The maximum height of a projectile is given by:
\[ H_{\text{max}} = \frac{u^2 \sin^2 \theta}{2g}, \]
where:
- \( u \) is the initial velocity,
- \( \theta \) is the angle of projection,
- \( g \) is the acceleration due to gravity.
Step 1: Relationship between maximum heights
If the initial velocity is halved, i.e., \( u' = \frac{u}{2} \), the new maximum height \( H_{2\text{max}} \) can be expressed as:
\[ \frac{H_{1\text{max}}}{H_{2\text{max}}} = \frac{u^2}{u'^2}. \]
Substitute \( u' = \frac{u}{2} \):
\[ \frac{H_{1\text{max}}}{H_{2\text{max}}} = \frac{u^2}{\left( \frac{u}{2} \right)^2}. \]
Step 2: Simplify the expression
Simplify \( \left( \frac{u}{2} \right)^2 \):
\[ \frac{H_{1\text{max}}}{H_{2\text{max}}} = \frac{u^2}{\frac{u^2}{4}} = 4. \]
Thus:
\[ H_{2\text{max}} = \frac{H_{1\text{max}}}{4}. \]
Step 3: Calculate the new maximum height
Substitute \( H_{1\text{max}} = 64 \, \text{m} \):
\[ H_{2\text{max}} = \frac{64}{4} = 16 \, \text{m}. \]
Therefore, the new maximum height of the projectile is \( H_{2\text{max}} = 16 \, \text{m} \).
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 : \(A_2 \rightleftharpoons 2A\)