2
western Pacific as well, a potently anomalous zone in its own right. Without going into the details of the data analysis, we sum- marize the conclusions that can be drawn from our study of the dispersion of Rayleigh waves on the three records at the South Pole: • There is a major, high velocity anomaly at shorter surface wave periods (periods less than 250 seconds) on the Kuril path that is absent on the other two paths. The most likely candidates for the cause of this anomaly are the subduction zones of the western Pacific. The absence of this anomaly on the Sumbawa path, plus other telling signs, indicates to us that the anomaly begins to be equilibrated, or at least is not as dramatically contrasted, with the surrounding mantle at depths on the order of 400-450 kilometers under the trenches. • Okal (1977) failed to identify the high velocity anomaly near subduction zones because of the use of a regionalization of the Earth based on a 15-degree grid, aligned along parallels of latitude and longitudinal meridians. These shorter period data should be reanalyzed for shallower Earth structure with a regionalization based on the surface expression of the major plate tectonic features of the Earth. • At longer periods, an independent-layer-by-independent- layer analysis of the type carried out by Masters et al. (1982) would seem to be unjustified. The anomalies probably ex- tend across the various layers of the Earth and, if the anomaly is truly present, is not likely to be confined to the interval between 420 and 650 kilometers depth. • The mantle on the long arc between the South Pole and Los Angeles has anomalous high velocities at shallow depth rela- tive to the global average for those depths and anomalous low velocities at greater depth; the latter anomalies may extend to perhaps 450 kilometer depth or even deeper. The long-arc anomaly is consistent with the low-velocity torus of the figure. • The global reference model we have used is 1066A of Gilbert and Dziewonski (1975). • It is tempting to assign the dispersion anomaly that persists to very long periods under the Sumbawa-South Pole great circle, and its absence under the not-too-distant Kuril-South Pole great circle, to the continuation of a deep continental root to depths perhaps as great as 650 kilometers or beyond, and to the absence of this deep S-wave velocity anomaly under the oceans. This result, if confirmed, would seem to be in accord with the model of a deep continental root proposed by Knopoff (1972, 1983) and Jordan (1975). A result that indicates the existence of profound differences in the thicknesses of the lithospheres between continental shields and the oceans places significant constraints on models of convection in the Earth's mantle. S The South Pole data represent an excellent benchmark against which to check the results of modern interpretations of deep mantle structure, especially in view of the aforemen- tioned absence of significant differential ellipticity correc- tions on South Pole data. We expect this application to be ever more important as data with the growing network of ultra- long period seismic stations become more and more available. This research was supported by National Science Foundation grant DPP 81-17325. References Gilbert, F., and A.M. Dziewonski. 1975. An application of normal mode theory to the retrieval of structural parameters and source mecha- nisms from seismic spectra. Philosophical Transactions of the Royal So- ciety of London, 278A, 187-269. Jordan, T.H. 1975. The continental tectosphere. Reviews of Geophysics and Space Physics, 13, 1-12. Kawakatsu, H. 1983. Can 'pure-path' models explain free oscillation data? Geophysical Research Letters, 10, 186-189. Knopoff, L. 1972. Observation and inversion of surface wave disper- sion. Tectonophysics, 13, 497-519. Knopoff, L. 1983. The thickness of the lithosphere from the dispersion of surface waves. Geophysical Journal of the Royal Astronomical Society, 74, 55-81. Masters, G.T., T.H. Jordan, P.G. Silver, and F. Gilbert. 1982. Asphencal earth structure from fundamental spheroidal-mode data. Nature, 298, 609-613. Okal, E.A. 1977. The effect of intrinsic ocean upper-mantle hetero- geneity on regionalization of long-period Rayleigh-wave phase ve- locities. Geophysical Journal of the Royal Astronomical Society, 49, 357-370. Sedimentary petrology of Permian and Triassic Beacon sandstones, northern Victoria Land D. C. PENNINGTON and J. W. COLLINSON Institute of Polar Studies Department of Geology and Mineralogy The Ohio State University Columbus, Ohio 43210 Petrographic analyses of Beacon sandstone samples that were collected in northern Victoria Land during the 1981-1982 field season (Collinson and Kemp 1982) indicate important composi- tional differences between Permian and Triassic units. Triassic samples contain volcanic detritus; Permian samples do not. Beacon exposures in the Rennick Glacier area (figure), including the Helliwell Hills, Morozumi Range, Lanterman Range, Neall Massif, and the Freyberg Mountains, which contain a Permian Glossopteris flora, are assigned to the Takrouna Formation of Dow and Neall (1974). A relatively thin sequence of sandstone exposed along the margin of the polar plateau, including Roberts Butte, Lichen Hills, and Vantage Hills, is characterized by volcanic detritus. A Middle to Late Triassic microflora has been reported from this unit at Section Peake in the Lichen Hills (Gair et al. 1965; Norris 1965). These Triassic rocks were referred to as "Takrouna(?) Formation" by Collinson and Kemp (1983), but a new name should be assigned. 10 ANTARCTIC JOURNAL

