Waveform inversion of very long period impulsive signals associated with magmatic injection beneath

We use data from broadband seismometers deployed around the summit of Kilauea Volcano to quantify the mechanism associated with a transient in the flow of magma feeding the east rift eruption of the volcano. The transient is marked by rapid inflation of the Kilauea summit peaking at 22 μrad 4.5 hours after the event onset, followed by slow deflation over a period of 3 days. Superimposed on the summit inflation is a series of sawtooth displacement pulses, each characterized by a sudden drop in amplitude lasting 5–10 s followed by an exponential recovery lasting 1–3 min. The sawtooth waveforms display almost identical shapes, suggesting a process involving the repeated activation of a fixed source. The particle motion associated with each sawtooth is almost linear, and its major swing shows compressional motion at all stations. Analyses of semblance and particle motion are consistent with a point source located 1 km beneath the northeast edge of the Halemaumau pit crater. To estimate the source mechanism, we apply a moment tensor inversion to the waveform data, assuming a point source embedded in a homogeneous half-space with compressional and shear wave velocities representative of the average medium properties at shallow depth under Kilauea. Synthetic waveforms are constructed by a superposition of impulse responses for six moment tensor components and three single force components. The origin times of individual impulses are distributed along the time axis at appropriately small, equal intervals, and their amplitudes are determined by least squares. In this inversion, the source time functions of the six tensor and three force components are determined simultaneously. We confirm the accuracy of the inversion method through a series of numerical tests. The results from the inversion show that the waveform data are well explained by a pulsating transport mechanism operating on a subhorizontal crack linking the summit reservoir to the east rift of Kilauea. The crack acts like a buffer in which a batch of fluid (magma and/or gas) accumulates over a period of 1–3 min before being rapidly injected into a larger reservoir (possibly the east rift) over a timescale of 5–10 s. The seismic moment and volume change associated with a typical batch of fluid are approximately 1014 N m and 3000 m3, respectively. Our results also point to the existence of a single force component with amplitude of 109 N, which may be explained as the drag force generated by the flow of viscous magma through a narrow constriction in the flow path. The total volume of magma associated with the 4.5-hour-long activation of the pulsating source is roughly 500,000 m3 in good agreement with the integrated volume flow rate of magma estimated near the eruptive site.

[1]  P. Okubo,et al.  Digitally Telemetered Broadband Seismic Network at Kilauea Volcano, Hawaii , 1998 .

[2]  A. D. Miller,et al.  Non‐double‐couple earthquake mechanisms at the Hengill‐Grensdalur Volcanic Complex, Southwest Iceland , 1997 .

[3]  Bernard A. Chouet,et al.  A free-surface boundary condition for including 3D topography in the finite-difference method , 1997, Bulletin of the Seismological Society of America.

[4]  J. Neuberg,et al.  Seismo-volcanic sources on Stromboli volcano , 1996 .

[5]  T. Iidaka,et al.  Mechanism of Phreatic Eruptions at Aso Volcano Inferred from Near-Field Broadband Seismic Observations , 1996, Science.

[6]  Bernard A. Chouet,et al.  Long-period volcano seismicity: its source and use in eruption forecasting , 1996, Nature.

[7]  Bernard A. Chouet,et al.  New Methods and Future Trends in Seismological Volcano Monitoring , 1996 .

[8]  M. Takeo,et al.  Source mechanism of seismic waves excited by pyroclastic flows observed at Unzen volcano, Japan , 1994 .

[9]  M. Takeo,et al.  The source of explosive eruptions of Sakurajima volcano, Japan , 1994 .

[10]  Jurgen Neuberg,et al.  Highlights from a seismic broadband array on Stromboli Volcano , 1994 .

[11]  Seismic radiation by magma injection: An anomalous seismic event near Tori Shima, Japan , 1993 .

[12]  M. Takeo The rupture process of the 1989 offshore ito earthquakes preceding a submarine volcanic eruption , 1992 .

[13]  M. Furumoto,et al.  Seismic Image of the Volcanic Tremor Source at Izu-Oshima Volcano, Japan , 1992 .

[14]  H. Yamasato,et al.  Analysis of long-period seismic waves excited by the November 1987 eruption of Izu-Oshima Volcano , 1990 .

[15]  H. Kawakatsu Centroid single force inversion of seismic waves generated by landslides , 1989 .

[16]  C. Young,et al.  Rupture of the 4 February 1976 Guatemalan earthquake , 1989 .

[17]  M. Ohtake,et al.  A monochromatic earthquake suggesting deep‐seated magmatic activity beneath the Izu‐Ooshima Volcano, Japan , 1987 .

[18]  A. Nikolaev,et al.  Lithospheric studies based on array analysis of P-coda and microseisms , 1987 .

[19]  Masayuki Kikuchi,et al.  Inversion of complex body waves-II , 1986 .

[20]  S. Sipkin,et al.  Earthquake processes in the Long Valley Caldera Area, California , 1985 .

[21]  H. Kanamori,et al.  Analysis of Seismic Body Waves Excited by the Mount St. Helens Eruption of May 18, 1980 , 1984 .

[22]  B. Julian Evidence for dyke intrusion earthquake mechanisms near Long Valley caldera, California , 1983, Nature.

[23]  H. Kanamori,et al.  Analysis of long‐period seismic waves excited by the May 18, 1980, eruption of Mount St. Helens—A terrestrial monopole? , 1982 .

[24]  Masayuki Kikuchi,et al.  Inversion of complex body waves , 1982 .

[25]  J. J. Zucca,et al.  Crustal structure of the southeast flank of Kilauea Volcano, Hawaii, from seismic refraction measurements , 1980 .

[26]  Bernard A. Chouet,et al.  Sources of seismic events in the cooling lava lake of Kilauea Iki, Hawaii , 1979 .

[27]  William L. Ellsworth,et al.  Three-Dimensional Crust and Mantle Structure of Kilauea Volcano, Hawaii , 1977 .

[28]  A. McBirney,et al.  Properties of some common igneous rocks and their melts at high temperatures , 1973 .

[29]  M. Taner,et al.  SEMBLANCE AND OTHER COHERENCY MEASURES FOR MULTICHANNEL DATA , 1971 .

[30]  M. J. Randall,et al.  The compensated linear‐vector dipole: A possible mechanism for deep earthquakes , 1970 .

[31]  G. Wallis One Dimensional Two-Phase Flow , 1969 .

[32]  M. Longuet-Higgins A theory of the origin of microseisms , 1950, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.