (M θ r ) curves and ultimate moment capacities with those measured by experiments and estimated by FE analyses and three-parameter power model.
Performance of the proposed prediction model is assessed by comparing the predicted values of M u and M θ r curves with those of measured by experiments and calculated by FE analysis and Kishi Chen's three-parameter power model (Kishi and Chen 1990).
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The calculated patterns compare favourably with those measured by experiment.
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.
While Measured by experiment, the actual light uniformity of the WD-CPC is 0.153, which is in agreement with simulations.
Some natural frequencies and their corresponding mass normalized mode shapes of physical structures may be measured by experiment.
Based on the home-built tapping-mode AFM experiment system, the resolution and the response time of the first and second order resonance measured by experiment are respectively: 0.83 nm, 0.42 nm; 1265 μs, 573 μs.
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