Given:
\[ |2a - 1| = 3[a] + 2\{a\} \]
Rewrite \(|2a - 1|\) in two forms depending on the value of \(a\):
In this case:
\[ 2a - 1 = [a] + 2a \]
Since \([a] = -1\), we find that \(a \in [-1, 0)\), which is a contradiction because \(a > \frac{1}{2}\). Therefore, this case is rejected.
Case 2: \(a < \frac{1}{2}\) In this case:
\[ -2a + 1 = [a] + 2a \]
Let \(a = I + f\) where \(I\) is the integer part and \(f\) is the fractional part, so \([a] = 0\) and \(\{a\} = f\).
Then we have:
\[ -2(I + f) + 1 = I + 2f \]
Substituting \(I = 0\), we get:
\[ 1 = 2f \implies f = \frac{1}{4} \]
Thus, \(a = \frac{1}{4}\).
Now, calculating \(72 \sum_{a \in S} a\): \[ 72 \times \frac{1}{4} = 18 \]
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 _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]