2 mol of a monoatomic ideal gas with initial volume of 5 L and pressure 10 bar undergoes an irreversible adiabatic expansion against a constant final pressure of 1 bar. The final volume (in L) is ________.
(Given: R = $8.314 \times 10^{-2}$ L bar $mol^{-1}$ $K^{-1}$)
(rounded off to one decimal place)
For an adiabatic process, the First Law ($\Delta U = q + w$) becomes $\Delta U = w$ since $q = 0$.
Work done ($w$) against a constant external pressure is given by $w = -P_{ext} \Delta V$. Substituting the values:
$w = -(1 \text{ bar}) (V_2 - 5 \text{ L})$For a monoatomic ideal gas, the change in internal energy ($\Delta U$) is $n C_v \Delta T$. Using $C_v = \frac{3}{2}R$ for a monoatomic gas:
$\Delta U = n \frac{3}{2}R (T_2 - T_1)$Using the ideal gas law ($PV=nRT$, so $T = \frac{PV}{nR}$):
$T_1 = \frac{P_1 V_1}{nR}$ $T_2 = \frac{P_2 V_2}{nR}$(Note: The final pressure of the gas $P_2$ equals the external pressure $P_{ext}$ at equilibrium).
Equating $\Delta U = w$ and substituting the expressions for $\Delta U$ and $w$:
$n \frac{3}{2}R (T_2 - T_1) = -P_{ext} (V_2 - V_1)$Substitute $T_1$ and $T_2$:
$n \frac{3}{2}R \left(\frac{P_2 V_2}{nR} - \frac{P_1 V_1}{nR}\right) = -P_{ext} (V_2 - V_1)$Simplify the equation:
$\frac{3}{2} (P_2 V_2 - P_1 V_1) = -P_{ext} (V_2 - V_1)$Substitute the known values ($P_1=10$ bar, $V_1=5$ L, $P_{ext}=1$ bar, $P_2=1$ bar):
$\frac{3}{2} ((1 \text{ bar}) V_2 - (10 \text{ bar})(5 \text{ L})) = -(1 \text{ bar}) (V_2 - 5 \text{ L})$Simplify and solve for $V_2$:
$1.5 (V_2 - 50) = -(V_2 - 5)$ $1.5 V_2 - 75 = -V_2 + 5$ $1.5 V_2 + V_2 = 5 + 75$ $2.5 V_2 = 80$ $V_2 = \frac{80}{2.5}$ $V_2 = 32$ LThe calculated final volume is 32 L, which lies within the specified range of 31.8 to 32.2 L.
When a gas is compressed suddenly then its temperature
During throttling process:

From the above Carnot cycle undergone by an ideal gas, identify the processes in which the change in internal energy is NON-ZERO.