To solve the problem, we must analyze the motion of the bodies using the principles of projectile motion. For the first case, a body of mass \( M \) is thrown horizontally from a height \( H \) with velocity \( v \) and lands 100 meters from the base of the tower.
Step 1: Determine Time of Flight for the First Case
The time of flight \( t \) for horizontal motion from height \( H \) is given by the equation: \( H = \frac{1}{2}gt^2 \). Solving for \( t \), we get \( t = \sqrt{\frac{2H}{g}} \).
Step 2: Horizontal Distance for the First Case
The horizontal distance covered is \( d = vt \). Given \( d = 100 \, \text{m} \), we have \( v\sqrt{\frac{2H}{g}} = 100 \).
Step 3: Solve for \( v \)
Rearrange to find \( v \): \( v = \frac{100}{\sqrt{\frac{2H}{g}}} \).
Step 4: Determine Flight Time for the Second Case
In the second scenario, a body of mass \( 2M \) is projected horizontally from height \( 4H \) with velocity \( \frac{v}{2} \). Using the formula \( 4H = \frac{1}{2}gt_2^2 \), solve for \( t_2 \): \( t_2 = \sqrt{\frac{8H}{g}} = 2\sqrt{\frac{2H}{g}} \).
Step 5: Calculate Horizontal Distance for the Second Case
Distance \( d_2 \) is given by \( d_2 = \left(\frac{v}{2}\right)t_2 = \left(\frac{100}{2\sqrt{\frac{2H}{g}}}\right)2\sqrt{\frac{2H}{g}} = 100 \, \text{m} \).
The solution is validated by checking the computed horizontal distance falls within the specified range, which is indeed 100 meters.
Result: The body of mass \( 2M \) touches the ground at a distance of 100 meters from the foot of the tower.
For the first body:
{Horizontal distance = horizontal velocity $\times$ time of flight.}
The time of flight for a height $H$ is:
\[t_1 = \sqrt{\frac{2H}{g}}.\]
The horizontal distance for the first body is:
\[x_1 = v \times t_1 = v \times \sqrt{\frac{2H}{g}}.\]
Given:
\[x_1 = 100 \, \text{m}.\]
For the second body:
The height is $4H$, so the time of flight is:
\[t_2 = \sqrt{\frac{2(4H)}{g}} = 2\sqrt{\frac{2H}{g}}.\]
The horizontal velocity is $\frac{v}{2}$. The horizontal distance for the second body is:
\[x_2 = \frac{v}{2} \times t_2.\]
Substitute $t_2 = 2\sqrt{\frac{2H}{g}}$:
\[x_2 = \frac{v}{2} \times 2 \sqrt{\frac{2H}{g}} = v \times \sqrt{\frac{2H}{g}}.\]
From the first case:
\[v \times \sqrt{\frac{2H}{g}} = 100 \, \text{m}.\]
Thus:
\[x_2 = 100 \, \text{m}.\]
{Final Result:}
\[x = 100 \, \text{m}.\]
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 : \(A_2 \rightleftharpoons 2A\)