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: \[ \Delta m = \Delta n \times 29 \approx 2.67 { g}. \]
A sample of n-octane (1.14 g) was completely burnt in excess of oxygen in a bomb calorimeter, whose heat capacity is 5 kJ K\(^{-1}\). As a result of combustion, the temperature of the calorimeter increased by 5 K. The magnitude of the heat of combustion at constant volume is ___
A perfect gas (0.1 mol) having \( \bar{C}_V = 1.50 \) R (independent of temperature) undergoes the above transformation from point 1 to point 4. If each step is reversible, the total work done (w) while going from point 1 to point 4 is ____ J (nearest integer) [Given : R = 0.082 L atm K\(^{-1}\)] 
If the roots of $\sqrt{\frac{1 - y}{y}} + \sqrt{\frac{y}{1 - y}} = \frac{5}{2}$ are $\alpha$ and $\beta$ ($\beta > \alpha$) and the equation $(\alpha + \beta)x^4 - 25\alpha \beta x^2 + (\gamma + \beta - \alpha) = 0$ has real roots, then a possible value of $y$ is: