Step 1: Calculate the total load on the beam.
Since the load is uniformly distributed with intensity \( q \) over a length of \( 2L \), the total load \( Q \) is:
\[
Q = q \times 2L = 2qL.
\]
Step 2: Analyze the support reactions.
The hinge at \( B \) splits the beam into two segments, but does not transfer bending moments, allowing us to consider each segment separately for the vertical reactions.
For segment \( AB \) (length \( L \)):
\[
\text{Total load on } AB = qL \quad \text{acting at the midpoint}.
\]
By symmetry and equilibrium, reaction at \( A \) (assuming \( B \) shares equally):
\[
R_A = \frac{qL}{2}.
\]
For segment \( BC \) (length \( L \)):
\[
\text{Total load on } BC = qL \quad \text{acting at the midpoint}.
\]
Assuming \( B \) takes all load from \( BC \) (as \( C \) is a roller and only resists vertical motion):
\[
R_B = \frac{qL}{2} + qL = \frac{3qL}{2}.
\]
Adding the contribution from \( AB \):
\[
R_B = \frac{qL}{2} + \frac{3qL}{2} = \frac{5qL}{2}.
\]
For support \( C \), considering overall equilibrium:
\[
R_C + R_A + R_B = 0 \quad \Rightarrow \quad R_C = - (R_A + R_B) = -\left(\frac{qL}{2} + \frac{5qL}{2}\right) = -3qL.
\]
After re-evaluating the total reactions considering the full beam, adjusting \( R_C \) to balance the moments and forces correctly:
\[
R_C = -qL.
\]