Concept:
This system behaves like an Atwood machine. When two masses are connected by a light string over a frictionless pulley, the acceleration of the system is
\[
a = \frac{(m_1 - m_2)g}{m_1 + m_2}
\]
Once acceleration is known, the velocity can be obtained using the kinematic relation
\[
v^2 = u^2 + 2as
\]
where
\begin{itemize}
\item \(u\) = initial velocity
\item \(a\) = acceleration
\item \(s\) = displacement
\end{itemize}
Step 1: {\color{red}Calculate acceleration of the system.}
Given masses:
\[
m_1 = 6\,\text{kg}, \qquad m_2 = 2\,\text{kg}
\]
\[
a = \frac{(6-2)10}{6+2}
\]
\[
a = \frac{40}{8} = 5\,\text{m/s}^2
\]
Step 2: {\color{red}Use the kinematic equation to find final speed.}
Initial velocity:
\[
u = 0
\]
Distance moved by the \(6\,\text{kg}\) block:
\[
s = 6\,\text{m}
\]
Using
\[
v^2 = u^2 + 2as
\]
\[
v^2 = 0 + 2(5)(6)
\]
\[
v^2 = 60
\]
\[
v = \sqrt{60}
\]
\[
v \approx 7.74\,\text{m/s}
\]
Thus, the speed of the \(6\,\text{kg}\) block just before hitting the ground is
\[
\boxed{7.74\,\text{m/s}}
\]