Sedimentary petrology of Permian and Triassic Beacon …€¦ · Without going into the details of the data analysis, we sum-marize the conclusions that can be drawn from our study

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Page 1: Sedimentary petrology of Permian and Triassic Beacon …€¦ · Without going into the details of the data analysis, we sum-marize the conclusions that can be drawn from our study

western Pacific as well, a potently anomalous zone in its ownright.

Without going into the details of the data analysis, we sum-marize the conclusions that can be drawn from our study of thedispersion of Rayleigh waves on the three records at the SouthPole:• There is a major, high velocity anomaly at shorter surface

wave periods (periods less than 250 seconds) on the Kurilpath that is absent on the other two paths. The most likelycandidates for the cause of this anomaly are the subductionzones of the western Pacific. The absence of this anomaly onthe Sumbawa path, plus other telling signs, indicates to usthat the anomaly begins to be equilibrated, or at least is not asdramatically contrasted, with the surrounding mantle atdepths on the order of 400-450 kilometers under thetrenches.

• Okal (1977) failed to identify the high velocity anomaly nearsubduction zones because of the use of a regionalization ofthe Earth based on a 15-degree grid, aligned along parallels oflatitude and longitudinal meridians. These shorter perioddata should be reanalyzed for shallower Earth structure witha regionalization based on the surface expression of the majorplate tectonic features of the Earth.

• At longer periods, an independent-layer-by-independent-layer analysis of the type carried out by Masters et al. (1982)would seem to be unjustified. The anomalies probably ex-tend across the various layers of the Earth and, if the anomalyis truly present, is not likely to be confined to the intervalbetween 420 and 650 kilometers depth.

• The mantle on the long arc between the South Pole and LosAngeles has anomalous high velocities at shallow depth rela-tive to the global average for those depths and anomalous lowvelocities at greater depth; the latter anomalies may extend toperhaps 450 kilometer depth or even deeper. The long-arcanomaly is consistent with the low-velocity torus of thefigure.

• The global reference model we have used is 1066A of Gilbertand Dziewonski (1975).

• It is tempting to assign the dispersion anomaly that persiststo very long periods under the Sumbawa-South Pole greatcircle, and its absence under the not-too-distant Kuril-SouthPole great circle, to the continuation of a deep continental root

to depths perhaps as great as 650 kilometers or beyond, andto the absence of this deep S-wave velocity anomaly underthe oceans. This result, if confirmed, would seem to be inaccord with the model of a deep continental root proposed byKnopoff (1972, 1983) and Jordan (1975). A result that indicatesthe existence of profound differences in the thicknesses of thelithospheres between continental shields and the oceansplaces significant constraints on models of convection in theEarth's mantle.

S The South Pole data represent an excellent benchmarkagainst which to check the results of modern interpretationsof deep mantle structure, especially in view of the aforemen-tioned absence of significant differential ellipticity correc-tions on South Pole data. We expect this application to be evermore important as data with the growing network of ultra-long period seismic stations become more and moreavailable.This research was supported by National Science Foundation

grant DPP 81-17325.

References

Gilbert, F., and A.M. Dziewonski. 1975. An application of normal modetheory to the retrieval of structural parameters and source mecha-nisms from seismic spectra. Philosophical Transactions of the Royal So-ciety of London, 278A, 187-269.

