A particle starts moving from rest under a constant acceleration, and covers a distance ‘X’ in ‘t’ seconds. The distance covered in next ‘t’ seconds is
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When motion starts from rest under constant acceleration:
Distance in first \(t\) seconds = \(X\),
Distance in next \(t\) seconds = \(3X\)
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.
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Approach Solution -2
Step 1: Understand the given information
- Initial velocity, \(u = 0\) (starts from rest)
- Constant acceleration, \(a\)
- Distance covered in first \(t\) seconds is \(X\)
Step 2: Use the equation of motion to find \(X\)
\[
X = ut + \frac{1}{2} a t^2 = 0 + \frac{1}{2} a t^2 = \frac{1}{2} a t^2
\]
Step 3: Find distance covered in next \(t\) seconds (from \(t\) to \(2t\))
Total distance covered in \(2t\) seconds:
\[
S_{2t} = ut' + \frac{1}{2} a (2t)^2 = 0 + \frac{1}{2} a (4 t^2) = 2 a t^2
\]
Distance covered in next \(t\) seconds = distance covered in \(2t\) seconds – distance covered in first \(t\) seconds:
\[
S = S_{2t} - X = 2 a t^2 - \frac{1}{2} a t^2 = \frac{3}{2} a t^2
\]
Step 4: Express the distance in terms of \(X\)
Recall \(X = \frac{1}{2} a t^2\), so:
\[
S = 3 \times \frac{1}{2} a t^2 = 3X
\]
Step 5: Final Conclusion
The distance covered in the next \(t\) seconds is \(3X\).