Question:

A body starts moving from rest with constant acceleration and covers displacement \(S_1\) in the first \((p - 1)\) seconds and \(S_2\) in the first \(p\) seconds. The displacement \(S_1 + S_2\) will be made in time:

Updated On: Nov 12, 2024
  • \(\sqrt{2p^2 - 2p + 1} \, s\)
  • \((2p + 1) \, s\)
  • \((2p - 1) \, s\)
  • \((2p^2 - 2p + 1) \, s\)
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The Correct Option is A

Solution and Explanation

Step 1: Calculate \(S_1\) in the First \((p - 1)\) Seconds

Since the body starts from rest, using the formula \(S = \frac{1}{2}at^2\),

\[ S_1 = \frac{1}{2}a(p - 1)^2 \]

Step 2: Calculate \(S_2\) in the First \(p\) Seconds

Using the same formula for \(S_2\),

\[ S_2 = \frac{1}{2}ap^2 \]

Step 3: Total Displacement \(S_1 + S_2\)

If \(S_1 + S_2\) represents the displacement in time \(t\), then:

\[ S_1 + S_2 = \frac{1}{2}at^2 \]

Substitute \(S_1\) and \(S_2\) values:

\[ \frac{1}{2}a(p - 1)^2 + \frac{1}{2}ap^2 = \frac{1}{2}at^2 \]

Simplify by canceling \(\frac{1}{2}a\):

\[ (p - 1)^2 + p^2 = t^2 \]

Step 4: Solve for \(t\)

\[ t = \sqrt{2p^2 - 2p + 1} \]

So, the correct answer is: \(\sqrt{2p^2 - 2p + 1} \, s\)

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Concepts Used:

Centripetal Acceleration

A body that moves in a circular motion (with radius r) at a constant speed (v) is always being accelerated uninterruptedly. Thus, the acceleration is at the right angle to the direction of the motion. It is towards the center of the sphere and that of the magnitude  𝑣2/r. 

The direction of the acceleration is extrapolated through symmetry arguments. If it points the acceleration out of the plane of the sphere, then the body would pull out of the plane of the circle.

Read More: Centripetal Acceleration