Step 1: Determine the length of the side of the equilateral triangle.
The total length of the wire is $L_{total} = 30\sqrt{3}$ cm.
The triangle has 3 equal sides, so the length of each side ($l$) is:
\[
l = \frac{L_{total}}{3} = \frac{30\sqrt{3}}{3} = 10\sqrt{3} \text{ cm}.
\]
Convert to SI units (meters): $l = 10\sqrt{3} \times 10^{-2} \text{ m} = 0.1\sqrt{3} \text{ m}$.
Step 2: State the formula for the magnetic force on a current-carrying wire.
The magnitude of the magnetic force $F$ on a segment of wire of length $l$ carrying a current $I$ in a uniform magnetic field $B$ is given by:
\[
F = I l B \sin\theta,
\]
where $\theta$ is the angle between the current direction (along the wire) and the magnetic field $\vec{B}$.
Step 3: Determine the angle $\theta$ for the side AC.
The magnetic field $\vec{B}$ is applied parallel to the side BC.
The angle between side AC and side BC in an equilateral triangle is $60^\circ$ (or $\pi/3$ rad).
The current flows along the sides, and the magnetic field is parallel to BC.
The angle $\theta$ between the current direction on side AC and the magnetic field (parallel to BC) is $60^\circ$.
Step 4: Substitute the given values and calculate the force.
Given values: $I=2$ A, $l=0.1\sqrt{3}$ m, $B=2$ T, and $\theta=60^\circ$.
\[
F_{AC} = I l B \sin(60^\circ).
\]
\[
F_{AC} = (2 \text{ A}) (0.1\sqrt{3} \text{ m}) (2 \text{ T}) \left(\frac{\sqrt{3}}{2}\right).
\]
\[
F_{AC} = 2 \times 0.1 \times 2 \times \frac{3}{2} = 0.2 \times 3 = 0.6 \text{ N}.
\]
\[
\boxed{F_{AC} = 0.6 \text{ N}}.
\]