A particle is subject to a V (r) = /r2 potential. Following the general strategy in Section
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With V r 3r eq 616 becomes 2 dr G do Letting y 1r this becomes 2 dy do ay 2mE L 2mE L Veff r p2 2222 1 2m3 r1 where a 1 679 We must now consider vario...View the full answer
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