A neat way to see why the ratio is exactly \(0.5\) regardless of the resistor's value is to note that the resistor's job during charging is entirely to dissipate the difference between what the source supplies and what ends up stored, and this split does not depend on how large \(R\) is, only on the fact that the capacitor's voltage rises exponentially toward \(V\).
Since \(E_{source}=CV^2\) and \(E_C=\tfrac12CV^2\) regardless of \(R\) (a larger \(R\) only slows down the charging, it does not change the final energies), the energy dissipated in the resistor is \[ E_R = E_{source}-E_C = CV^2 - \tfrac12CV^2 = \tfrac12CV^2 \] which is exactly equal to \(E_C\) itself. In other words, charging a capacitor through any resistor always splits the source's energy exactly in half between the capacitor and the resistor.
Therefore, the correct answer is 0.500.
A $\Delta$-network connected with its Y-equivalent is shown. Find the resistances $R_1, R_2, R_3$.