testing deformation-enhanced element mobility in...
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Testing Deformation-Enhanced Element Mobility in PlagioclaseNaomi Barshi*, Christie Rowe, and Vincent van HinsbergDepartment of Earth and Planetary Sciences, McGill University, Montréal, QC, Canada
Why do we care?
How can deformation enhance element mobility?
Where can we study this?
What changes along the map-scale strain gradient? What should change at the grain scale?
Deformation at Meter to Micrometer Scales
Strain
Chemistry
Plagioclase Phenocrysts
Pressure and Temperature
What does this boil down to?
Where did the information come from?
Who helped us?
Variable gabbro,diorite and tonalite;some hypabyssal
Hornblende-biotite tonalite
Gabbro
Probable magmaticring complexes
Mafic cone-sheetassemblages
Ensenada
La Paz
115oW 110oW
29oN
33oN
Maparea
PacificOcean
San Diego
USA
México
Gulf of California
Baja California
Country rocks
Outer Unit
Central Unit
Sampling transects
1 km
115º40’W31º05’N
30º55’N
115º50’W
Other Intrusives
San José tonalite
Metasediments/Metavolcanics
106 Ma
103 Ma
105 Ma
Northwest Northeast
5 mm
0
0.5
1
1.5
2
2.5
3
640 660 680 700 720 740 760 780
Pres
sure
(kb
ar)
Temperature (ºC)
Results of Plagioclase-Hornblende Thermobarometry
MX23
MX05
MX08
MX16
MX11
MX14
MX13
-90
-75
-60
-45
-30
-15
0
15
30
45
60
75
90
1 2 3 4 5
-90
-75
-60
-45
-30
-15
0
15
30
45
60
75
90
1 2 3 4 5 6 7 8
-90
-75
-60
-45
-30
-15
0
15
30
45
60
75
90
1 2 3 4 5
Orientation and Shape in Samples
~115-97 Ma E
?
W
North America6-8 km depth
Strain
Com
posi
tiona
l Con
tras
ts
Detecti
on Li
mits
This study
Measurable strain enhanced diffusion
500 µm subgrains faint, straight twins
curved twins
l0
lb
100 µm
∆G
Distance
A B C D E
20
25
30
35
40
45
50
0.1
0.15
0.2
0.25
0.3
0 0.5 1 1.5 2 2.5 3 3.5 4
Var
iati
on in
Ori
enta
tion
(a
ngle
from
hor
izon
taal
in d
egre
es)
Phen
ocry
st P
ropo
rtio
n (%
of t
hin
sect
ion
area
)
Distance from Pluton Edge (log m)
Plagioclase Phenocryst Abundance and Orientation
Aspect Ratio
Angle Between Long Axis and
Reference Line
Rigid-body rotation
Reference Rotation and internal deformation
Idealized Relationships Between Orientation and Shape
0.30
0.35
0.40
0.45
-100 -75 -50 -25 0 25 50 75
Ano
rthi
te P
ropo
rtio
n
Distance from boundary (µm)
Calcium Diffusion Profiles (EPMA)
210
260
310
360
410
460
510
560
1350
1400
1450
1500
1550
1600
1650
1700
-60 -40 -20 0 20 40 60
Ba
Con
cent
rati
on (
ppm
)
Sr C
once
ntra
tion
(pp
m)
Distance from zone boundary (µm)
Tracel Element Profiles (LA-ICP-MS)
0 100 200 300 400 500 600 700
Ba La Li Mg
Pb Rb Sr
An100 with 0.004 wt% H2O
An100 with 0.07 wt% H2O
An60 with 0.3 wt% H2O
Ab100 with 0.2 wt% H2O
Dislocation Creep
Diffusion Creep
Diffusion
An100 with 0.004 wt% H2O
An100 with 0.07 wt% H2O
An60 with 0.3 wt% H2O
Ab100 with 0.2 wt% H2O (Ryb
acki
and
Dre
sen,
200
4)
(Agg
rega
ted
data
for
~A
n 30 fr
om B
rady
and
C
hern
iak,
201
0)
Activation Energy (kJ/mol)
Study area of fully-exposed strain gradient in tonalite with compositionally zoned plagioclase phenocrysts which serve as physical and chemical strain markers. Maps modified from Johnson et al.4
and sattelite image from Digital Globe/GoogleEarth 2014.
