AI summary · arXiv: 2610.24566v1 · astro-ph.EP

Radar and Infrasound Observations of the 2026 May 30 Cape Cod Bay Superbolide

Juha Vierinen, Ryan Volz, Marc Fries, Elizabeth A. Silber, Sarah Albert, Philip J. Erickson, Matthias Clahsen, Frank D. Lind,
and 5 more authorsNico Pfeffer, John Swoboda, Allan Weatherwax, Simon G. Shepherd, Jorge L. Chau
Original paper Submitted to arXiv on 17 Oct. 2026 24 pages, 12 figures. Submitted to The Astronomical Journal License: CC BY 4.0

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The essentials

Combined radar and infrasound observations trace the Cape Cod Bay bolide from upper-atmospheric entry to falling meteorites, constraining its trajectory, orbit, fragmentation region, and likely mechanical strength.

Question

How can the 2026 Cape Cod Bay bolide’s atmospheric trajectory, pre-impact orbit, fragmentation, and meteorite fall be reconstructed from observations? What do these measurements imply about the meteoroid’s strength and possible composition?

Method

The authors combined 31.65 MHz VHF meteor-radar head-echo and plasma-trail measurements with four weather-radar datasets, infrasound records from 199 sensors, and optical observations. They fitted the trajectory using 229 range measurements, 137 Doppler measurements, and 146 trail positions, then used dark-flight modeling and backward orbit propagation; infrasound analysis used five retained single-station detections and two multi-sensor directional measurements.

Findings

  • Result VHF radar detected the head echo from about 90 to 71 km altitude and plasma-trail echoes down to a 33.61 km radar terminus.
    See the passage in the paper
    Trail echoes remain detectable far below the head-echo interval, down to approximately 30 km.
  • Result Weather-radar detections and dark-flight modeling place the likely meteorite strewn field in Cape Cod Bay, with six radar-constrained modeled fragments ranging from 3.2 g to 1.425 kg.
    See the passage in the paper
    The six weather-radar-constrained landing solutions shown in Figure 8 have modeled masses from 3.2 g to 1.425 kg.
  • Authors’ interpretation The reconstructed heliocentric orbit lies near the cometary–asteroidal classification boundary, and the catalogue search found no convincing parent-body or established-shower association.
    See the passage in the paper
    The reconstructed orbit lies near the cometary–asteroidal classification boundary, with no convincing association with a catalogued parent body or established meteor shower.
  • Authors’ interpretation The authors interpret the radar and dark-flight evidence as consistent with a dense, mechanically strong meteoroid, possibly iron-rich, while noting that its composition is unconfirmed.
    See the passage in the paper
    The radar and dark-flight evidence are consistent with a dense, mechanically strong meteoroid, possibly iron-rich, but the composition remains to be confirmed by recovered material or independent compositional constraints.
  • Result Infrasound analysis estimated an energy of 0.45 kt TNT equivalent and its directional measurements supported a source near the radar terminus.
    See the passage in the paper
    Applying the multi-station bolide period-yield relation of E. A. Silber et al. [62] gives an infrasonic energy estimate of 0.45 kt TNT equivalent.

Limitations

  • The radar-derived total fall-mass method is unvalidated and excludes larger meteorites that may have escaped radar detection.
    See the passage in the paper
    This radar-reflectivity method is unverified, and the iron-composition survival assumption is not a composition determination.
  • The meteoroid’s composition has not been confirmed by recovered material or independent compositional constraints.
    See the passage in the paper
    the composition remains to be confirmed by recovered material or independent compositional constraints.
  • The trajectory and terminus are supported by the weather-radar detections, but this is not a fully independent validation because the dark-flight model uses the meteor-radar trajectory and terminus as inputs.
    See the passage in the paper
    Agreement between the detections and the modeled dark flight therefore supports the reconstructed fall sequence, although it does not provide a fully independent validation of the meteor-radar trajectory.

Why it matters

The authors argue that meteor-radar plasma tracking, together with weather-radar and infrasound measurements, can connect atmospheric entry to near-ground meteorite fall and enable reconstruction of orbits and fragmentation regions. These observations also provide constraints for models of hypersonic shock flow, plasma wakes, and acoustic radiation.

Written by AI from the paper. Passages are checked word for word against the text we analysed; the rest may contain errors.

AI-generated keywords: Cape Cod Bay superbolide; meteorite fall; meteor radar; infrasound; meteoroid orbit

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  • Original abstract
The paper reconstructs the atmospheric entry and likely meteorite fall of the 30 May 2026 Cape Cod Bay superbolide. It examines whether observations from multiple sensor types can connect the meteoroid’s upper-atmosphere trajectory and pre-impact orbit with its fragmentation and surviving fragments. The daytime bolide’s reported impact energy was 1.1 kilotons of TNT equivalent. The authors combine VHF meteor-radar measurements of entry-generated plasma, weather-radar detections of descending solid fragments, and infrasound recordings of the atmospheric shock. They also compare their reconstruction with optical observations and astronomical catalogues. The VHF radar network detected plasma surrounding the meteoroid rather than the solid body itself. The authors used range, Doppler, and interferometric measurements to fit the trajectory, while plasma positions in the wake extended the track below the altitude at which the head echo was visible. The fitted path descended from about 90 km to a radar terminus at 33.61 km. The authors interpreted weather-radar signatures as falling meteorites and combined them with wind measurements in a dark-flight model to estimate fragment paths and landing locations. They screened infrasound recordings from stations within 2,000 km for plausible arrivals. Array processing and envelope timing constrained the direction of the signals, while their periods were used to estimate the event’s energy. Finally, the authors propagated the radar-derived trajectory backward to estimate the meteoroid’s heliocentric orbit. The entry track was steep and southeastward, with a speed of about 26 km/s at 100 km altitude. Head echoes disappeared near 72 km, but short-lived wake echoes remained detectable down to about 30 km. The authors identify 33.61 km as the radar terminus and interpret it as the end of detectable plasma production, likely associated with breakup. Weather radars detected fragments as low as 7.6 km above mean sea level. The modeled fall region is centered in Cape Cod Bay, with a strewn field roughly 6 km east–west by 5 km north–south. Six radar-constrained fragment solutions have modeled masses ranging from 3.2 g to 1.425 kg. Estimates of total surviving mass vary widely: 560 kg based on an assumed 10% survival rate for an iron body, compared with 82 kg from a radar-reflectivity method that the authors describe as unvalidated and incomplete. Several observations suggest that the meteoroid was relatively dense and mechanically strong, and possibly iron-rich, although its composition has not been established. Its modeled dynamic pressure reached about 7 MPa near the terminus. The head-echo spectra showed no resolved signs of fragmentation during the observed segment, and the modeled fragment distribution contains relatively few small meteorites. The paper estimates a pre-atmospheric mass of about 5,600 kg based on an external estimate. However, the radar measurements did not resolve deceleration and therefore cannot independently determine the mass. The reconstructed orbit has a semimajor axis of 2.44 AU, an eccentricity of 0.752, and a Jupiter Tisserand parameter of 2.99, near the conventional boundary between cometary and asteroidal orbits. Empirical classification criteria produce conflicting results, and comparisons with catalogues reveal no convincing parent asteroid, comet, or established meteor-shower association. Infrasound yields an energy estimate of about 0.45–0.51 kilotons, below the CNEOS estimate of 1.1 kilotons but within the reported dispersion of empirical energy relations. The authors conclude that combining radar, weather radar, and infrasound can trace large bolides from atmospheric entry toward ground impact and help constrain their orbits and fragmentation.

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