The displacement of a particle moving with constant acceleration from rest is given by:
\[
S = ut + \frac{1}{2}at^2
\]
Since initial velocity \(u = 0\), the distance covered in time \(t\) is:
\[
X = \frac{1}{2}at^2 \quad \text{(Equation 1)}
\]
Now, total distance covered in time \(2t\) is:
\[
S_{2t} = \frac{1}{2}a(2t)^2 = \frac{1}{2}a \cdot 4t^2 = 2at^2
\]
Distance covered in the next \(t\) seconds = \(S_{2t} - S_t\)
\[
= 2at^2 - \frac{1}{2}at^2 = \frac{3}{2}at^2 = 3X \quad \text{(from Equation 1)}
\]
Hence, the particle travels 3X distance in the next \(t\) seconds.