Vacancy and atomic migration amount to lattice deformation. (Figure after Porter and Easterling1, Fig. 2.6.)
Strain gradient sample locations, with ranch for scale.
Magmatic alignments, Hbl dominates mafic phases
Bt flattening, increasing Plg alignment
Connected Bt, fewer Plg phenocrysts, smaller Hbl
Solid-state, Bt foliation, Plg phenocrysts rare
Strain adds energy to the lattice, making the atomic jumps easier (cyan line on graph above). Activation energies for diffusion and deformation are similar, for example in plagioclase2,3.
For this small strain, deformation-enhanced element mobility cannot be measured in plagioclase with present methods. However, previous work6,7 in silicates indicates it can be measured in natural samples. Future work should explore variables such as compositional contrasts, strain, time, temperature, pressure, thermal history, and analytical methods to constrain the realm of deformation enhanced diffusion.
Dislocations provide efficient travel paths that mobilize during deformation.
Thanks to the Field Rheology and FlexPet groups at McGill University for support and assistance. Thanks to Lang Shi for help with the electron microprobe at McGill, André Poirier for help with the LA-ICP-MS at UQÀM/GEOTOP, and Matt Paulson for help in the field. This project was funded by NSERC (van Hinsberg and Rowe), FQRNT (Rowe), GEOTOP and GREAT (Barshi), and a Robert Wares Fellowship (Rowe). Thanks also to Scott Johnson and John Brady for invaluable advice and discussions.
Point Defects
Activation EnergyLine Defects
1. Porter, D. A., Easterling, K. E., 1989. Phase Transformations in Metals and Alloys. 2. Brady, J. B., Cherniak, D. J., 2010. Reviews in Mineralogy and Geochemistry 72 (1), 899–920.3. Rybacki, E., Dresen, G., 2000. Tectonophysics 382, 173–187.4. Johnson, S. E., Tate, M. C., Fanning, C. M., 1999. Geology 27, 743–746. 5. Holland, T., Blundy, J., 1994. Contributions to Mineralogy and Petrology 116 (4), 433–447.6. Büttner, S. H., Kasemann, S. A., 2007. American Mineralogist 92 (11), 1862–1874.7. Reddy, S. M., Timms, N. E., Trimby, P., Kinny, P. D., Buchan, C., Blake, K., 2006. Geology 34 (4), 257–260.
Strongly deformed, phenocrysts rare, strong alignment in foliation
Ellipses fit to Plg phenocrysts circled in thin sections show rotation with little internal deformation. Here the reference line is foliation.
Phenocrysts decrease in abundance and size with increasing strain toward the edge of the pluton. Decreasing variation of phenocryst long axes shows increasing preferrent alignment.
Pressures and temperatures measured in plagioclase and hornblende5 do not vary with strain indicating no systematic fluid overprint nor divergent thermal history.
• Total integrated elongation: 1.5±.5% at the composition zone boundary (cyan line)
• Localized strain in the hinge of the bend: total elongation of 11±2%.
Three intragrain regions accommodate extension with different deformation mechanisms. The shortening direction is approximately vertical to this grain, consistent with the elongation direction (measured in oriented thin section) and flattening of the pluton carapace.
Thin section scan, xpl Photomicrograph, xpl
We anticipated that diffusion profiles would be more smooth with increasing strain for the same elements (here Ca) and that more slowly diffusing species (Ba) would show more sharp steps than more rapid diffusers (Sr). Rather, we see perfect, consistent major element profiles. Trace element profiles have variation which cannot be accounted for.
We measured diffusion profiles and strain in zoned plagioclase phenocrysts with complete internal strain gradients. This way, we control for variables such as starting concentrations, magmatic history, and crystallographic orientation effects. We present results from the grain with highest strain, nicknamed “MTL”.
Undeformed, little to no magmatic alignment
Very low strain, strong magmatic alignment, long
phenocrysts
Least deformed
Most deformed
Optical and compositional image overlay
If deformation enhances element mobility in minerals:
• Geochronometers, thermometers, and barometers based on static diffusion models cannot be applied to deformed rocks.
• Deformation can be directly linked to a time-dependent process as a basis for a strain speedometer.
EAct EAct