{'fraction_non_alphanumeric': 0.03318777292576419, 'fraction_numerical': 0.028820960698689956, 'mean_word_length': 4.483253588516747, 'pattern_counts': {'":': 0, '<': 0, '<?xml version=': 0, '>': 0, 'https://': 0, 'lorem ipsum': 0, 'www.': 0, 'xml': 0}, 'pii_count': 0, 'substrings_counts': 0, 'word_list_counts': {'cursed_substrings.json': 0, 'profanity_word_list.json': 0, 'sexual_word_list.json': 0, 'zh_pornsignals.json': 0}}
Kinematics of OB Stars

The kinematics of 1817 stars of class O-B5 are examined. The 1655 stars with distances up to 1 kpc are taken from the Hipparcos catalog and 162 stars with distances greater than 1 kpc from Westlin's study of OB stars. The Ogorodnikov-Milne model of Galactic kinematics, with Edmondson's second-order terms included, is used for the equations of condition and mixed total least squares-least squares (TLS-LS) is used for the reduction method. Reasonable values for the parameters of Galactic kinematics are obtained. In particular, Oort A and B constants yield a Galactic rotation of 258.7 ± 34.29 km s-1 if we take the distance of the Sun from the Galactic center as 8.5 ± 1.1 kpc. Although lower than the higher values obtained by some other investigators and higher than the IAU's recommended 220 ± 20 km s-1, all the determinations fall with their stated mean errors. Thus, no evidence for a significant difference in the various determinations exists. Evidence does exist, however, to assert that the TLS-LS reduction model with second-order terms seems superior to ordinary least-squares with only first-order terms.