Step 1: Relation between time period and force constant.
For SHM,
\[
T = 2\pi \sqrt{\frac{m}{k}}
\Rightarrow k \propto \frac{1}{T^2}
\]
Step 2: Determine individual force constants.
\[
k_1 \propto \frac{1}{(0.8)^2}, \quad
k_2 \propto \frac{1}{(0.6)^2}
\]
Step 3: Resultant force constant.
When both forces act together in the same direction,
\[
k = k_1 + k_2
\]
Step 4: Express new time period.
\[
\frac{1}{T^2} = \frac{1}{(0.8)^2} + \frac{1}{(0.6)^2}
\]
\[
\frac{1}{T^2} = \frac{1}{0.64} + \frac{1}{0.36}
= 1.5625 + 2.7778 = 4.3403
\]
\[
T = \frac{1}{\sqrt{4.3403}} \approx 0.48\,\text{s}
\]
Step 5: Conclusion.
The new periodic time is \(0.48\,\text{s}\).