Jordan, T.H. 1975. The continental tectosphere. Reviews of Geophysicsand Space Physics, 13, 1-12.

Kawakatsu, H. 1983. Can 'pure-path' models explain free oscillationdata? Geophysical Research Letters, 10, 186-189.

Knopoff, L. 1972. Observation and inversion of surface wave disper-sion. Tectonophysics, 13, 497-519.

Knopoff, L. 1983. The thickness of the lithosphere from the dispersionof surface waves. Geophysical Journal of the Royal Astronomical Society,74, 55-81.

Masters, G.T., T.H. Jordan, P.G. Silver, and F. Gilbert. 1982. Asphencalearth structure from fundamental spheroidal-mode data. Nature, 298,609-613.

Okal, E.A. 1977. The effect of intrinsic ocean upper-mantle hetero-geneity on regionalization of long-period Rayleigh-wave phase ve-locities. Geophysical Journal of the Royal Astronomical Society, 49,357-370.

Sedimentary petrology of Permian andTriassic Beacon sandstones, northern

Victoria LandD. C. PENNINGTON and J. W. COLLINSON

Institute of Polar StudiesDepartment of Geology and Mineralogy

The Ohio State UniversityColumbus, Ohio 43210

Petrographic analyses of Beacon sandstone samples that werecollected in northern Victoria Land during the 1981-1982 field

season (Collinson and Kemp 1982) indicate important composi-tional differences between Permian and Triassic units. Triassicsamples contain volcanic detritus; Permian samples do not.Beacon exposures in the Rennick Glacier area (figure), includingthe Helliwell Hills, Morozumi Range, Lanterman Range, NeallMassif, and the Freyberg Mountains, which contain a PermianGlossopteris flora, are assigned to the Takrouna Formation ofDow and Neall (1974). A relatively thin sequence of sandstoneexposed along the margin of the polar plateau, includingRoberts Butte, Lichen Hills, and Vantage Hills, is characterizedby volcanic detritus. A Middle to Late Triassic microflora hasbeen reported from this unit at Section Peake in the Lichen Hills(Gair et al. 1965; Norris 1965). These Triassic rocks were referredto as "Takrouna(?) Formation" by Collinson and Kemp (1983),but a new name should be assigned.

10 ANTARCTIC JOURNAL

Page 2: Sedimentary petrology of Permian and Triassic Beacon …€¦ · Without going into the details of the data analysis, we sum-marize the conclusions that can be drawn from our study

o to 20 30 40 50km

SCALE

72S

11? 1L 2 FREYBERG

00 cMOUNTAINS

C)-

Robets Butte 00

in

NM

73——__-t-1

Pain a73

0

Tobin Mesa

(Gaa MesaZe9

-Vulcan Hills

160E 162E t64E

Locality map of northern Victoria Land. ("km" denotes kilometer.)

Both Permian and Triassic units rest directly on basementrocks in their respective regions. Known thicknesses of theTakrouna Formation, which do not exceed 300 meters, are in-complete and therefore probably represent only part of thePermian. Triassic thicknesses, which are up to 45 meters, repre-sent only the upper part of the Triassic. Volcanic influx, there-fore, began in the northern Victoria Land region during LatePermian or Early Triassic. In southern Victoria Land, volcanicdetritus occurs lowest in the Fleming Member of the FeatherFormation, which is probably Lower Triassic (Collinson, Pen-nington, and Kemp 1983). In the central Transantarctic Moun-tains, volcanic influx began during the deposition of the UpperPermian Buckley Formation (Barrett 1969).

Modal analyses of 53 samples (300 points per sample) indicatethat sandstones of the Takrouna Formation range in composi-tion from quartzarenite to subfeldsarenite and, in three cases,feidsarenite (classification of Folk, Andrews, and Lewis 1970).Detrital grains include quartz, feldspar, biotite, muscovite,crystalline and metasedimentary lithic fragments, and heavyminerals. Quartz grains are typically unstrained to slightly un-dulose; polycrystalline grains make up less than 10 percent.Quartz grains are mostly subangular to subrounded and com-monly display syntaxial overgrowths. Feldspar content rangesup to 25 percent and is almost entirely potassium feldspar,except in samples from Neall Massif where plagioclase is com-mon, but not dominant. Potassium feldspar grains are micro-dine and orthoclase in approximately equal amounts. The

source terrain, which was probably the local basement rocks,was dominated by acidic crystalline rocks, but included low-grade metasedimentary rocks.

