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:
Since the body starts from rest, using the formula \(S = \frac{1}{2}at^2\),
\[ S_1 = \frac{1}{2}a(p - 1)^2 \]
Using the same formula for \(S_2\),
\[ S_2 = \frac{1}{2}ap^2 \]
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 \(\frac{1}{2}a\):
\[ (p - 1)^2 + p^2 = t^2 \]
\[ t = \sqrt{2p^2 - 2p + 1} \]
So, the correct answer is: \(\sqrt{2p^2 - 2p + 1} \, s\)
The portion of the line \( 4x + 5y = 20 \) in the first quadrant is trisected by the lines \( L_1 \) and \( L_2 \) passing through the origin. The tangent of an angle between the lines \( L_1 \) and \( L_2 \) is:
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