Step 1: Write the overall equilibrium equations for the full structure.
Taking $A$ as the origin, with $B$ at 1.2 m, the 25 kN load at 1.4 m, and $C$ at 2.0 m, vertical balance of the whole structure gives $R_A + R_B + R_C = 10 + 25 = 35$ kN.
Taking moments of the whole structure about $A$: $R_B(1.2) + R_C(2.0) - 10(0.5) - 25(1.4) = 0$, which simplifies to $1.2R_B + 2.0R_C = 40$.
Step 2: Bring in the hinge condition as a third equation.
Since the hinge at 1.0 m from $A$ transmits no moment, the moment of everything to its left about the hinge must be zero on its own: $R_A(1.0) - 10(0.5) = 0$, giving $R_A = 5$ kN.
This extra condition is what makes an otherwise indeterminate three reaction beam solvable.
Step 3: Substitute $R_A$ into the vertical balance.
$R_B + R_C = 35 - 5 = 30$, so $R_B = 30 - R_C$.
Step 4: Substitute into the moment equation and solve for $R_C$.
$1.2(30 - R_C) + 2.0R_C = 40$
$36 - 1.2R_C + 2.0R_C = 40$
$0.8R_C = 4$, so $R_C = 5$ kN.
Final Answer:
Solving the whole structure together with the hinge condition gives the same reaction as splitting it into two pieces.
\[ \boxed{R_C = 5 \text{ kN}} \]