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Waves Test - 41

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Waves Test - 41
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  • Question 1
    1 / -0
    A particle performing S.H.M. starts from equilibrium position and its time period is $$16$$ second. After $$2$$ seconds its velocity is $$\pi \ m/s$$. Amplitude of oscillation is $$(\cos 45^{\circ} = \dfrac {1}{\sqrt {2}})$$
    Solution
    let $$x=asin\omega t$$
    on differentiating both side $$v=A\omega cos\omega t$$
    $$\pi=A\times\dfrac{2\pi}{T}cos\dfrac{2\pi}{T}t$$
    on putting T=16 sec and t=2 sec
    $$8=Acos45$$ 
    $$A=8\sqrt{2}$$
  • Question 2
    1 / -0
    Two sound waves having a phase difference of $$60^o$$, have a path difference of :
    Solution
    Path difference $$\Delta = \dfrac{\lambda}{2\pi}\times \Delta \phi$$
    $$=\dfrac{\lambda}{2\pi}\times \dfrac{\pi}{3} = \dfrac{\lambda}{6}$$
  • Question 3
    1 / -0
    A progressive wave is represented by y = 12 sin (5t - 4x) cm. On this wave, how far away are the two points having phase difference of 90$$^o$$?
    Solution
    Given equation for the wave is $$y = 12 \textrm{sin}(5t-4x)$$

    Phase is given by $$5t-4x$$. At a given instant, let two points $$x_1$$ and $$x_2$$ differ in phase by $$90^o = \pi/2$$.
    $$\Rightarrow (5t-4x_1)-(5t-4x_2) = \pi/2$$
    $$\Rightarrow 4|x_2-x_1| = \pi/2$$

