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Angular motion measurements from a component-level laboratory experiment under dynamic loading are utilized.
Preliminary cloud motion measurements from the images at 283 and 365 nm reveal some differences, which may be due to altitude but could also be due to differences and changes in morphology (sources or processes producing the contrasts).
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Hueso et al. (2015) attribute the cloud patterns between 0.3 and 1 µm to altitudes between 60 and 72 km and their near-infrared cloud motion measurements match those from the Pioneer Venus probe and VeGa balloon derived winds at altitudes between 56 and 62 km, differing from the 58 64 km level derived by (Sánchez-Lavega et al. 2008) from radiative calculations.
Perhaps the most direct method of verifying it comes from proper motion measurements of water masers in nearby galaxies (for example, in the nearby spiral NGC4258).
First cloud motion measurements on Venus were reported from ground-based images by Boyer (1965), Beebe et al. (1973), and from first spacecraft observations from Mariner 10 flyby images by Suomi (1975), Suomi et al. (1976), Sidi (1976), Limaye (1977), Limaye and Suomi (1981).
If you take the maximum radial velocity observed to be the true velocity of the masers, then from the proper motion measurements you can derive a distance.
Proper motion measurements give the shock speed around the shell, which varies from 3000 to 7400 km/s.
First, it treats motion measurements and motion estimates separately.
AR advised on the proprioception and range of motion measurements.
The diffusion constant that was calculated from Brownian motion measurement is inversely proportional to the hydrodynamic diameter of the measured particle; low diffusion constant usually correlates with large mucin gelation/aggregation [21], [22].
Motion sensors such as the accelerometer enable live motion measurement.
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