Three years' observations of Tonga‐Fiji‐Kermadec earthquakes at stations in New Zealand have been analysed by the statistical techniques applied to Herrin's “1968 Seismological Tables for P Phases”, to yield smoothed regional travel times for P and S . The travel‐time curve for P is later than Herrin's until it merges with it at about 30°, implying lower velocities than those of Herrin's model at shallow levels in the upper mantle, and higher velocities at deeper levels. The travel‐time curve for S crosses the Jeffreys‐Bullen curve at 21° and 27° and has a greater curvature in this range. A correlation between the isostatic gravity anomaly and the mean travel‐time residual at the stations is tentatively explained in terms of higher velocities in the deep seismic zone.
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M. J. Randall (1971) studied this question.
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