g.f. ndlovu 1 , t.i. ivankina 2 , r.n. vasin 2

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The study of Quartz Textures in Multiphase rocks using Neutron Diffraction Texture Analysis at the JINR, Dubna JINR, Summer Student Practice, September 2009 G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2 1 Council for Scientific and Industrial Research (CSIR), Pretoria, South Africa 2 Frank Laboratory of Neutron Physics, Joint Institute for Nuclear Research, Dubna, Russia

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The study of Quartz Textures in Multiphase rocks using Neutron Diffraction Texture Analysis at the JINR, Dubna. G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2. 1 Council for Scientific and Industrial Research (CSIR), Pretoria, South Africa - PowerPoint PPT Presentation

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Page 1: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

The study of Quartz Textures in Multiphase rocks using Neutron Diffraction Texture Analysis

at the JINR, Dubna

JINR, Summer Student Practice, September 2009

G.F. Ndlovu1, T.I. Ivankina2, R.N. Vasin2

1 Council for Scientific and Industrial Research (CSIR), Pretoria, South Africa2 Frank Laboratory of Neutron Physics, Joint Institute for Nuclear Research,

Dubna, Russia

Page 2: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Main topics • Why Quartz

• Why measure texture• Goals • Methods• Results

• Experimental• Theoretical

• Conclusions• Acknowledgements

Page 3: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Why Quartz• Most common compound in the Earth’s Crust (SiO2 ) and most useful• Occurs in all environments and all rock types - sedimentary,

metamorphic or igneous• Its piezoelectric properties make it highly useful in modern technology

Outokumpu Deep Drilling Project depth - 2516 m

OKU 818Composition- quartz (~40%)- mica (~30-40%)- plagioclase (~20-30%)

Page 4: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Why do geologists measure texture?• The modelling of physical anisotropies (seismic wave velocities, heat

conductivity, thermal expansion, magnetic, piezoelectric, etc.) of rocks

Deconvolution of the deformation history of rocks on the basis of the symmetry of the mineral textures, which commonly reflect the symmetry of deformation

Texture Property Rock sample (marble)

Single crystal

Page 5: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Crystallographic texture

Many materials are polycrystalline bodies, i.e. they consist of grains (crystallites) with a different size and orientation.

Crystallographic texture is the lattice (or crystallographic) preferred orientation of crystallites of the same phase (mineral) in the chosen coordinate system: LPO (or CPO).

Random orientation:NO crystallographic

texture

Aligned grains:One-component

crystallographic texture

Multi-component crystallographic texture

The properties of the polycrystal are anisotropic and depend upon texture

Page 6: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Objectives• Learn about the operation of the SKAT diffractometer

– Measure the diffraction spectra of geological samples (quartz-bearing)

• Use AutoIndex, GeoTOF, Pole Figure plot and Beartex programs – Indexation of spectra– Extracted experimental pole figures from spectra– Obtain quantitative 3D orientation distribution function (ODF)- quantitative measure

of texture

Page 7: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Experimental

using neutrons creates completely new possibilities, some of which are unique and inaccessible by x rays

Main Advantages of Neutron Diffraction Technique

• low absorption of neutrons in matter »large sample volumes accessible• TOF » complete diffraction patterns can be recorded• application of multiple detectors » measurements are fast• excellent spectral resolution » suitable for polyphase geological samples with many diffraction lines• unique scattering angle 2 of all detectors » minimum of intensity corrections required

Texture diffractometer SKAT operates in the beam of the reactor IBR-2 (JINR, Dubna, Russia). 19 detectors are placed completely on the assembly ring maintaining the axial symmetry with respect to the neutron beam

SA ASS

A

Methods

Schematic view of the SKAT’s detector system. 19 detector modules named from A to S, with S in the center of the pole figure.

The line on the unit sphere corresponds to the scattering vectors of detector ring, line in the XY plane is its stereographic projection.

The grid of the measured pole figure. Small circle corresponds to the plane projection of the scattering vectors, dots shown where the data on pole density are situated.

Pole sphere Pole figure raster

Page 8: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Mathematic description of the crystallographic texture: orientation distribution function (ODF) f(g), where (g) corresponds to the rotation to align the coordinate system of the sample Ka with the coordinate system of the crystallite Kb.

