The wavelength of the radiation emitted, when in a hydrogen atom electron falls from infinity to stationary state 1, would be (Rydberg constant = 1.097×10⁷ m⁻¹)
(a) 406 nm
(b) 192 nm
(c) 91 nm
(d) 9.1×10⁻⁸ nm
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The wavelength of the radiation emitted, when in a hydrogen atom electron falls from infinity to stationary state 1, would be (Rydberg constant = 1.097×10⁷ m⁻¹)
(a) 406 nm
(b) 192 nm
(c) 91 nm
(d) 9.1×10⁻⁸ nm
→ [B]
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