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Question

In Rutherford’s scattering experiment, what happens to an alpha-particle with a large impact parameter?

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Explanation

**Bohr's stationary orbits** defined by angular momentum quantization L = n ħ, ħ = h/2π, n=1 ground state, electron in these orbits does not radiate despite acceleration, contrary to classical EM theory which predicts atom collapse due to energy loss via radiation, Bohr postulates to explain observed stability and discrete spectra. For a large impact parameter, the alpha-particle experiences minimal deflection ( θ ≈ 0 ) and goes nearly undeviated. Using E_n = -13.6/n² eV, r_n = n² a₀, L = n h/2π, R = R₀ A^¹/³, BE = Δm c² and 1 u = 931.5 MeV, evaluation yields Goes nearly undeviated, consistent with Bohr

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