The magnetic flux \( \Phi_B \) linked with the coil is given by:
\[
\Phi_B = B A \cos \theta.
\]
Where:
\( B \) is the magnetic field,
\( A \) is the area of the coil,
\( \theta \) is the angle between the normal to the surface of the coil and the magnetic field.
The area of the coil is:
\[
A = \pi r^2 = \pi (0.1)^2 = 0.0314 \, \text{m}^2.
\]
The magnetic field \( B \) is the dot product of the vector \( \vec{B} \) and the unit vector normal to the surface of the coil:
\[
\vec{B} \cdot \hat{n} = (1.0 \hat{i} + 0.5 \hat{j}) \cdot (0.6 \hat{i} + 0.8 \hat{j}) = 1.0 \times 0.6 + 0.5 \times 0.8 = 0.6 + 0.4 = 1.0 \, \text{mT}.
\]
Thus, the magnetic flux is:
\[
\Phi_B = 1.0 \times 0.0314 = 0.0314 \, \text{Wb} = 31.4 \, \mu \text{Wb}.
\]