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Chapter 7<br />
MECHANISMS FOR SECONDARY CLAST MODIFICATION: A DISCUSSION<br />
The thermal influence from the intruded granitic matrix <strong>of</strong> the Shatter Zone<br />
had a significant influence on clast size distribution (CSD) data trends,<br />
specifically for Bar Harbor Formation Type 3 clasts. The marked decrease in<br />
small clast populations and boundary shape values as well as the increase in<br />
clast circularity implies a non-fractal mechanism was active in the modification <strong>of</strong><br />
clast size, shape, and abundance. Potential mechanis<strong>ms</strong> are explored for post<br />
brecciation modification and I determine that disaggregation through partial melt<br />
<strong>of</strong> clasts is the dominant mechanism at play. Transient two-dimensional models<br />
are produced in order to quantitatively characterize the migration <strong>of</strong> solidus<br />
temperatures through a conductively heated clast, and to determine the evolution<br />
<strong>of</strong> CSD as clasts begin to partially melt. I show that disaggregation <strong>of</strong> clasts can<br />
lead to a bi-fractal and eventually non-fractal CSD. Magma flow, a constraint<br />
ignored in the thermal-mechanical model, is required to physically disaggregate<br />
the melted clasts. Thermal fracture is another possible secondary mechanism<br />
and is treated in a transient two-dimensional thermal stress model. Results show<br />
that late-stage thermal fracture occurred in diorite clasts, but less is known about<br />
the thermal stress characteristics <strong>of</strong> the structurally anisotropic Bar Harbor<br />
Formation.<br />
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