In an isothermal process, the temperature remains constant, so the internal energy of an ideal gas does not change:
ΞU = 0
The work done in an isothermal expansion is given by:
W = nRT ln(Vf / Vi)
where Vf = 2.5V0 and Vi = V0. Substituting:
W = RT0 ln(2.5)
The expression RT0 ln(2) is incorrect; hence, statement (A) is not valid.
Since ΞU = 0, statement (B) is correct.
In an isobaric process, the pressure remains constant. The work done is:
W = PΞV
Using the ideal gas law (PV = nRT), the work done can be expressed as:
W = nRΞT
For a monoatomic ideal gas, ΞT = Tf β T0, but the given expression (3/2)RT0 is incorrect.
Thus, statement (C) is invalid.
The change in internal energy is:
ΞU = (3/2) nRΞT
The expression (9/2)RT0 does not align with this derivation.
Thus, statement (D) is incorrect.
The correct statements are (B) and (C).
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 ____