BHU PMT BHU PMT Solved Paper-2003

  • question_answer
    Equations of motion in the same direction are given by:                 \[\begin{align}   & {{y}_{1}}=2a\,\,\sin \left( \omega t-kx \right) \\  & {{y}_{2}}=2a\,\,\sin \left( \omega t-kx-\theta  \right) \\ \end{align}\] The amplitude of the medium particle will be:                                                                    [BHU M-2003]

    A)  \[2a\,\,\cos \,\theta \]                

    B)  \[\sqrt{2}a\,\,\cos \,\theta \]

    C)   \[4a\,\,\cos \,\frac{\theta }{2}\]                             

    D)  \[\sqrt{2}a\,\,\cos \,\frac{\theta }{2}\]

    Correct Answer: C

    Solution :

                     Key Idea: Resultant displacement is sum of individual displacements. Given \[{{y}_{1}}\] and \[{{y}_{2}}\] the displacement at a point x at any instant\[t\] Then by principle of superposition, the resultant displacement at that point is \[y={{y}_{1}}+{{y}_{2}}\] Given, \[{{y}_{1}}=2a\,\sin \left( \omega t-kx \right),\]                                 \[{{y}_{2}}=2a\,\sin \left( \omega t-k\,x-\theta  \right)\]                 \[\therefore \]\[y=2a\left[ \sin \left( \omega t-kx \right)+\sin \left( \omega t-kx-\theta  \right) \right]\] Using the formula                 \[\sin A+\sin \,B=2\sin \,\frac{A+B}{2}\cos \frac{A-B}{2}\] \[y=2a\left[ 2\,\sin \frac{\left( \omega t-kx+\omega t-kx-\theta  \right)}{2}\times \cos \frac{\omega t-kx-\left( \omega t-kx-\theta  \right)}{2} \right]\] \[\therefore \]  \[y=4a\,\,\cos \frac{\theta }{2}\sin \left( \omega t-kx-\frac{\theta }{2} \right)\]  ?(1) Also, standard equation of wave is                                 \[y=A\,\sin \left( \omega t-kx \right)\]                    ...(2) Comparing Eqs. (1) and  (2), we get                                 \[A=4\,a\,\,\cos \frac{\theta }{2}\]


You need to login to perform this action.
You will be redirected in 3 sec spinner