Surface movements of emplaced lava flows measured by synthetic aperture radar interferometry

Lava flows continue to move after they have been emplaced by flow mechanisms. This movement is largely vertical and can be detected using differential synthetic aperture radar (SAR) interferometry. There are three main components to this motion: (1) movement of surface scatterers, resulting in radar phase decorrelation, (2) measurable subsidence of the flow surface due to thermal contraction and clast repacking, and (3) time-dependent depression of the flow substrate. These effects act in proportion to the thickness of the lava flow and decay with time, although there is a time lag before the third component becomes significant. We explore these effects using SAR data from the ERS satellites over the Etna volcano, Sicily. Phase decorrelation on young, thick a’a lava flows persists for a few years and probably results from surface block rotations during flow contraction. Maximum measured subsidence rates of the 1991–1993 lava flow over a period of 70 days are about 0.7 mm day−1, but are potentially greater in areas of data decorrelation. These rates fall to <2.7×10−2 mm day−1 after about 20 years in flows about 50 m thick, sooner for thinner flows. Comparison with measured subsidence rates on Kilauean lava lakes suggests that thermal contraction only accounts for about one third of the observed subsidence. The remaining motion is thought to come from surface clast repacking during cooling and from creep mechanisms in the flow substrate. Measurements of postemplacement surface movement provide new constraints on the thermomechanical properties of lava flows and have cautionary implications for the interpretation of interferometric SAR data of volcanoes. © 2001 American Geophysical Union.

[1]  J. Muller,et al.  The potential use of phase coherence time series and LANDSAT-TM in predicting IfSAR scatterer behaviour on Mt. Etna volcano , 2000 .

[2]  Charles A. Williams,et al.  Post-emplacement lava subsidence and the accuracy of ERS InSAR digital elevation models of volcanoes , 2001 .

[3]  R. Bamler,et al.  Phase statistics of interferograms with applications to synthetic aperture radar. , 1994, Applied optics.

[4]  Nick Marechal Tomographic formulation of interferometric SAR for terrain elevation mapping , 1995, IEEE Trans. Geosci. Remote. Sens..

[5]  G. Wadge,et al.  Lava flow volume and morphology from digitised contour maps : a case study at Mount Etna, Sicily , 1999 .

[6]  F. Birch,et al.  SECTION 7: COMPRESSIBILITY; ELASTIC CONSTANTS (See also Section 9) , 1966 .

[7]  M. Shepard,et al.  Lava flow surface roughness and depolarized radar scattering , 1996 .

[8]  Riccardo Lanari,et al.  Dynamic deformation of Etna Volcano observed by satellite radar interferometry , 1998 .

[9]  Howard A. Zebker,et al.  Decorrelation in interferometric radar echoes , 1992, IEEE Trans. Geosci. Remote. Sens..

[10]  F. Rocca,et al.  Seismic Migration For Sar Focusing: Interferometrical Applications , 1990 .

[11]  J. Garvin,et al.  Lava flow topographic measurements for radar data interpretation , 1993 .

[12]  S. Calvari,et al.  Formation of lava tubes and extensive flow field during the 1991–1993 eruption of Mount Etna , 1998 .

[13]  K. Feigl,et al.  The displacement field of the Landers earthquake mapped by radar interferometry , 1993, Nature.

[14]  Charles Werner,et al.  Accuracy of topographic maps derived from ERS-1 interferometric radar , 1994, IEEE Trans. Geosci. Remote. Sens..

[15]  D. Massonnet,et al.  Deflation of Mount Etna monitored by spaceborne radar interferometry , 1995, Nature.

[16]  Zhong Lu,et al.  Synthetic aperture radar interferometry of Okmok volcano, Alaska: radar observations , 2000 .

[17]  Lisa R. Gaddis,et al.  Geologic analyses of Shuttle Imaging Radar (SIR-B) data of Kilauea Volcano, Hawaii , 1989 .

