A spectral line in the spectrum of H atom has a wavenumber of 15222.22 cm−1 . The transition responsible for this radiation is (Rydberg constant R = 109677 cm−1)
3→2
Here, let recall what is wave number
J=1λ⇒λ=1¯ν
And also,
¯ν=1λ=R×Z2[1n21−1n22]
Therefore,
λ=1¯ν=115222.22=6.569×10−5cm=6569˚A (visible light wavelength)
Clearly, it lies in the visible region i.e., in Balmer series. Hence, n1=2. Using the relation for wave number for H atom,
¯ν=1λ=RZ2(1n21−1n22)
15222.22=109677(122−1n22)
n2=3
The required transition is 3→2.
Hence, (c) is correct.
Note: (d) is wrong because 2→3 will absorb radiation