




\( H_{max} = \frac{u^2 \cos^2 \phi}{2g} \)
To solve this problem, we need to determine the relationship between the maximum height \(h_m\) reached by a projectile and its angle of projection \(\phi\) with the vertical axis. Let's break down the problem:
The maximum height \(h_m\) of a projectile is given by the formula:
\(h_m = \frac{(v_0 \sin \theta)^2}{2g}\)
Here, \(v_0\) is the initial velocity, \(\theta\) is the angle of projection with the horizontal, and \(g\) is the acceleration due to gravity.
Since the angle of projection \(\phi\) is with the vertical, we relate it to the angle \(\theta\) by:
\(\theta = 90^\circ - \phi\)
Substituting \(\theta = 90^\circ - \phi\) into the maximum height formula, we get:
\(h_m = \frac{(v_0 \sin(90^\circ - \phi))^2}{2g}\)
We know that \(\sin(90^\circ - \phi) = \cos \phi\). Thus, the expression becomes:
\(h_m = \frac{(v_0 \cos \phi)^2}{2g}\)
Simplifying this, we have:
\(h_m = \frac{v_0^2 \cos^2 \phi}{2g}\)
This matches the given correct answer. Therefore, the relationship between the maximum height \(h_m\) and the angle \(\phi\) is:
Thus, the correct answer is that \(h_m\) can be expressed as:
\(h_m = \frac{v_0^2 \cos^2 \phi}{2g}\)
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 : \(A_2 \rightleftharpoons 2A\)