Step 1: Use the ideal gas law. Initially, let \( n_i \) be the number of moles of air, \( V \) the volume, and \( R \) the ideal gas constant: \[ PV = n_iRT_i \quad {and} \quad \frac{P}{2}V = n_fR(300 { K}), \] where \( n_i = \frac{8}{29} \) moles (assuming air is mostly nitrogen, \( M = 29 { g/mol} \)), and \( T_i = 400 { K} \).
Step 2: Calculate the final number of moles and the difference. From the equations, it follows that: \[ n_f = \frac{n_i T_i}{2 \times 300} = \frac{\frac{8}{29} \times 400}{600} = \frac{8}{43.5} { moles}. \] The moles of air escaped: \[ \Delta n = n_i - n_f = \frac{8}{29} - \frac{8}{43.5} \approx 0.092 { moles}. \] The mass of the air escaped: \[ \Delta m = \Delta n \times 29 \approx 2.67 { g}. \]
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____