    Thus, distance between the two points is $$\pi/8$$ $$\textrm{cm}$$
  • Question 4
    1 / -0
    A simple harmonic wave of amplitude $$8$$ unit travels along positive $$x$$-axis. At any given instant of time, for a particle at a distance of $$10 cm$$ from the origin, the displacement is $$+6$$ unit and for a particle at a distance of $$25 cm$$ from the origin, the displacement is $$+4$$ unit. Calculate the wavelength.
    Solution
    $$Y=A\sin { \dfrac { 2\pi  }{ \lambda  }  } \left( vt-x \right)$$
    $$ \dfrac { Y }{ A } =\sin { 2\pi  } \left( \dfrac { t }{ T } -\dfrac { x }{ \lambda  }  \right)$$
    In first case, $$ \dfrac { { Y }_{ 1 } }{ A } =\sin { 2\pi  } \left( \dfrac { t }{ T } -\dfrac { { x }_{ 1 } }{ \lambda  }  \right) $$
    Here, $${ Y }_{ 1 }=+6$$, $$A=8$$, $${ x }_{ 1 }=10 cm$$
    $$\dfrac { 6 }{ 8 } =\sin { 2\pi  } \left( \dfrac { t }{ T } -\dfrac { 10 }{ \lambda  }  \right) $$                .....(i)
    Similarly in the second case,
    $$\dfrac { 4 }{ 8 } =\sin { 2\pi  } \left( \dfrac { t }{ T } -\dfrac { 25 }{ \lambda  }  \right)$$                       .....(ii)
    From equation (i),
    $$ 2\lambda \left( \dfrac { t }{ T } -\dfrac { 10 }{ \lambda  }  \right) =\sin ^{ -1 }{ \left( \dfrac { 6 }{ 8 }  \right)  } =0.85 rad$$
    $$\Rightarrow \dfrac { t }{ T } -\dfrac { 10 }{ \lambda  } =0.14$$                     ....(iii)
    Similarly from equation (ii),
    $$2\pi \left( \dfrac { t }{ T } -\dfrac { 25 }{ \lambda  }  \right) =\sin ^{ -1 }{ \left( \dfrac { 4 }{ 8 }  \right)  } =\dfrac { \pi  }{ 6 } rad$$
    $$\Rightarrow \dfrac { t }{ T } -\dfrac { 25 }{ \lambda  } =0.08$$                  ....(iv)
    Subtracting equation (iv) from equation (iii), we get
    $$\dfrac { 15 }{ \lambda  } =0.06$$
    $$\Rightarrow \lambda =250 cm$$
  • Question 5
    1 / -0
    The equation of a simple harmonic wave is given by $$y = 6 \sin{2\pi} \left(2t-0.1x\right)$$, where $$x$$ and $$y$$ are in $$mm$$ and $$t$$ is in seconds. The phase difference between two particles $$2 mm$$ apart at any instant is
    Solution
    Given equation can be written as $$y = 6\sin(4\pi t- 0.2\pi x)$$
    $$\therefore$$ Phase $$\phi = -0.2\pi x$$
    $$\Rightarrow\phi_1 = -0.2\pi x_1$$ and $$\phi_2 = -0.2\pi x_2$$
    $$\therefore$$ Phase difference $$\Delta\phi =|\phi_2 - \phi_1| =| -0.2\pi(x_2-x_1)|$$
    given $$(x_2 - x_1) = 2mm$$ substituting in above equation we get $$\Delta\phi = 0.2\times{180^0}\times{2} = 72^0$$
  • Question 6
    1 / -0
    Two particles A and B execute simple harmonic motions of periods T and 5T / 4. They start from mean position. The phase difference between them when the particle A complete one oscillation will be:
    Solution
    Equations of motion of the practicals are
    $$X_1=A_1 sin \dfrac{2\pi}{T_1}t$$
    and $$ X_2=A_2 sin \dfrac{25}{T_2}t$$
    $$\therefore $$ Phase difference $$\Delta \phi =\left ( \dfrac{2\pi}{T_1}-\dfrac{2\pi}{T_2} \right )t$$
    $$=\left ( \dfrac{2\pi}{T}-\dfrac{2\pi}{5T/4} \right )t$$
    at t=T
    $$\Delta \phi =\left ( 2 \pi -\dfrac{4 \times 2\pi}{5} \right )\frac{T}{T}=\dfrac{2\pi}{5}$$
  • Question 7
    1 / -0
    The phenomena during arising due to the superstition of waves is/are :
    Solution
    Beat stationary waves, lissajous figures all correspond to the phenomena of superposition of waves.
  • Question 8
    1 / -0
    A progressive wave is represented as $$y=0.2\cos \pi (0.04 t+0.2x-\dfrac{\pi}{6})$$ where distance is expressed in cm and time in second. What will be the minimum distance between two particles having the phase difference of $$\dfrac{\pi}{2}$$?
    Solution
    On comparing the given equation with
    $$y=a\cos (\omega t + kx - \phi)$$
    we get, $$k=\dfrac{2\pi}{\lambda}=0.02$$
    and $$\lambda = 100 cm$$
    It is given that phase difference between particles $$\triangle \phi = \dfrac{\pi}{2}$$
    So, the path difference between them, 
    $$\triangle p = \dfrac{\lambda}{2\pi}\times \triangle \phi$$
    $$=\dfrac{\lambda}{2\pi}\times \dfrac{\pi}{2}=\dfrac{\lambda}{4}=\dfrac{100}{4}=25 cm$$
  • Question 9
    1 / -0
    With the propagation of a longitudinal wave through a material medium the quantities transmitted in the propagation direction are
    Solution
    $$\textbf{Explanation}$$
    $$\bullet$$In longitudinal wave,particle vibrates in the direction of motion of wave.
    $$\bullet$$When wave travels it means energy transfers from one end to other in the direction of propagation of wave.
    $$\bullet$$Particles vibrate in the direction of propagation of wave so linear momentum also transmitted in the direction of propagation of wave.
  • Question 10
    1 / -0
    At a moment in a progressive wave, the phase of a particle executing SHM is $$\dfrac {\pi}{3}$$. Then the place of the particle $$15\ cm$$ ahead and at time $$\dfrac {T}{2}$$ will be, if the wavelength is $$60\ cm$$.
    Solution
    Let the phase of second particle is $$\phi$$. Hence the phase difference two particles is $$\triangle \phi = \dfrac {2\pi}{\lambda} \triangle x$$
    $$\left (\phi - \dfrac {\pi}{3}\right ) = \dfrac {2\pi}{60}\times 15$$
    $$\phi = \dfrac {\pi}{2} + \dfrac {\pi}{3}$$
    $$\phi = \dfrac {5\pi}{6}$$.
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