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).
Match List - I with List - II.
Consider the following statements:
(A) Availability is generally conserved.
(B) Availability can neither be negative nor positive.
(C) Availability is the maximum theoretical work obtainable.
(D) Availability can be destroyed in irreversibility's.
At a particular temperature T, Planck's energy density of black body radiation in terms of frequency is \(\rho_T(\nu) = 8 \times 10^{-18} \text{ J/m}^3 \text{ Hz}^{-1}\) at \(\nu = 3 \times 10^{14}\) Hz. Then Planck's energy density \(\rho_T(\lambda)\) at the corresponding wavelength (\(\lambda\)) has the value \rule{1cm}{0.15mm} \(\times 10^2 \text{ J/m}^4\). (in integer)
[Speed of light \(c = 3 \times 10^8\) m/s]
(Note: The unit for \(\rho_T(\nu)\) in the original problem was given as J/mΒ³, which is dimensionally incorrect for a spectral density. The correct unit J/(mΒ³Β·Hz) or JΒ·s/mΒ³ is used here for the solution.)