Loading…
DATA STATUS
457 series loaded · last import on 2026-10-26

Earth tide and moonquakes The Earth triggers the deep moonquakes

Correspondences

What is linked, what is not

Each arc joins two phenomena tested on this site. Green and animated: clear link (correlation significant at 5 % after correcting for autocorrelation, or a response outside chance in an event study). Grey: inconclusive test. A statistical link alone does not establish causation.

  • Clear link
  • Inconclusive
Hypotheses tested
33
Clear links
24
correlation p < 0.05 or epochs outside chance
Causation demonstrated
0
a correlation demonstrates none

Arc width from |r| of the stored result; several tests between the same phenomena are drawn as stacked arcs.

Hypothesis tested: The Earth deforms the Moon by its tide, the more so as the Moon is close (perigee) and according to its position relative to the Earth’s equator. If this stress triggers the deep moonquakes, each nest should wake at the same phase of the anomalistic month (27.55 d) and of the draconic month (27.21 d). The synodic month (29.53 d), that of the phases and of sunlight, is the control: the Sun does not heat the Moon 900 km down (Lammlein 1977; Bulow et al. 2007).
Nests set by the tide
28 / 28
anomalistic month, p < 0.01 per nest; 28 also by the draconic month; median R 0.94; probability by chance < 10⁻¹⁰
Nests set by the phases
1 / 28
synodic month (control): as many as chance predicts (p = 0.24); median R 0.17
Deep moonquakes tested
955
of the 28 nests with at least 10 quakes, out of 106 located nests
Period analysed
1969-07-27 → 1977-09-30
computed on Oct 26, 2026 · engine v1.0
Nest A1 (186 quakes, 867 km): distribution in the month (%)
Show the data as a table
The 28 nests tested
NestQuakesDepth (km)Anomalistic month (R, p)Draconic month (R, p)Synodic month (R, p)
A1186867 0.60 · < 0,0010.73 · < 0,0010.08 · 0.280
A8681,086 0.70 · < 0,0010.61 · < 0,0010.25 · 0.013
A9571,037 0.70 · < 0,0010.98 · < 0,0010.18 · 0.140
A1853925 0.92 · < 0,0010.79 · < 0,0010.09 · 0.650
A751893 0.91 · < 0,0010.81 · < 0,0010.12 · 0.460
A33 (far side)49877 0.97 · < 0,0010.57 · < 0,0010.15 · 0.310
A641844 0.89 · < 0,0010.94 · < 0,0010.08 · 0.750
A2041945 0.50 · < 0,0010.52 · < 0,0010.08 · 0.750
A3034931 0.76 · < 0,0010.99 · < 0,0010.13 · 0.590
A1432933 0.97 · < 0,0010.66 · < 0,0010.10 · 0.740
A4030867 0.97 · < 0,0010.86 · < 0,0010.14 · 0.550
A4230907 0.81 · < 0,0010.99 · < 0,0010.08 · 0.830
A16291,019 0.98 · < 0,0010.79 · < 0,0010.13 · 0.640
A527933 0.90 · < 0,0010.83 · < 0,0010.36 · 0.031
A3926933 0.98 · < 0,0010.96 · < 0,0010.15 · 0.560
A21251,037 0.96 · < 0,0010.89 · < 0,0010.14 · 0.630
A1520747 0.92 · < 0,0010.72 · < 0,0010.21 · 0.420
A4418908 0.97 · < 0,0010.97 · < 0,0010.22 · 0.430
A9718989 0.98 · < 0,0010.97 · < 0,0010.29 · 0.220
A2516924 0.99 · < 0,0010.95 · < 0,0010.15 · 0.700
A3416971 0.95 · < 0,0010.99 · < 0,0010.25 · 0.380
A1715807 0.90 · < 0,0010.99 · < 0,0010.29 · 0.290
A4115847 0.97 · < 0,0010.97 · < 0,0010.26 · 0.380
A1913974 0.98 · < 0,0010.94 · < 0,0010.26 · 0.440
A27131,085 0.94 · < 0,0010.78 · < 0,0010.39 · 0.140
A5011828 0.94 · < 0,0010.96 · < 0,0010.65 · 0.007
A8211919 0.98 · < 0,0010.93 · < 0,0010.30 · 0.390
A1010988 0.77 · 0.0010.96 · < 0,0010.23 · 0.590

Aligned series (CSV)

Method and sources

Event catalogue of the Apollo seismic network (levent.1008, Nakamura et al. 1981, updated; PDS Geosciences) and positions of the deep nests (Nakamura 2005). For each deep moonquake assigned to a nest, the phase of the Moon at the onset of the signal is computed in three months: mean anomaly M′ (anomalistic month), argument of latitude F (draconic) and mean elongation D (synodic), after Meeus (1998, eq. 47.2 to 47.5). For each nest of at least 10 quakes, the Rayleigh test measures the clustering of the phases (length R of the mean vector, p after Zar 2010). The number of nests significant at p < 0.01 is compared with the 1 % expected by chance (binomial law, nests assumed independent).

Computation parameters
{
    "test": "Rayleigh test per nest (Zar 2010, eq. 27.4) for nests of at least 10 events; count of nests with p < 0.01 against a binomial(n, 0.01) null",
    "phase": "mean anomaly M′, argument of latitude F and mean elongation D of the Moon at the onset time (Meeus 1998, eq. 47.2–47.5)",
    "control": "synodic month: sunlight and phase, without tidal role at this period",
    "catalogue": "Apollo passive seismic experiment, lunar event list levent.1008 (Nakamura et al. 1981, updated) and deep nest locations (Nakamura 2005), PDS Geosciences Node"
}

Inputs :

Reading this result
The result is clear: every nest tested follows the tide, almost none the phases. This is the proof, known since the 1970s, that the Earth’s tide triggers the deep moonquakes. The preferred phase changes from nest to nest, as each responds to a different component of the tidal stress: phases therefore do not add up across nests, and the test is made nest by nest. Nests are defined by the likeness of their signals, which does not depend on the date. Correlation is not causation: common factors (seasons, cycles, trends) or coincidence can produce it. The p-values account for autocorrelation (effective n) but not for preprocessing choices; the confidence interval comes from a block bootstrap. The limits of the source data apply.
SOURCES OF THIS PAGE
Lammlein (1977)
Lammlein, D. R. (1977). Lunar seismicity and tectonics. Physics of the Earth and Planetary Interiors, 14, 224–273. · doi:10.1016/0031-9201(77)90175-3
Licence : Published literature; cited
Bulow et al. (2007)
Bulow, R. C., Johnson, C. L., Bills, B. G., & Shearer, P. M. (2007). Temporal and spatial properties of some deep moonquake clusters. JGR Planets, 112, E09003. · doi:10.1029/2006JE002847
Licence : Published literature; cited
Nakamura (2005)
Nakamura, Y. (2005). Farside deep moonquakes and deep interior of the Moon. JGR Planets, 110, E01001. · doi:10.1029/2004JE002332
Licence : Published literature; cited