We can calculate the final concentration of the NaOH solution using the dilution formula: \[ C_1 V_1 + C_2 V_2 = C_f V_f \]
Where: - \( C_1 = 2 \, \text{M} \) (concentration of first solution), - \( V_1 = 20 \, \text{mL} \) (volume of first solution), - \( C_2 = 0.5 \, \text{M} \) (concentration of second solution), - \( V_2 = 400 \, \text{mL} \) (volume of second solution), - \( C_f \) is the final concentration, and - \( V_f = V_1 + V_2 = 20 + 400 = 420 \, \text{mL} \).
Now, substitute the values: \[ (2 \times 20) + (0.5 \times 400) = C_f \times 420 \] \[ 40 + 200 = C_f \times 420 \] \[ C_f = \frac{240}{420} = 0.571 \, \text{M} \]
Thus, the final concentration is approximately \( 0.57 \, \text{M} \), or \( 5.7 \times 10^{-2} \, \text{M} \).
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 _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]
A small block of mass \(m\) slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration \(a_0\). The angle between the inclined plane and ground is \(\theta\) and its base length is \(L\). Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is _______. 