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functions
On the Accuracy of Surface‐Wave Dispersion Measurements from Horizontal‐Component Ambient Noise Cross Correlations
Ground‐Motion Model for Hard‐Rock Sites by Correction of Surface Recordings (Part 2): Correction, Mixed‐Effects Regressions, and Results
Direct Image Dissimilarity Inversion of Ambient Noise Multimodal Dispersion Spectrograms
Finite‐Frequency Delay Times of Phase Segments for Body Waves
Noise Reduction from Vertical‐Component Seismograms Recorded by Broadband Ocean‐Bottom Seismometers Deployed at the Western Pacific
Impact of Site‐Response Characterization on Probabilistic Seismic Hazard in the Po Plain (Italy)
Empirical Distance Metrics Relationships and Uncertainties in Seismic Hazard Assessment
A Method to Simulate High‐Frequency Decay of Acceleration Spectra of Ground Motions without the Need for Kappa or f max Filters
Magnitude and Slip Scaling Relations for Fault‐Based Seismic Hazard
Finite‐Frequency Kernels for Pg Wavetrains
On the Ratio of Full‐Resonance to Square‐Root‐Impedance Amplifications for Shear‐Wave Velocity Profiles That Are a Continuous Function of Depth
MagMin_PT: An Excel-based mineral classification and geothermobarometry program for magmatic rocks
Role of Earth-Moon rotational dynamics in the shaping of the surface of our planet
ABSTRACT The age of the Moon (1.55–1.78 b.y. old) as calculated from its regression as a function of geological time is much younger than the currently accepted age (ca. 4.52 Ga) determined by radiometric dating of lunar samples collected by Apollo astronauts. This discrepancy has posed a serious challenge for planetary scientists to account satisfactorily for the formation and subsequent breakup of Pangea. Conventional orbital models of the Earth-Moon system cannot explain why Pangea formed on only one hemisphere of Earth, whereas this study’s proposed two-stage rotation model can provide a plausible explanation. Calculations and a plot of the Earth-Moon separation distance against geologic age suggest that, during their first ~3.0 b.y., Earth and the Moon were mutually tidally locked, rotating as an integrated unit about a barycenter (designated as stage I rotation). Beginning 1.55 Ga, however, Earth disengaged from its tidal lock with the Moon and entered its current orbital mode (designated as stage II rotation). The dynamics associated with the two rotational modes of the Earth-Moon system throughout Earth’s history are hypothesized to constitute the driving forces for the migration and coalescence of landmasses during stage I rotation to create Pangea, and its ultimate breakup and drifting during stage II rotation.