Step 1: Apply the assumption of no blade curvature.
When blade curvature is neglected, the pump behaves as if the water leaves the impeller tip carrying the full peripheral (tip) speed as its whirl velocity, so \( V_{w2} = u_2 \). Euler's pump equation for the ideal (theoretical) head then simplifies to \[ H_{th} = \dfrac{u_2 V_{w2}}{g} = \dfrac{u_2^2}{g} \]
Step 2: Bring in the manometric efficiency.
Manometric efficiency compares the actual delivered head to this ideal head: \( \eta_{man} = \dfrac{H_m}{H_{th}} \), so the ideal head is \[ H_{th} = \dfrac{H_m}{\eta_{man}} = \dfrac{60}{0.70} = 85.71\ \text{m} \]
Step 3: Solve for the impeller tip speed.
From Step 1, \( u_2 = \sqrt{g H_{th}} = \sqrt{9.81 \times 85.71} \approx \sqrt{840.86} \approx 29.00\ \text{m/s} \)
Step 4: Convert tip speed to impeller diameter.
The tip speed of a rotating impeller relates to its diameter and rotational speed by \( u_2 = \dfrac{\pi D N}{60} \), where \( N \) is in rpm. Rearranging, \[ D = \dfrac{60\,u_2}{\pi N} = \dfrac{60 \times 29.00}{\pi \times 2000} \approx 0.2769\ \text{m} = 27.69\ \text{cm} \]
Final Answer:
The impeller diameter of the pump is about 27.69 cm.
\[ \boxed{27.69\ \text{cm}} \]