According to Bohr's theory the wavelength of the radiations emitted from hydrogen atom is given by

1
\(\frac{1}{\lambda } = R\left[ {\frac{1}{{n_1^2}} - \frac{1}{{n_2^2}}} \right]\)
2
\(\frac{1}{\lambda } = {R^2}\left[ {\frac{1}{{n_1^2}} - \frac{1}{{n_2^2}}} \right]\)
3
\(\frac{1}{\lambda } = R\left[ {\frac{1}{{n_2^2}} - \frac{1}{{n_1^2}}} \right]\)
4
\(\frac{1}{\lambda } = \frac{1}{R}\left[ {\frac{1}{{n_1^2}} - \frac{1}{{n_2^2}}} \right]\)

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