A seconds pendulum has time period:
\[
T=2\text{ sec}.
\]
The time period of a simple pendulum is:
\[
T=2\pi\sqrt{\frac{l}{g}}.
\]
For the same pendulum, length \(l\) remains constant.
Therefore:
\[
T\propto \frac{1}{\sqrt{g}}.
\]
Let the gravity on earth be:
\[
g.
\]
On the new planet, gravity is half:
\[
g'=\frac{g}{2}.
\]
Now:
\[
\frac{T'}{T}=\sqrt{\frac{g}{g'}}.
\]
Substitute \(g'=\frac{g}{2}\):
\[
\frac{T'}{T}=\sqrt{\frac{g}{g/2}}.
\]
\[
\frac{T'}{T}=\sqrt{2}.
\]
So:
\[
T'=T\sqrt{2}.
\]
Since:
\[
T=2\text{ sec},
\]
we get:
\[
T'=2\sqrt{2}\text{ sec}.
\]
Hence, the time period on that planet is:
\[
2\sqrt{2}\text{ sec}.
\]