Step 1: Split the structure at the hinge.
The hinge cannot carry a moment, so treat the beam as two separate pieces: a left piece from \( A \) to the hinge, and a right piece from the hinge to \( C \), joined only by a shared vertical force at the hinge.
The left piece carries the \( 10 \) kN load at \( 0.5 \) m from \( A \), with the hinge sitting \( 1.0 \) m from \( A \), so the load is \( 0.5 \) m from the hinge.
Step 2: Solve the left piece for the reaction at A.
Taking moments about the hinge for the left piece alone (the hinge carries no moment, so this check is valid): \( R_A \times 1.0 - 10 \times 0.5 = 0 \).
This gives \( R_A = 5 \) kN.
Step 3: Find the force transferred through the hinge.
Vertical balance of the left piece: \( R_A + F_{hinge} - 10 = 0 \), so \( F_{hinge} = 10 - 5 = 5 \) kN acting upward on the left piece from the right piece.
By Newton's third law, the left piece pushes down on the right piece at the hinge with the same \( 5 \) kN.
Step 4: Solve the right piece by taking moments about B.
The right piece carries the \( 5 \) kN hinge force (\( 0.2 \) m to the left of \( B \)), the \( 25 \) kN load (\( 0.2 \) m to the right of \( B \)), and reactions \( R_B \) and \( R_C \), with \( C \) sitting \( 0.8 \) m to the right of \( B \).
Taking moments about \( B \): \( 5 \times 0.2 - 25 \times 0.2 + R_C \times 0.8 = 0 \).
Step 5: Solve for \( R_C \).
\( 1 - 5 + 0.8 R_C = 0 \), so \( 0.8 R_C = 4 \) and \( R_C = 5 \) kN.
Final Answer:
The vertical reaction at the pin support C balances the loads carried through the hinge and across the right span.
\[ \boxed{R_C = 5 \text{ kN}} \]