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Question: In an isothermal irreversible expansion of an ideal gas : A. \(\Delta U = 0\) B. \( - {w_q} = n...

In an isothermal irreversible expansion of an ideal gas :
A. ΔU=0\Delta U = 0
B. wq=nRT[1P2P1] - {w_q} = nRT[1 - \frac{{{P_2}}}{{{P_1}}}]
C. ΔH0\Delta H \ne 0
D. All of these

Explanation

Solution

An isothermal process is one in which the pressure and volume of the system change but temperature remains constant . In case of isothermal irreversible expansion , the gas is allowed to expand slowly , its temperature tends to fall but some of the heat from the surrounding is conducted to the gas , keeping the temperature constant .

Complete step by step answer:
When a gas expands isothermally irreversibly , ΔV\Delta V and hence PΔVP\Delta V is positive and so Δq\Delta q will also be positive . Therefore , when a gas expands isothermally , an amount of heat equivalent to the work done by the gas has to be supplied from an external source .
Here , ΔV\Delta V = change in volume
PΔVP\Delta V = the work done
Δq\Delta q =heat
Now we know that in the isothermal process temperature remains constant . Therefore , since internal energy (U) is a function of temperature its value is also equal to zero .
ΔU=0\Rightarrow \Delta U = 0
In isothermal irreversible expansion , internal pressure is much different from external pressure . For example if internal pressure is much greater than the external pressure , then as the expansion takes place against the external pressure irreversibly , the work done is given by
w=Pext×ΔVw = - {P_{ext}} \times \Delta V

Hence option A is correct , that is ΔU=0\Delta U = 0 .

Note:
The work done in isothermal irreversible expansion is lesser than the work done in isothermal reversible expansion .
Also in the irreversible expansion , external pressure remains constant but in reversible expansion , external pressure has to be decreased continuously so as to remain infinitesimally smaller than the internal pressure .