Step 1: Given data and conversion.
Maximum speed of the boat in still water = 27 km/h
Speed of river = 9 km/h
Speed of ball thrown vertically = 10 m/s
Acceleration due to gravity, \( g = 10 \, \text{m/s}^2 \)
First, convert the boat’s speed (downstream) into m/s:
\[
\text{Boat speed downstream} = 27 + 9 = 36 \, \text{km/h}
\]
\[
36 \, \text{km/h} = 36 \times \frac{1000}{3600} = 10 \, \text{m/s}
\]
Hence, the boat moves with a horizontal velocity of \( 10 \, \text{m/s} \) relative to the ground.
Step 2: Motion analysis (in observer’s frame).
The man in the boat throws the ball vertically upward with a speed of \( 10 \, \text{m/s} \) relative to the boat. Since the boat is moving horizontally with \( 10 \, \text{m/s} \), the horizontal component of the velocity of the ball (as seen by an observer on the river bank) is also \( 10 \, \text{m/s} \).
The vertical motion is independent of the horizontal motion. The time of flight for vertical motion is:
\[
T = \frac{2u}{g} = \frac{2 \times 10}{10} = 2 \, \text{s}
\]
Step 3: Horizontal range as seen from the river bank.
During this time, the ball continues moving horizontally with velocity \( 10 \, \text{m/s} \). Thus, horizontal range:
\[
R = u_x \times T = 10 \times 2 = 20 \, \text{m}
\]
Convert to centimeters:
\[
R = 20 \times 100 = 2000 \, \text{cm}
\]
Final Answer:
\[
\boxed{2000 \, \text{cm}}
\]