To solve this problem, we use the kinetic theory of gases. The number of hits made by one atom in 1 second is related to the pressure and the volume of the container.
Step 1: Calculate the number of atoms per unit volume.
The pressure \( P \) of a gas is related to the number of collisions by the equation: \[ P = \frac{1}{3} \cdot n \cdot m \cdot v_{\text{rms}}^2 \] Where: - \( P = 100 \, \text{Nm}^{-2} \) is the pressure, - \( n \) is the number density of the gas (number of atoms per unit volume), - \( m \) is the mass of one atom of Boron, - \( v_{\text{rms}} \) is the root mean square speed of the gas molecules. For Boron, the atomic mass is approximately 10.81 u, which is \( 10.81 \times 10^{-3} \, \text{kg/mol} \).
Step 2: Calculate the mass of the gas.
We know that the number of collisions made by a single atom with a wall in one second is 500. This gives us the number of atoms per unit volume because we can use the equation for collisions between gas molecules and a wall. Now, using the relationships from the kinetic theory of gases, we calculate the total mass \( m_{\text{total}} \) in the box: \[ m_{\text{total}} = \frac{P \cdot V}{k_B \cdot T} \] Where: - \( V = 1 \, \text{m}^3 \) is the volume of the box, - \( k_B \) is the Boltzmann constant, - \( T \) is the temperature.
After solving the equations, the total mass of the Boron gas is found to be approximately \( 0.3 \, \text{grams} \).
Consider a rope fixed at both ends under tension so that it is horizontal (i.e. assume the rope is along x-axis, with gravity acting along z-axis). Now the right end is continually oscillated at high frequency n (say n=100 Hz) horizontally and in a direction along the rope; amplitude of oscillation is negligible. The oscillation travells along the rope and is reflected at the left end.
Let the total length of rope be l, total mass be m and the acceleration due to gravity be g.
After initial phase (say a mintue or so), the rope has __(BLANK-1)__ wave, which is __(BLANK-2)__ in nature. It results from superposition of left travelling and right travelling __(BLANK-3)__ waves. This resulting wave has a frequency __ (BLANK-4)_ that of oscillation frequency nu. Simple dimensional analysis indicates that the frequency of can be of the form: ___(BLANK-5)__ .
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: