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 \( 0.3 \, \text{grams} \).
The motion of a particle in the XY plane is given by \( x(t) = 25 + 6t^2 \, \text{m} \); \( y(t) = -50 - 20t + 8t^2 \, \text{m} \). The magnitude of the initial velocity of the particle, \( v_0 \), is given by:
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: