Step 1: Find the blade tangential speed.
The runner turns at \(N = 600\) RPM with outer diameter \(D = 1\) m.
The tangential speed is \(u = \dfrac{\pi D N}{60} = \dfrac{\pi \times 1 \times 600}{60} = 31.42\) m/s.
Step 2: Find the whirl component of the inlet velocity.
The guide blade angle of \(15^{\circ}\) sets the direction of the absolute velocity \(V_1\).
The flow (normal) component is \(V_{f1} = 10\) m/s, so the whirl component is \(V_{w1} = \dfrac{V_{f1}}{\tan 15^{\circ}} = \dfrac{10}{0.2679} = 37.32\) m/s.
Step 3: Apply the inlet velocity triangle for the runner.
The runner vane angle \(\beta\) is measured from the relative velocity, so \(\tan \beta = \dfrac{V_{f1}}{V_{w1} - u}\).
Put in the numbers: \(\tan \beta = \dfrac{10}{37.32 - 31.42} = \dfrac{10}{5.90} = 1.693\).
Final Answer:
The inlet vane angle of the runner works out close to \(59.4^{\circ}\), inside the accepted key range.
\[ \boxed{\beta \approx 59.4^{\circ}} \]