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Oscillations Test - 17

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Oscillations Test - 17
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  • Question 1
    1 / -0
    A simple harmonic oscillator is of mass $$0.100$$ kg. It is oscillating with a frequency of $$\dfrac{5}{\pi }$$Hz. If its amplitude of vibration is $$5$$ cm, the force acting on the particle at its extreme position is
    Solution
    $$ F   =  m   {\omega}^{2}  A$$
     $$\omega  =  2\pi  f = 10   rad  / sec$$
    $$F =  0.1 \times 100\times \dfrac{5}{100}$$
        $$  =  0.5  N  $$ 
  • Question 2
    1 / -0
    Two particles executing SHM of the same amplitude and frequency on parallel lines side by side. They cross one another when moving in opposite directions each time their displacement is $$\dfrac{\sqrt{3}}{2}$$ times their amplitude. The phase difference between them is:
    Solution
    since $$x=A\sin { \left( \omega t+\phi  \right)  }$$
    $$\\ \dfrac { \sqrt{3}A

    }{ 2 } =A\sin { \left( \omega t+\phi  \right)  } \\ \Rightarrow \sin {

    \left( \omega t+\phi  \right)  } =\dfrac{\sqrt{3}}{2} \\ \Rightarrow \omega

    t+\phi =60^{ \circ  }or\quad 120^{ \circ  }$$
    so the one particle has phase of $$60^{ \circ  }$$ and another has $$120^{ \circ  }$$
    So the phase difference is $$120^{ \circ  }-60^{ \circ  }=60^{ \circ  }$$
  • Question 3
    1 / -0
    A particle is in S.H.M of amplitude $$ 2$$ cm. At extreme position the force is $$4$$N. At the point mid-way between mean and extreme position, the force is :
    Solution
    Amplitude = 2 cm
    Force = 4N
    $$F = mw^{2}A=4$$
    $$F_{1} = mw^{2}x$$
    Since $$F$$ is directly proportional to $$x$$ so , at midpoint the force when the amplitude is $$2 \ cm$$ will be $$2N$$
  • Question 4
    1 / -0
    The average speed of S.H.M oscillator averaged over  $$\dfrac{3T}{8}$$ is
  • Question 5
    1 / -0
    The net external force acting on the disc when its centre of mass is at displacement $$x$$ with respect to its equilibrium position is:
    Solution
    $$\textbf{Given:- }$$ The net external force acting on the disc 

    $$\textbf{Solution:-}$$ Net Force acting on a body is given by the formula:  
               $$\vec{F_{net}} = m.\vec{a}$$
    Where,
    $$\vec{F_{net}}$$ is the net force acting on the body

    m is the mass of the body

    $$\vec{a}$$ is the acceleration of the body

    We will insert$$\left ( -2kx + F \right )$$ in the place of $$\vec{F_{net}}$$

    $$-2kx + F = Ma_{c}................(1)$$

    Where,
    k is the spring constant
    x is the distance by which the spring has been stretched
    F is the friction force on the disk
    M is the mass of disk
    $$a_{c}$$ is the acceleration of centre of mass of the disk

    Net Torque acting on a body is given by the formula,

    $$\vec{\tau _{net}} = I\vec{\alpha }...............(2)$$

    Where,

    $$\vec{\tau _{net}}$$ is the net Torque acting on the body

    I is the moment of inertia of the body

    $$\vec{\alpha }$$ is the angular acceleration of the body

    Additionally, Torque is also calculated as follows,
    $$\vec{\tau _{net}} = \vec{F}\times R................(3)$$

