For a strong electrolyte, the molar conductivity \(\Lambda_m\) can be expressed as:
\[\Lambda_m = \Lambda_m^0 - A\sqrt{C}\]
where \(\Lambda_m^0\) is the molar conductivity at infinite dilution, \(A\) is a constant, and \(C\) is the concentration.
The term \(A\sqrt{C}\) has units of \(\text{S cm}^2 \text{mol}^{-1}\), so the units of \(A\) must be \(\text{S cm}^2 \text{mol}^{-3/2} \text{L}^{1/2}\) to ensure dimensional consistency when multiplied with \(\sqrt{C}\) (units of \(\text{mol}^{1/2} \text{L}^{-1/2}\)).
Let $ f(x) = \begin{cases} (1+ax)^{1/x} & , x<0 \\1+b & , x = 0 \\\frac{(x+4)^{1/2} - 2}{(x+c)^{1/3} - 2} & , x>0 \end{cases} $ be continuous at x = 0. Then $ e^a bc $ is equal to
Total number of nucleophiles from the following is: \(\text{NH}_3, PhSH, (H_3C_2S)_2, H_2C = CH_2, OH−, H_3O+, (CH_3)_2CO, NCH_3\)