Xb

Zb

Yb

β

γ

α

Theoretical Methods

(Xa,Ya,Za): Ka – right-handed, Cartesian sample coordinate system.(Xb,Yb,Zb): Kb – right-handed, Cartesian crystal coordinate system.

Quantitatively the orientation of the certain crystallite (g) is described by three Euler angles g={α,β,γ}. All the possible orientations (0 ≤ α,γ ≤ 2π; 0 ≤ β ≤ π) form the orientation G-space.

f (g) describes the volumetric fraction of crystallites with the orientation g+dg. It is normalized to 1:

The traditional method for the representation of preferred orientations is pole figures, i.e.,stereographic projection of the normals to the planes (hkl). A pole figure gives an answer to the question:Which volume fraction of the sample have a orientation for which the lattice plane normal coincide with a sample direction Z

Spherical coordinates of normal to crystalographic plane (001) ( pole P2)

Neutron diffraction quartz PF (11-20)

stereographic projection of pole Р 2

Page 9: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Data processingNormalized diffraction spectra

Experimental pole figures (measured simultaneously due to application of TOF-method)

Calculation of the ODF (WIMV method)

Recalculation of pole figures using the ODF•(0001) - absent reflection•(11-20),•(10-11), (01-11) – overlapped.

ODF characteriztion: texture index F2, construction of the ODF-histogram and ODF-spectrum

Page 10: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Crystallographic textures that are characteristic of quartzites

Dauphine twins, type I: two crystals, one rotated around [0001] on 180°. Pole figures, stereographic projection, linear scale contours.

Model texture, type II(type I + misorientation)Pole figures, stereographic projection, linear scale contours.

A.N. Nikitin, T.I. Ivankina, K. Ullemeyer, R.N. Vasin, 2008, published in Kristallografiya, 2008, Vol. 53, No. 5, pp. 859–866

PFs exhibit strong, symmetrically dependent peaks of high pole density

Differ from the first-type textures by diffused peaks and lower pole density

Page 11: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Model texture, type III(rotation around normal to (02-23))Pole figures, stereographic projection, linear scale contours, rotation axis direction: left to right.

Model texture, type IV(rotation around normal to (02-21))Pole figures, stereographic projection, linear scale contours, rotation axis direction: left to right.

Analogous quartz textures in different rocks

The (001) PF exhibits a diffused pole-density peak with a tendency to waist distribution of c axes along small-circle arcs

Page 12: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Results(1

1-21

)

Experimental pole figures

TOF-chanels

Inte

nsity

, a.u

(10-

11)

(10-

10)

(11-

20)

(10-

12)

Recalculation of pole figures using the ODF•(11-21),(01-11) - absent reflection•(10-11), (01-12) – overlapped

Fig. 1. Diffraction spectrum and pole figures corresponding to indexed reflections for the OKU 818 quartzite sample

•The main objective of texture analysis is to obtain information on the crystal orientation distribution in the sample•Incomplete pole figures and regions of the diffraction spectrum containing overlapping peaks

Page 13: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

001 110 101 011

0.3 1.6 0.5 1.3 0.6 1.3 0.6 1.6

Recalculated pole figures of the principle crystallographic planes

• The texture of a polycrystalline sample is a statistical ensemble of crystallites. • A statistically representative number of crystallites or grains is needed to obtain reliable information. • Obtaining reproducible pole figures requires 104–105 grains

Page 14: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Conclusions• Experimental PFs were used to reconstruct ODFs, on the basis of which PFs were calculated for

the principal directions in quartz bearing rock samples

• The rock sample under study exhibit a strong quartz texture (the maximum pole density > 1.56)

• Pole figure data processing yielded the complete texture for quartz

• In addition to the mineral textures factors like oriented, microcracks and grain boundaries control the elastic properties of rock samples

• Useful in studying how quartz grains interact with or are affected by other minerals during deformation

Remarks – Improve the intensity/background ratio and increase the flux of thermal neutrons at the sample position

Page 15: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Acknowledgements• Many thanks to the following Organisations and

Personnel

– JINR, Dubna – FNL, JINR, Dubna

• Dr. Tatyana Ivankina• Dr. Roman Vasin

– The NRF• Dr. Noel Jacobs

– The CSIR & Univ of Free State• Prof. Thembela Hillie• Prof. Wiets Roos

Page 16: G.F. Ndlovu 1 , T.I. Ivankina 2 , R.N. Vasin 2

Thank You!