[18]  Lisa R. Gaddis,et al.  Lava flow surface textures - SIR-B radar image texture, field observations, and terrain measurements , 1990 .

[19]  Richard M. Goldstein,et al.  Studies of multibaseline spaceborne interferometric synthetic aperture radars , 1990 .

[20]  G. Wadge,et al.  The volume and shape of the 1991–1993 lava flow field at Mount Etna, Sicily , 1997 .

[21]  Christophe Delacourt,et al.  Tropospheric corrections of SAR interferograms with strong topography. Application to Etna , 1998 .

[22]  Didier Massonnet,et al.  Reduction of the need for phase unwrapping in radar interferometry , 1996, IEEE Trans. Geosci. Remote. Sens..

[23]  K. Feigl,et al.  Radar interferometry and its application to changes in the Earth's surface , 1998 .

[24]  J. Murray The influence of loading by lavas on the siting of volcanic eruption vents on Mt Etna , 1988 .

[25]  R. Bamler,et al.  Synthetic aperture radar interferometry , 1998 .

[26]  Stevens Nf Lava flow volume and morphology from ERS synthetic aperture radar interferometry. , 1999 .

[27]  P. Long,et al.  Two-stage vesiculation in the Cohassett flow of the Grande Ronde Basalt, south-central Washington , 1987 .

[28]  P. C. Grew,et al.  Stress corrosion theory of crack propagation with applications to geophysics , 1977 .

[29]  Jan-Peter Muller,et al.  Volcano monitoring using interferometric SAR , 1997 .

[30]  P. Rosen,et al.  Atmospheric effects in interferometric synthetic aperture radar surface deformation and topographic maps , 1997 .

[31]  Peter J. Mouginis-Mark,et al.  The effect of varying acquisition parameters on the interpretation of SIR-C radar data: The Virunga volcanic chain☆ , 1997 .

[32]  Paolo Papale,et al.  The evolution of lava flows from ephemeral vents at Mount Etna: Insights from vesicle distribution and morphological studies , 1997 .

[33]  Rosalind J Wright,et al.  Cooling mechanisms and an approximate thermal budget for the 1991–1993 Mount Etna lava flow , 1997 .

[34]  D. L. Peck Cooling and vesiculation of Alae lava lake, Hawaii , 1978 .

[35]  Maria Luisa Carapezza,et al.  The control of lava flow during the 1991 1992 eruption of Mt. Etna , 1993 .

[36]  Effects of compressibility on the flow of lava , 1991 .

[37]  M. C. Kleinrock,et al.  The magma body at Kilauea Iki lava lake: Potential insights into mid-ocean ridge magma chambers , 1994 .

[38]  Fabio Rocca,et al.  The wavenumber shift in SAR interferometry , 1994, IEEE Trans. Geosci. Remote. Sens..

[39]  Didier Massonnet,et al.  Atmospheric Propagation heterogeneities revealed by ERS‐1 interferometry , 1996 .

[40]  Lars M. H. Ulander,et al.  Repeat-pass SAR interferometry over forested terrain , 1995 .

[41]  Pierre Briole,et al.  Volcano‐wide fringes in ERS synthetic aperture radar interferograms of Etna (1992–1998): Deformation or tropospheric effect? , 2000 .

[42]  P. Rosen,et al.  Analysis of Active Lava Flows on Kilauea Volcano, Hawaii, Using SIR-C Radar Correlation Measurements , 1996 .

[43]  Christophe Delacourt,et al.  Post‐eruptive deformation associated with the 1986–87 and 1989 lava flows of Etna detected by radar interferometry , 1997 .

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

[45]  M. Manga Waves of bubbles in basaltic magmas and lavas , 1996 .

[46]  Zhong Lu,et al.  Synthetic aperture radar interferometry coherence analysis over Katmai volcano group, Alaska , 1998 .

[47]  Giorgio Franceschetti,et al.  SIR‐C/X‐SAR multifrequency multipass interferometry: A new tool for geological interpretation , 1996 .