Step 1: The force at \(A\) is vertical; hence the moment about \(C\) equals the force magnitude times the perpendicular (horizontal) distance from \(C\) to the line of action of the force through \(A\).
From the geometry, \(B\) is directly above \(C\) by \(L_2\) (\(\theta_2=90^\circ\)), and \(A\) is located from \(B\) by \(L_1\) at an angle \(\theta_1\) to the horizontal. Therefore the horizontal distance of \(A\) from \(C\) is
\[
x_A=L_1\cos\theta_1.
\]
Step 2: Compute the moment magnitude:
\[
M_C=F\,x_A
=400\;\text{N}\times (0.040\;\text{m})\cos45^\circ
=400\times 0.02828
\approx 11.3~\text{N}\cdot\text{m}.
\]