HR: 1340h
AN: GP33A-0090 [Abstracts]
TI: A Paleomagnetic and Magnetic Anisotropy Study of the Carboniferous Shepody Formation, New Brunswick and
Nova Scotia, Canada: Possible Evidence for Inclination Shallowing in Continental Red Beds.
AU: * Bilardello, D
EM: dabc@lehigh.edu
AF: Lehigh University, EES
31, Williams Dr., Bethlehem, PA 18015
United States
AU: Kodama, K P
EM: kpk0@lehigh.edu
AF: Lehigh University, EES
31, Williams Dr., Bethlehem, PA 18015
United States
AB:
To check the validity of the Tan and Kodama [2002] hematite inclination correction, the Carboniferous red beds of the Shepody
Formation (Hopewell Group, New Brunswick and Nova Scotia, Canada) were sampled. A detailed magnetic stratigraphy for these
rocks had been previously reported by DiVenere and Opdyke [1990, 1991]. The corrected paleopoles could then be compared to
inclination-corrected paleopoles from the coeval Mauch Chunk Formation and Glenshaw Formation of Pennsylvania.
Stepwise thermal demagnetization and chemical demagnetization were used on standard sized cores to isolate the characteristic
remanence (ChRM). The two thermally and chemically treated populations yielded identical mean directions at the 95%
confidence level, with mean D= 357.5°, I= -18° and α95= 4.7°, corresponding to a paleopole position of
34.7° N, 118.5° E, A95= 3.9°.
Anisotropy of magnetic susceptibility (AMS) was measured for all samples and for each chemical demagnetization step to apply
an inclination correction.
Samples from different sites were divided into two groups, based on their AMS foliation. The individual particle anisotropy
was estimated by fitting corrected directions to theoretical correction curves [Tan and Kodama, 2003] as a function of
individual particle anisotropy. The best fit suggests that individual particle anisotropies of a= 1.07 and 1.15 should
be used for the Shepody Formation; however, the corrected directions (D= 178.3° I= 47.6°, α95= 13.7°)
have a strongly elliptical distribution. Assuming that a circular, or azimuthally uniform, distribution would be closer to
that caused by random errors in measurement and orientation, a correction using a= 1.1 and 1.4 was made because it
gives both an acceptable fit to the theoretical curves and an azimuthally uniform directional distribution. The uniformity of
the directional distribution was calculated by Mu [Fisher et al., 1987; Tauxe, 1993]. The mean corrected direction of D=
177.9°, I= 29.1°, α95= 8.4° yields a corrected paleopole at 27.8° N, 117.8° E, A95=
6.6°. This pole position agrees remarkably well with the inclination-corrected Carboniferous red bed paleopole of the
Mauch Chunk Formation, northeastern PA (27.9° N, 110.4° E, A95= 8.7°) [Kodama, 2005], with the corrected pole
of the Carboniferous magnetite-bearing rocks of the Conemaugh Group of southwestern PA (24.5° N, 116.9° E, A95=
8.7°) [Kodama, 2005], and a re-calculated Carboniferous red bed paleopole of the Maringouin Formation of New Brunswick,
Canada (31.4° N, 114.3° E, A95= 7.3°) from data of Newton and Kodama [2004] and new data from this study. The
mean pole position lies at 27.9° N, 114.9° E, A95= 4.6°, N= 4.
Because individual particle anisotropy is difficult to determine experimentally for hematite-bearing sedimentary rocks,
partial thermal remanence magnetization (pTRM) experiments were performed in order to determine remanence anisotropy and
better constrain the a value. pTRM experiments show a distinctive remanence anisotropy fabric in sample core
coordinates, but not in geographic and/or stratigraphic coordinates, indicating that the fabric is an artifact of the
experimental set up. A different method for measuring remanence anisotropy involving high field isothermal remanence will be
tested in order to constrain the a value.
DE: 1599 General or miscellaneous
SC: Geomagnetism and Paleomagnetism [GP]
MN: Fall Meeting 2005