Concept:
When an object is dropped under the influence of uniform gravity from an initial height \(h_1\), its potential energy converts completely into kinetic energy just before impact. Upon bouncing, it leaves the ground with a reduced velocity, and its remaining kinetic energy converts back into potential energy as it rises to a new maximum height \(h_2\).
Step 1: Calculating the velocity of the ball just before hitting the ground.
Let \(h_1 = 1 \text{ m}\) be the initial drop height, and let \(g\) be the acceleration due to gravity. Using the third equation of motion (\(v^2 = u^2 + 2as\)) with an initial downward velocity \(u = 0\):
\[
v_1^2 = 0 + 2gh_1 \quad \Rightarrow \quad v_1 = \sqrt{2gh_1}
\]
Substituting \(h_1 = 1\):
\[
v_1 = \sqrt{2g(1)} = \sqrt{2g}
\]
Step 2: Calculating the rebound velocity after ground impact.
The problem states that upon hitting the ground, the ball's velocity is reduced by 20%. This means it retains 80% of its approach velocity.
Let \(v_2\) be the upward rebound velocity immediately after the bounce:
\[
v_2 = v_1 - (20% \text{ of } v_1) = 80% \text{ of } v_1
\]
\[
v_2 = 0.80 \times v_1
\]
Substituting our expression for \(v_1\) from
Step 1:
\[
v_2 = 0.8 \sqrt{2g}
\]
Step 3: Computing the subsequent rebound height \(h_2\).
Let \(h_2\) be the maximum height the ball reaches after bouncing. At this peak height, its upward velocity drops to zero. Applying the equation of motion for this upward phase:
\[
0 = v_2^2 - 2gh_2 \quad \Rightarrow \quad 2gh_2 = v_2^2
\]
Solving for \(h_2\):
\[
h_2 = \frac{v_2^2}{2g}
\]
Now substitute our expression for \(v_2 = 0.8\sqrt{2g}\) into this formula:
\[
h_2 = \frac{(0.8 \sqrt{2g})^2}{2g}
\]
Squaring the terms in the numerator:
\[
h_2 = \frac{(0.8)^2 \times (2g)}{2g}
\]
Canceling the common factor \(2g\) from both the numerator and denominator:
\[
h_2 = (0.8)^2 = 0.64 \text{ m}
\]
Thus, the ball will rise to a height of 0.64 meters, which corresponds to option (1).