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:
To solve this problem, we need to understand the motion of a body under constant acceleration. The given information tells us that the body starts from rest and covers displacements \( S_1 \) in \((p - 1)\) seconds and \( S_2 \) in \( p \) seconds. We want to find the time in which the displacement \( S_1 + S_2 \) is covered.
Let's break down the solution with step-by-step reasoning:
Thus, the time in which the displacement \( S_1 + S_2 \) is covered is the option: \(\sqrt{2p^2 - 2p + 1} \, s\).
Therefore, the correct option is:
\(\sqrt{2p^2 - 2p + 1} \, s\)
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: \(\sqrt{2p^2 - 2p + 1} \, s\)
In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

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