Step 1: Geometry of a disk under parallel-beam projection.
In parallel-beam CT, the Radon projection at view angle \(\theta\) of a circular inclusion (disk) is a \emph{rectangular} profile of constant height whose center lies at the signed distance
\[
s = x_0 \cos\theta + y_0 \sin\theta
\]
from the rotation origin, where \((x_0,y_0)\) is the center of the inclusion. The width of this rectangle equals the disk diameter (here \(5\ \mathrm{mm}\)) and is independent of \(\theta\).
Step 2: Number of views needed to solve for the center.
Each single view gives one linear equation in the unknowns \((x_0,y_0)\) via \(s\). Two distinct view angles \(\theta_1\) and \(\theta_2\) yield
\[
\begin{cases}
s_1 = x_0 \cos\theta_1 + y_0 \sin\theta_1,
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s_2 = x_0 \cos\theta_2 + y_0 \sin\theta_2,
\end{cases}
\]
which can be solved uniquely for \((x_0,y_0)\) so long as \(\theta_2 \not\equiv \theta_1 \ (\mathrm{mod}\ \pi)\).
Thus, the minimum number of distinct projection views needed to locate the inclusion is \(\boxed{2}\) (e.g., orthogonal views at \(0^\circ\) and \(90^\circ\)). The given beam width (30 mm) exceeds the object size (20 mm), ensuring full coverage but not affecting this minimum.