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: \(\sqrt{2p^2 - 2p + 1} \, s\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
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.
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