Ideal Gas Equation and Density Relationship:
For an ideal gas, the equation is given by:
\( PV = nRT \)
or,
\( P = \frac{nRT}{V} \)
where \( P \) is the pressure, \( T \) is the temperature, \( R \) is the gas constant, \( n \) is the number of moles, and \( V \) is the volume.
We can express \( P \) in terms of density \( \rho \) by substituting \( \rho = \frac{m}{V} \), where \( m \) is the mass of the gas:
\( P = \frac{\rho RT}{M} \)
where \( M \) is the molar mass of the gas. Rearranging, we get:
\( \rho = \frac{PM}{RT} \)
Analyze the PT Graph for Different Densities:
Since \( \rho = \frac{PM}{RT} \), for a given temperature \( T \), the density \( \rho \) of the gas is directly proportional to the pressure \( P \):
\( \rho \propto P \)
Therefore, at the same temperature, a higher pressure indicates a higher density.
Interpretation of the PT Diagram:
In the given PT diagram, we observe that:
\( P_1 > P_2 > P_3 \) for the same temperature \( T \)
Therefore, based on the proportional relationship \( \rho \propto P \) at constant temperature, we have:
\( \rho_1 > \rho_2 > \rho_3 \)
Conclusion:
The correct statement is: \( \rho_1 > \rho_2 \) which corresponds to Option (2).
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.
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: