JEE Main & Advanced AIEEE Solved Paper-2004

  • question_answer
    The wavelength of the radiation emitted, when in a hydrogen atom electron falls from infinity to stationary state 1, would be (Rydberg constant\[=1.097\times {{10}^{7}}\text{ }{{m}^{-1}})\]

    A) 91 nm   

    B)        192nm 

    C)        406 nm

    D)        \[9.1\times {{10}^{-8}}nm\]

    Correct Answer: A

    Solution :

    \[\frac{1}{\lambda }={{\overline{v}}_{H}}={{\overline{R}}_{H}}\left[ \frac{1}{n_{1}^{2}}-\frac{1}{n_{2}^{2}} \right]\] \[=1.097\times {{10}^{7}}\left[ \frac{1}{{{1}^{2}}}-\frac{1}{{{\infty }^{2}}} \right]\] \[\therefore \]\[\lambda =\frac{1}{1.097\times {{10}^{7}}}m=9.11\times {{10}^{-8}}m\] \[=91.1\times {{10}^{-9}}m=91.1nm\]        \[(1nm={{10}^{-9}}m)\]


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