The cylinder-piston system's walls and piston are made of rigid adiabatic material. Side A and Side B contain N2 and O2, respectively, which have the same temperature, pressure, and volume initially. Given that $T_{A1} = T_{B1} = 300\ \mathrm{K}$, $p_{A1} = p_{B1} = 0.1\ \mathrm{MPa}$, $V_{A1} = V_{B1} = 0.5\ \mathrm{m^3}$. The piston can move freely without friction within the cylinder. After the electric heater on side A is powered on, it slowly heats side A until $p_{A2} = 0.22\ \mathrm{MPa}$. Assume that both gases are ideal gases and calculate using constant specific heats: (see Figure Q1-1). ($M_{N_2} = 28.0 \times 10^{-3}\ \mathrm{kg/mol}$, $M_{O_2} = 32.0 \times 10^{-3}\ \mathrm{kg/mol}$, $R = 8.3145\ \mathrm{J/(mol\cdot K)}$, $c_{V,N_2} = 742.1\ \mathrm{J/(kg\cdot K)}$, $c_{V,O_2} = 649.6\ \mathrm{J/(kg\cdot K)}$, adiabatic index $\gamma = 1.4$)