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sgr ms thesis - University of Maine

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This thermal fracture model explains the late stage fracture for diorite<br />

clasts, but it does not take into account the anisotropic nature <strong>of</strong> the Bar Harbor<br />

Formation. Rock heterogeneity creates a far more complex thermal stress<br />

problem because crack formation is not solely dependent on the thermal<br />

gradient. Clarke et al. (1998) discuss the three different possibilities for fracture<br />

development in anisotropic xenoliths. The first is determined by the thermal<br />

gradient and this is used in the above model (thermal gradient cracking). The<br />

second mechanism for crack formation in a layered material becomes operative<br />

when one layer has a differing thermal expansion coefficient than its counterpart<br />

(thermal expansion mismatch cracking). Third, a material may have an<br />

anisotropic fabric that leads to preferred crack propagation in one direction<br />

(thermal anisotropy cracking). Bar Harbor Formation rocks can exhibit all three <strong>of</strong><br />

these fracture types due to their compositional layering, and they may be more<br />

susceptible to thermal fracture than suggested by this model. The thermal<br />

gradient cracking model therefore provides a low end-member possibility for the<br />

proliferation <strong>of</strong> thermal cracks in Bar Harbor clasts.<br />

If thermal fracture was prevalent, each clast would fracture according to a<br />

new size distribution: for thermal fracture, D s = 2.156 (Glazner and Bartley,<br />

2006). The new value <strong>of</strong> D s is the combination <strong>of</strong> the explosive fracture event and<br />

the secondary thermal fracture event, and repeated fracture events always<br />

increase D s by a fractional amount (Jebrak, 1997). Also, field evidence suggests<br />

that not all diorite clasts experienced thermal fracture, therefore late-stage<br />

thermal fracture did not have a significant effect on diorite dike CSD results.<br />

114

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