(a) = Lyman series,
(b) = Balmer series,
(c) = Paschen series,
(d) = Brackett series,
(e) = Pfund series
(b) Lyman series – UV region
Balmer series – Visible region
Paschen series – Infrared region
Brackett series – Infrared region
Pfund series – Infrared region
(c) In hydrogen atom there is one electron which is present in first orbit in ground state. When energy is supplied this electron may be excited to some higher energy level. Since in a sample of hydrogen there are large number of atoms, the electrons in different atoms absorb different amounts of energies and are excited to different higher energy levels. Now, from excited states, the electron may return to ground state in one or more jumps. These different downward jumps are associated with different amounts of energies and hence result in the emission of radiations of different wavelengths which appear as different lines in the hydrogen spectrum. Series – Obtained when electron jumps from any of the higher energy levels to
Lyman series – 1st energy level
Balmer series – 2nd energy level
Paschen series – 3rd energy level
Brackett series – 4th energy level
Pfund series – 5th energy level
(d) n1 = 2, n2 = 3, RH = 109677 cm-1
