Jökull


Jökull - 01.12.1984, Page 75

Jökull - 01.12.1984, Page 75
Inhomogeneous magnetization Measurement of sample ing, however, may prevent one from obtaining in different positions, samples of optimum size and shape from a lava. averaeed ANISOTROPY EFFECTS Interference from induced magnetization in earth’s field Viscous or isothermal remanence present Weak magnetization Large uncertainty in direction and pole latitude, especially if inclination is low Spinning of sample, or field nulling by Helmholtz coils a.f. demagnetization until primary direction is isolated Variable amplification of signal Accuracy of each measurement a few degrees. Pole pos. calculated from 3-5 samples/flow. To give some crude numbers on the relative certainty of correct polarity determination (excluding errors from geological sources, such as remagnetization), one may estimate that a care- ful fluxgate determination of lava polarity is likely to be correct about 80% of the time, but laboratory measurements will yield an unambi- guous polarity up to 95% of the time. For this, it may be necessary to omit occasional samples, e.g. those suspected of being for some reason incorrectly oriented. The reasons for ambiguous results in 5% of Icelandic lava flows have not yet been fully investigated, but this will be dealt with below. It is possible that in some cases secondary remanent magnetizations have higher coercivities (stability) than the primary remanence. Resampling flows at a different site and/or at a different height in the flow has been found to resolve directional ambiguities in perhaps every other case, but sometimes the resampling only brings added con- fusion. Very fine-grained lavas, thin lavas, and colum- nar basalts may be more prone than others to instability and to acquiring secondary magnetiza- tion, especially if altered. Felspar-porphyritic lavas generally seem rather stable. In this context it should also be mentioned that weathering of lavas affects only the glassy phase in the rocks but is not harmful to the opaque minerals. Weather- It has been noted (e.g. Kristjansson and McDougall 1982) that paleomagnetic directions from Icelandic lavas, while apparently very reli- able and internally consistent, are more scattered than would be expected by comparison with data from other formations of similar age. It has therefore been suggested that possibly grain orientation effects during flow and cooling of these lavas may cause magnetic anisotropy, tending to align remanence directions towards the horizontal plane. Anisotropy effects in some basalt lava flows and dikes have been investigated by Ellwood (1978), using a low-field torsion balance. He finds that there is very little evidence for systema- tic anisotropy effects in Icelandic lavas, and sug- gests that various randomizing effects during the flow dominate over horizontal flow- or stress- induced anisotropy. The present author has introduced a strong anhysteretic magnetization into some 15 cylindri- cal basalt samples. The A.R.M. was applied at right angles to the drilling direction of these, which was on average at 33° below the horizontal. In this experiment the anisotropic component appeared to be generally at or below 3%, which was also the level of systematic errors in the instrument used. Anisotropy does therefore not seem to be a serious factor in determining the remanence direction of basalt lavas. However, its effect may possibly be larger in acid and andesitic lavas where flow structures are visually evident. This has not yet been investigated in Iceland. At the moment the main reason for the large between-lava scatter of paleomagnetic directions in Iceland appears to lie in properties of the geomagnetic field, caused by conditions in the Earth’s core. DIFFERENCES BETWEEN MAGNE- TICALLY STABLE AND UNSTABLE SAMPLES Among the magnetic differences observed between magnetically stable samples from Ice- land on one hand and unstable samples on the other, is the fact that median destructive fields for the original T.R.M. of stable samples are JÖKULL 34. ÁR 73
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