Eighteen samples of Triassic sandstones along the margin ofthe polar plateau range from subfeldsarenite to volcanic feld-sarenite in composition. Detrital constituents include quartz,feldspar, biotite, muscovite, heavy minerals, and crystalline,volcanic, and metasedimentary lithic fragments. Quartz isdominated by unstrained to slightly undulose grains. Grainsare subangular to subrounded, clear (rarely contain inclusions),and are commonly embayed. Syntaxial overgrowths are rare.Feldspar constitutes 10-25 percent of samples and both pla-gioclase (andesine) and potassium feldspar occur in equalamounts. Lithic fragments are dominated by felsic volcanicclasts. Other volcanic grains include fragments with euhedralplagioclase microlites that are either randomly oriented or ex-hibit pilotaxitic texture, minor mafic fragments that consist ofplagioclase microlites in a hematitic groundmass, andtuffaceous fragments that contain altered shards. Zeolite, prob-ably laumontite, occurs as cement.

A sample from the top of a 18-meter-thick section at RobertsButte is a crystal tuff. It contains approximately 50 percentcrystals of anhedral quartz, which in some cases are embayed,anhedral to subhedral plagioclase (andesine), subhedralorthoclase, microcline, and less common sanidine, and biotite.Volcanic rock fragments are common. The groundmass consistsof quartz and feldspars with abundant shards, which appear tobe welded in places, and abundant glass.

Detrital modes of Triassic sandstones suggest a source terraindominated by acidic to intermediate volcanic rocks. These rocksare similar to volcaniclastic rocks of Triassic age that occur alongthe Transantarctic Mountains from the Nielsen Plateau to north-ern Victoria Land (Elliot 1975).

This work was supported in part by National Science Founda-tion grant DPP 80-20098.

References

Barrett, P.J. 1969. Stratigraphy and petrology of the mainly fluviatilePermian and Triassic Beacon rocks, Beardmore Glacier, Antarctica.Institute of Polar Studies Report 34.

Collinson, J.W., and N.R. Kemp. 1982. Sedimentology of the TakrounaFormation, a Permian-Triassic fluvial deposit in northern VictoriaLand. Antarctic Journal of the U.S., 17(5), 15-17.

Collinson, J.W., and N.R. Kemp. 1983. Permian-Triassic sedimentarysequence in northern Victoria Land, Antarctica. In R.L. Oliver, P.R.James, and J.B. Jago (Eds.), Antarctic earth science. Australian Acade-my of Science, Canberra.

Collinson, J.W., D.C. Pennington, and N.R. Kemp. 1983. Sedimentarypetrology of Permian-Triassic fluvial rocks in Allan Hills, centralVictoria Land. Antarctic Journal of the U.S., 18(5), 20-22.

Dow, J.A.S., and V.E. Neall. 1974. Geology of the lower Rennick Glacier,northern Victoria Land, Antarctica. New Zealand Journal of Geology andGeophysics, 17, 659-714.

Elliot, D.H. 1975. Gondwana basins of Antarctica. In K.S.W. Campbell(Ed.), Gondwana Geology. Canberra: Australia National UniversityPress.

Folk, R.L., P.B. Andrews, and D.W. Lewis. 1970. Detrital sedimentaryrock classification and nomenclature for use in New Zealand. NewZealand Journal of Geology and Geophysics, 13, 937-968.

Gair, H.S., G. Norris, and J. Ricker. 1965. Early Mesozoic microflorasfrom Antarctica. New Zealand Journal of Geology and Geophysics, 8,231-235.

Norris, G. 1965. Triassic and Jurassic miospores and acritarchs from theBeacon and Ferrar Groups, Victoria Land, Antarctica. New ZealandJournal of Geology and Geophysics, 8, 236-277.

1984 REVIEW 11