Given: \[ \Delta T_f = 0.558°C \quad \text{and} \quad k_f = 1.86 \, \text{K} \, \text{kg/mol} \] We know that: \[ \Delta T_f = i \times k_f \times m \] where \(i\) is the van't Hoff factor (number of ions produced per formula unit), \(m\) is the molality, and \(k_f\) is the cryoscopic constant.
Given that the molality of the solution is 0.1 m, we have: \[ \Delta T_f = i \times 1.86 \times 0.1 \] Substituting the given value of \(\Delta T_f\): \[ 0.558 = i \times 1.86 \times 0.1 \] \[ i = \frac{0.558}{1.86 \times 0.1} = 3 \] This implies that the complex ion must dissociate into 3 ions in solution. The complex that corresponds to \(i = 3\) is [Cr(NH\(_3\))\(_5\)]Cl\(_2\), as it would dissociate into 1 Cr\(^3+\) ion and 2 Cl\(^-\) ions.
Thus, the correct complex is [Cr(NH\(_3\))\(_5\)]Cl\(_2\).
The cause for deviation from Raoult’s law in the colligative properties of non-ideal solutions lies in the nature of interactions at the molecular level. These properties show deviations from Raoult’s law due to difference in interactions between solute–solvent, solute–solute and solvent–solvent. Some liquids on mixing form azeotropes which are binary mixtures having the same composition in liquid and vapour phase and boil at a constant temperature. In such cases, it is not possible to separate the components by fractional distillation. There are two types of azeotropes called minimum boiling azeotrope and maximum boiling azeotrope. (a) Pure ethanol cannot be prepared by fractional distillation of ethanol–water mixture. Comment.
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).