For 1 mol of gas, the plot of pV vs. p is shown below. p is the pressure and V is the volume of the gas. What is the value of compressibility factor at point A?
When solving compressibility factor problems:
Start by expressing \(Z = \frac{PV}{RT}\) and substitute the appropriate gas law (e.g., Van der Waals equation).
Expand and simplify using the given conditions to isolate terms involving \(V\), \(a\), and \(b\).
Pay attention to the behavior of \(Z\) in real gas scenarios.
\(1-\frac{a}{RTV}\)
\(1+\frac{b}{V}\)
\(1-\frac{b}{V}\)
\(1+\frac{a}{RTV}\)
For 1 mole of real gas, \[ PV = ZRT \] From the graph, \(PV\) for a real gas is less than \(PV\) for an ideal gas at point A. Thus, \(Z < 1\). The compressibility factor \(Z\) is given by: \[ Z = 1 - \frac{a}{V_m RT} \] Substituting into the definition of \(Z\) and simplifying: \[ Z = 1 - \frac{a}{RTV} \]
A substance 'X' (1.5 g) dissolved in 150 g of a solvent 'Y' (molar mass = 300 g mol$^{-1}$) led to an elevation of the boiling point by 0.5 K. The relative lowering in the vapour pressure of the solvent 'Y' is $____________ \(\times 10^{-2}\). (nearest integer)
[Given : $K_{b}$ of the solvent = 5.0 K kg mol$^{-1}$]
Assume the solution to be dilute and no association or dissociation of X takes place in solution.
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]