Balmer found that the wavelength of all lines in hydrogen spectrum can be represented by λ1=R(n121−n221)
where R is Rydbergs constant.
Given, n2=3,n1=2 ∴λ11=R(221−321)=365R ⇒λ21=R(221−421)=163R ⇒λ1λ2=3R16×365R ⇒λ2=10880λ1
Given, λ1=6563A˚ ∴λ2=18080×6563=4861A˚