1. Lyman series, Balmer series, Paschen series, Bracket series, P fund series
3. \(\bar v=\frac{1}{λ}=R_H\Big[\frac{1}{n^2_1}-\frac{1}{n^2_2}\Big]\) = \(R_H\Big[\frac{1}{2^2}-\frac{1}{3^2}\Big]\)
4.
\(\bar v=\frac{1}{λ}=R_H\Big[\frac{1}{n^2_1}-\frac{1}{n^2_2}\Big]\)
Longest wavelength n1 = 2 and n2 = 3
\(\bar v=\frac{1}{λ}=R_H\Big[\frac{1}{n^2_1}-\frac{1}{n^2_2}\Big]\)= \(R_H\Big[\frac{1}{2^2}-\frac{1}{3^2}\Big]\)
= 1.097 x 107x \(\frac{5}{36}\)
λ = \(\frac{1}{R_H\Big[\frac{1}{2^2}-\frac{1}{3^2}\Big]}\) = 6563 x 10-10
= 6563A0
Shortest Wavelength n1 = 2 and n2 = α
\(\bar v=\frac{1}{λ}=R_H\Big[\frac{1}{n^2_1}\frac{1}{n^2_2}\Big]\) = \(R_H\Big[\frac{1}{2^2}-\frac{1}{\alpha^2}\Big]\)
\(\frac{1}{R_H\Big[\frac{1}{2^2}-\frac{1}{\alpha^2}\Big]}\)= \(\frac{1}{1.097\times10^7\Big(\frac{1}{4}\Big)}\)
= 3646 x 10-10m = 3646 A0