    Where,
    R is the distance of the Force from the center of mass of the body

    Now combining equations 2 and 3,

    $$\vec{F}\times R = T\vec{\alpha}$$

    $$\vec{F} = \dfrac{T\vec{\alpha}}{R}.................(4)$$

    In Pure Rolling condition,

    $$a_{c} = \vec{\alpha_{c}}R$$

    Moment of inertia of a disk is given by the formula,

    F $$= \dfrac{\dfrac{1}{2}MR^{2}}{R}\times \dfrac{a_{c}}{R}$$

    $$\Rightarrow F = \dfrac{1}{2}Ma_{c}$$

    Inserting the value of F in equation 1,

    $$\Rightarrow -2kx + \dfrac{1}{2}Ma_{c} = -Ma_{c}$$

    $$\Rightarrow \dfrac{1}{2}Ma_{c} + Ma_{c} = 2kx $$

    $$\Rightarrow \dfrac{3}{2}Ma_{c} = 2kx$$

    $$\Rightarrow Ma_{c} = \dfrac{4}{3}kx$$

    $$\Rightarrow MA_{c} = \dfrac{4}{3}kx$$

    $$\textbf{Hence the correct option is D}$$
  • Question 6
    1 / -0
    A particle executes SHM on a straight line path. The amplitude of oscillation is 2 cm. When the displacement of the particle from the mean position is 1 cm, the numerical value of the magnitude of acceleration is equal to the numerical value of the magnitude of the velocity. The frequency of SHM is:
    Solution

    Let y is the displacement $$y=a\sin \omega t$$

    $$\omega =\dfrac{2\pi }{T}$$

    It is given that,

    Displacement y = 1

    Amplitude a = 2

    So $$1=3\sin \dfrac{2\pi t}{T}$$

    Since, acceleration in SHM is $$a={{\omega }^{2}}y$$

    And velocity in SHM is $$v=\omega \sqrt{{{a}^{2}}-{{y}^{2}}}....(1)$$

    $$\because v=\omega $$

    Put all the values in equation (1)

    $$ \dfrac{4{{\pi }^{2}}}{{{T}^{2}}}=\dfrac{2\pi }{T}\left( \sqrt{{{a}^{2}}-1} \right) $$

    $$ \dfrac{2\pi }{T}=\left( \sqrt{3} \right) $$

    $$ T=\dfrac{2\pi }{\sqrt{3}} $$

  • Question 7
    1 / -0
    The number of independent constituent simple harmonic motions yielding a resultant displacement equation of the periodic motion as $$y=8 sin^{2}(\frac{t}{2})sin (10t)$$ is:
    Solution
    The resultant displacement equation of periodic motion is given by

    $$y=8sin^2(\dfrac{t}{2}). sin(10t)$$

    $$y=4.2sin^2(\dfrac{t}{2}). sin (10t)$$

    $$y=4[1-cost].sin(10t)$$   (as, $$2sin^2(\dfrac{t}{2})=1-cost$$)

    $$y=4sin(10t)-4sin(10t).cost$$

    $$y=4sin(10t)-2sin(11t)-sin(9t)$$ (as, $$2sinAtsinBt=sin(A+B)t+sin(A-B)t$$)

    There are three independent constituent simple harmonic motion.

    The correct option is D.
  • Question 8
    1 / -0
    A particle performs SHM with a period T and amplitude a. The mean velocity of the particle over thetime interval during which it travels a distance a/2 from the extreme position is
    Solution

  • Question 9
    1 / -0
    A particle is subjected to two mutually perpendicular simple harmonic motions such that its x andy coordinates are given by
    $$x=2 \sin \omega t; y=2 \sin \left ( \omega t+\frac{\pi }{4} \right )$$ 
    The path of the particle will be :
    Solution

  • Question 10
    1 / -0
    A spring is suspended under gravity with a block attached to it. The block oscillates in the vertical plane according to  $$x = a sin wt$$ with time period $$8$$ seconds. The ratio of velocities of the particle at $$t = 1$$ sec to $$t = 3$$ sec is
    Solution
    $$x = a sin \omega t$$
    $$V = \dfrac {dx}{xt} = a\omega cos \omega t$$
    $$T = \dfrac {2\pi}{\omega} ; \omega = \dfrac {2\pi}{T} = \dfrac {\pi}{4} \dfrac {rad}{sec}$$
    $$\dfrac {V_1}{V_2} = \dfrac {cos \omega t_1}{cos \omega t_2} = \dfrac {cos \dfrac {\pi}{4}}{cos \dfrac {3\pi}{4}} = \dfrac {1}{1}$$
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