{"id":804204,"date":"2026-11-05T01:55:32","date_gmt":"2026-11-05T06:55:32","guid":{"rendered":"https:\/\/spaceweekly.com\/?p=804204"},"modified":"2026-11-05T01:55:32","modified_gmt":"2026-11-05T06:55:32","slug":"nasa-deliberately-smashed-apollo-12s-empty-lunar-lander-into-the-moon-at-about-3750-mph-in-1969-and-a-seismometer-the-crew-had-set-up-on-19-november-before-leaving-recorded-the-moon-ringing","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=804204","title":{"rendered":"NASA deliberately smashed Apollo 12\u2019s empty lunar lander into the Moon at about 3,750 mph in 1969, and a seismometer the crew had set up on 19 November before leaving recorded the Moon ringing like a bell for nearly an hour."},"content":{"rendered":"


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The impact was not an improvised disposal maneuver. Apollo 12\u2019s flight plan called for the lunar module ascent stage to provide a controlled seismic source after Charles Conrad Jr. and Alan Bean returned to Richard Gordon in the command module Yankee Clipper<\/em>. The ascent stage of Intrepid<\/em> was jettisoned, remotely deorbited and sent toward the lunar surface; its descent stage remained at the Apollo 12 landing site.<\/p>\n

The experiment mattered because scientists knew the source. Natural moonquakes and meteoroid impacts can be recorded seismically, but important properties of those sources have to be reconstructed from the signals themselves. For Intrepid<\/em>, NASA knew the event timing and had tightly constrained the spacecraft\u2019s trajectory and impact conditions, giving the Passive Seismic Experiment a calibration event for examining how seismic energy moved through lunar material.<\/p>\n

NASA\u2019s National Space Science Data Center lists the impact at 22:17:17.7 UTC on November 20, 1969, with a velocity of 1.68 km\/s (3 760 mph) and a trajectory 3.7\u00b0 above the local horizontal. The Apollo 12 Preliminary Science Report placed the source 75.9 km (47.2 miles) from the seismic station. Conrad and Bean had deployed the Apollo Lunar Surface Experiments Package, including its Passive Seismic Experiment, during their first moonwalk on November 19.<\/p>\n

A controlled seismic experiment on the Moon<\/h2>\n
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LRO image of the impact area and debris field of Intrepid\u2019s ascent stage, east of the Fra Mauro B crater. Credit: NASA <\/figcaption><\/figure>\n<\/div>\n

The seismogram did not behave like a simple pulse followed by rapid decay. All three long-period components recorded the impact, and the signal rose gradually to a peak-to-peak amplitude of about 10 nm over approximately seven minutes before declining slowly into the background. NASA\u2019s Preliminary Science Report put the total duration at about 55 minutes; the Apollo 12 Mission Report used approximately 50 minutes, while later NASA historical accounts summarize the response as lasting nearly one hour.<\/p>\n

The seven-minute buildup is physically important. The collision occurred on a much shorter timescale, so the delayed maximum belongs to the seismic wavefield recorded after the impact rather than to a seven-minute collision process. Distinct seismic phases were difficult to identify after the beginning of the record, leaving a prolonged wave train in which energy arrived over an extended interval.<\/p>\n

Apollo investigators considered whether debris thrown from the impact might produce enough secondary impacts to explain the long disturbance. The Preliminary Science Report found that the first seismic arrival was too fast for nearby ejecta to account for the onset and shifted attention to propagation through the Moon. The investigators did not, however, establish one unique propagation mechanism from the Apollo 12 recording.<\/p>\n

Why the signal lasted nearly an hour <\/h2>\n
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\"Recording
Recording from the Apollo 12 seismometer of the intentional crash of Intrepid\u2019s ascent stage. Credit: NASA<\/figcaption><\/figure>\n<\/div>\n

One early interpretation centered on weak intrinsic attenuation. Attenuation is the loss of seismic-wave energy as a wave travels through material. Apollo investigators expressed that behavior partly through the seismic quality factor, Q: higher Q corresponds to less energy lost during each cycle. Under the assumptions used in their preliminary analysis, they estimated Q values of roughly 3 000\u20135 000 for the material sampled by the signal, compared with values of 10\u2013300 that the report cited for most terrestrial crustal materials. The values were preliminary model-dependent estimates, not a direct measurement of a single universal lunar Q.<\/p>\n

Scattering offered another part of the explanation. When a seismic wave encounters strong changes in rock properties, part of its energy is redirected rather than continuing along one simple path. In a highly heterogeneous medium, many redirected portions of the same event can reach a detector at different times. Seismologists call the prolonged tail of arrivals the seismic coda.<\/p>\n

The original Apollo team treated that interpretation cautiously. A diffusion calculation reproduced aspects of the slow decay but did not verify the scattering hypothesis, and the investigators also considered a near-surface waveguide associated with seismic velocity increasing with depth. Apollo 12 therefore established the unusual waveform much more securely than it established a unique explanation for the waveform.<\/p>\n

What later research revealed about lunar scattering<\/h2>\n
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\"Conrad
Conrad working on the central station of the Apollo Lunar Surface Experiment Package, with its various instruments deployed around it. Credit: NASA <\/figcaption><\/figure>\n<\/div>\n

Later analysis placed stronger quantitative constraints on the problem. Blanchette-Guertin, Johnson and Lawrence (2012) examined 369 higher-quality lunar seismograms from 72 events using characteristic rise and decay times. They found that intrinsic attenuation, scattering and possible focusing of energy in a near-surface low-velocity layer all contribute to lunar coda decay and stated that their exact individual contributions could not be uniquely quantified. For shallow events, their results supported scattering in a global near-surface layer as the dominant contribution under particular frequency and distance conditions.<\/p>\n

The authors proposed the megaregolith as that major scattering layer. The megaregolith is the heavily impact-processed upper lunar material, including fragmented ejecta over fractured crust. Physically, such heterogeneity gives seismic waves many interfaces at which their direction can change, spreading the energy from one impulsive event across many paths and arrival times rather than producing only a few clean phases.<\/p>\n

Onodera, Kawamura, Tanaka, Ishihara and Maeda (2022) tested lunar scattering with full three-dimensional seismic-wave simulations. Their simulated Apollo signals reproduced the strongly scattered character of the observations, and the model yielded a lunar scattering intensity about 10 times that of the heterogeneous terrestrial region used for comparison. The factor is a model-derived comparison, not a direct measurement of the whole Moon against the whole Earth, and the authors identified the detailed heterogeneous structure of the lunar subsurface as an unresolved problem.<\/p>\n

How Apollo impacts became probes of the lunar interior<\/h2>\n
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