The measured distortion polarizations of a group of bis-arylmercury co~npounds show that they do not exhibit exalted atom polarizations. The apparent orientation polarization of each is appreciable. Two of them, which are substituted symmetrically with methoxyl or nitro, exhibit moments expected from the rotation which is generated in such substances. By comparison of bis-4-bromophenylmercury202 with the analogue containing the ordinary isotopic mixture of mercury the apparent moments are shown to be unrelated to nuclear asymmetry. The conclusion is unaltered that the appare~lt nlonlerlts of bis-arylmercury compounds are due to effective non-linearity in the C-Hg-C bond.In continuation of our search t o explain the apparently anomalous electric moments of bis-arylmercury compounds (1) we have re-examined and extended the work of Hampson (2), who originally observed the anomalies. Essentially we have arrived a t a conclusion which partakes of Hampson's original explanation as a "flexibility moment", which was later generally endorsed by Sidgwick (3) as not unexpected when mercury is involved.Hampson's opinion that he had measured an orientation polarization of bis-phenylmercury and its symmetrical p-methyl, fluoro, chloro, and bromo analogues was not generally accepted. In particular there were some (4) who tried to attribute the anomaly t o atom polarization, an argument which Coop and Sutton themselves questioned on the basis of the unrealistic force constant which would be required. Finally the question whether diphenylmercury exhibited an abnormally high atom polarization was for the first time put t o the test of experiment (1, 5) and was answered in the negative.Indeed the value obtained by direct measurement of distortion polarization (PD, i.e. PE+*) for diphenylmercury was found to be lower than that expected according to the commonly used methods of calculating molecular refraction (RIIR, i.e. P,) by addition of the constituent atom refraction according to Eisenlohr (6) or of the bond refractions according to Vogel (7). Since the low distortion polarization implies a definite dipole moment which is unexpected among bis-mercurials it is necessary to decide why these distortion polarizations are low. Consequently the distortion polarizations of a series of bis-mercurials have been examined by the method of dielectric constant determination with compressed wafers of randomly oriented powders together with a number of other substances more or less related. The results are sho\vn in Table I, where the differences between PD and an average of MRD by the methods of Eisenlohr and Vogel are shown in the last column.The distortion polarization (PD) of diphenylmercury has been redetermined with a result in good agreement with the 57.1 cc reported previously (1). The low value (negative difference) is reflected in comparable differences for the series of substituted diphenylmercurys, items 2-8 inclusive. On the other hand item 9, dimesitylmercury, shows a distortion polarization which is higher than the aver...