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emplacement <strong>of</strong> mafic magma, resulting in elastic failure <strong>of</strong> the metasedimentary<br />
and diorite wall rock and virtually instantaneous fragmentation and entrainment <strong>of</strong><br />
the clasts in hot granitic magma. The degree <strong>of</strong> brecciation is gradational, with<br />
clast supported breccias at the outer margin <strong>of</strong> the zone grading inward to<br />
granitic-matrix supported breccia, and finally into clast-free Cadillac Mountain<br />
Granite. Field observations point to an explosive breccia mechanism, and clast<br />
size distribution analysis yields fractal dimensions (D s > 3) that agree with those<br />
known to result from explosion (D s > 2.5). Field and microstructural data and<br />
observations suggest that the clast sizes and shapes <strong>of</strong> the metasedimentary<br />
host rocks reflect post-brecciation modification by partial melting and thermal<br />
fracture, while diorite dike fragments experienced little modification after the<br />
original brecciation event. Clast circularity increases with proximity to the magma<br />
reservoir, whereas clast boundary shape decreases; this implies thermal wear on<br />
clast surfaces. Numerical modeling is employed to explore the possible thermalmechanical<br />
effects on the size distribution <strong>of</strong> clasts. Instantaneous immersion is<br />
assumed for metasedimentary clasts (650°C) in a hot granitic matrix (800°C -<br />
900°C), and our thermal analysis is restricted to conductive heat transfer<br />
corrected for latent heat. The amount <strong>of</strong> clast melt is primarily dependent on the<br />
melt temperature <strong>of</strong> the clast, the matrix to clast volume ratio, and the initial<br />
magma intrusion and clast temperatures. Results show that thermal fracture and<br />
clast melt were viable secondary modification processes, and magma flow was<br />
necessary for disaggregation <strong>of</strong> melted clasts to occur. Angular clasts are highly<br />
susceptible to corner break-<strong>of</strong>f owing to large tensile stresses associated with