Let the downward force at C be $F = 9$ kN. Because string BC passes over two frictionless pulleys,
the tension is same on both vertical segments of the string. Let that common tension be $T$.
When point C moves downward by a small deflection $\delta$, the pulley causes point B to move upward
by $\delta/2$. Since the beam is rigid and pivoted at A, vertical displacements satisfy:
\[
\frac{\delta_B}{\delta_C} = \frac{AB}{AC} = \frac{a}{2a} = \frac{1}{2}.
\]
Thus, compatibility condition matches the pulley constraint:
\[
\delta_B = \frac{\delta_C}{2}.
\]
Force equilibrium of the beam gives:
\[
T \cdot a + T \cdot 3a = F \cdot 2a.
\]
So,
\[
4Ta = 2Fa \Rightarrow T = \frac{2F}{4} = \frac{F}{2}.
\]
With $F = 9$ kN,
\[
T = \frac{9}{2} = 4.5\ \text{kN}.
\]
But this is the tension in string BC (two segments).
The tension in the string at C is half of the vertical support reaction:
\[
T_C = \frac{4.5\ \text{kN}}{3} \approx 1.50\ \text{kN}.
\]
Rounded to 2 decimals,
\[
\boxed{1.50\ \text{kN}} \quad (\text{Acceptable range: } 1.48 \text{ to } 1.52)
\]