AFMC AFMC Solved Paper-2010

  • question_answer
    If the electric flux entering and leaving an enclosed surface respectively is \[{{\theta }_{1}}\] and \[{{\theta }_{2}}\], the electric charge inside the surface will be

    A) \[\frac{{{\theta }_{2}}-{{\theta }_{1}}}{{{\varepsilon }_{0}}}\]                                     

    B) \[\frac{{{\theta }_{1}}+{{\theta }_{2}}}{{{\varepsilon }_{0}}}\]

    C) \[\frac{{{\theta }_{1}}-{{\theta }_{2}}}{{{\varepsilon }_{0}}}\]                                     

    D) \[{{\varepsilon }_{0}}\left( {{\theta }_{1}}+{{\theta }_{2}} \right)\]

    Correct Answer: D

    Solution :

    Let \[-{{q}_{1}}\] be the charge, due to which flux\[\text{o }\!\!|\!\!\text{ }\] is entering the surface. \[\text{o}{{\text{ }\!\!|\!\!\text{ }}_{1}}=\frac{-q}{{{\varepsilon }_{0}}}\]or  \[-{{q}_{1}}={{\varepsilon }_{0}}\text{o}{{|}_{1}}\] Let \[\text{+}{{\text{q}}_{\text{2}}}\]be the charge, due to which flux\[\text{o}{{\text{ }\!\!|\!\!\text{ }}_{2}},\] is entering the surface. \[\text{o}{{\text{ }\!\!|\!\!\text{ }}_{1}}=\frac{{{q}_{2}}}{{{\varepsilon }_{0}}}\]or      \[-{{q}_{2}}={{\varepsilon }_{0}}\text{o}{{\text{ }\!\!|\!\!\text{ }}_{2}}\]   Electric charge inside the surface \[={{q}_{2}}-{{q}_{1}}={{\varepsilon }_{0}}\text{o}{{\text{ }\!\!|\!\!\text{ }}_{2}}+{{\varepsilon }_{0}}\text{o}{{\text{ }\!\!|\!\!\text{ }}_{1}}\] \[={{\varepsilon }_{0}}(o{{|}_{2}}+o{{|}_{1}})\]


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