The freezing point depression \( \Delta T_f \) is given by: \[ \Delta T_f = K_f \times m \] where \( K_f \) is the freezing point depression constant, and \( m \) is the molality.
Step 1: First, calculate the molality \( m \): \[ m = \frac{\text{mol of solute}}{\text{kg of solvent}} = \frac{\frac{1}{256}}{\frac{50}{1000}} = \frac{1}{256} \times \frac{1000}{50} = 0.078125 \, \text{mol/kg} \]
Step 2: Using the formula for freezing point depression: \[ \Delta T_f = K_f \times m \] Substitute \( \Delta T_f = 0.40 \, K \) and \( m = 0.078125 \, \text{mol/kg} \): \[ 0.40 = K_f \times 0.078125 \] \[ K_f = \frac{0.40}{0.078125} = 1.86 \, \text{K kg mol}^{-1} \]
Final Conclusion: The freezing point depression constant is 1.86 K kg mol\(^{-1}\), which corresponds to Option (3).
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 ____
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is: