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An electron from various excited states of hydrogen atom emit radiation to come to the ground state. Let λₙ, λ_b be the de Broglie wavelength of the electron in the n^th state and the ground state respectively. Let Λₙ be the wavelength of the emitted photon in the transition from the n^th state to the ground state. For large n, (A, B are constants)
(1) Λₙ ≈ A + B/λₙ²
(2) Λₙ ≈ A + B λₙ
(3) Λₙ² ≈ A + B λₙ²
(4) Λₙ² ≈ λₙ
- Λₙ ≈ A + B/λₙ²
- Λₙ ≈ A + B λₙ
- Λₙ² ≈ A + B λₙ²
- Λₙ² ≈ λₙ
Correct answer: Λₙ ≈ A + B/λₙ²
Solution
The correct option indicates that the wavelength of the emitted photon, Λₙ, is inversely related to the square of the de Broglie wavelength of the electron in the n^th state, which aligns with the principles of quantum mechanics where higher energy transitions result in shorter wavelengths of emitted radiation.
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