Related Formula
(1)/(λ) = RZ²((1)/(n₁²) - (1)/(n₂²))$$\frac{1}{\lambda} = RZ^2\left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right)$$
Core Logic
Statement I is a factual description of how the hydrogen emission spectrum is obtained. Dissociation yields excited atoms that emit light at discrete frequencies. So Statement I is true.
For Statement II:
First line of Lyman series for H atom (Z=1, n₁=1, n₂=2$Z=1, n_1=1, n_2=2$):
(1)/(λ₁) = R(1)²((1)/(1²) - (1)/(2²)) = R(1 - (1)/(4)) = (3R)/(4)$$\frac{1}{\lambda_1} = R(1)^2\left(\frac{1}{1^2} - \frac{1}{2^2}\right) = R\left(1 - \frac{1}{4}\right) = \frac{3R}{4}$$
Second line of Balmer series for He^+$He^+$ (Z=2, n₁=2, n₂=4$Z=2, n_1=2, n_2=4$):
(1)/(λ₂) = R(2)²((1)/(2²) - (1)/(4²)) = 4R((1)/(4) - (1)/(16)) = 4R((3)/(16)) = (3R)/(4)$$\frac{1}{\lambda_2} = R(2)^2\left(\frac{1}{2^2} - \frac{1}{4^2}\right) = 4R\left(\frac{1}{4} - \frac{1}{16}\right) = 4R\left(\frac{3}{16}\right) = \frac{3R}{4}$$
Since (1)/(λ₁) = (1)/(λ₂)$\frac{1}{\lambda_1} = \frac{1}{\lambda_2}$, their wavelengths (and therefore frequencies) are exactly the same. Statement II is true.
Step 1: Final Conclusion
Both statements are correct.
Chapter Mix
Class 11 Chemistry: Structure of Atom