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Q.
The limiting line in Balmer series will have a frequency of (Rydberg constant, $R_{\infty}=3.29\times10^{15}$ cycles/s)
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Solution:
$\bar{v}=\frac{1}{\lambda}=R_{H}Z\left(\frac{1}{n^{2}_{1}}-\frac{1}{n^{2}_{2}}\right)$
In Balmer series $n_{1} = 2 \& n_{2}=3, 4, 5 .....$ Last line of the spectrum is called series limit
Limiting line is the line of shortest wavelength and high energy when $n_{2}=\infty$
$\therefore \bar{v}=\frac{1}{\lambda}=\frac{R_{H}}{n^{2}_{1}}=\frac{3.29\times10^{15}}{2^{2}}=\frac{3.29\times10^{15}}{4}$
$=8.22\times10^{14}s^{-1}$