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Oscillations Test - 14

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Oscillations Test - 14
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  • Question 1
    1 / -0
    A particle of mass $$3$$kg, attached to a spring with force constant $$48$$ N/m execute simple harmonic motion on a frictionless horizontal surface. The time period of oscillation of the particle, in seconds, is?
    Solution
    The time period of mass,
    $$T=2\pi\sqrt{\dfrac{m}{k}}$$
    Given, $$m=3$$kg
    $$k=48$$N/m
    $$T=2\pi\sqrt{\dfrac{3}{48}}=2\pi\sqrt{\dfrac{1}{16}}$$
    $$=2\pi\times \dfrac{1}{4}=\dfrac{\pi}{2}$$.
  • Question 2
    1 / -0
    The displacement of a particle varies with time, according to the equation $$y = a \sin \omega  t + b \cos \omega t$$
    Solution
    (d) : $$y = a \sin \omega t + b \cos  \omega t$$

    The amplitude of motion is given by 
     
    $$A = \sqrt{a^{2} + b^{2}}$$

    Hence, verifies the option (d).
  • Question 3
    1 / -0
    The diagram shows a ball hanging on a string. The ball swings from point $$W$$ to point $$Z$$ and back to point $$W$$.
    Which statement about the ball is correct?

    Solution
    It is a case of simple pendulum . 
    we know that
    by conservation of energy
    $$KE+PE=$$ constant.
    At point Y , PE is min.
    So, the kinetic energy at mean position is maximum in this case.
    Since ,Y is the mean position , so, the kinetic energy is max. at point $$Y$$.
  • Question 4
    1 / -0
    The velocity of a particle performing simple harmonic motion, when it passes through its mean position is 
    Solution
    Equation of SHM particle 
    $$Y=a\sin \omega t\\V=a\omega \sin\omega t$$
    $$V_{max}=a\omega$$
  • Question 5
    1 / -0
    The length of simple pendulum is increased by $$1\%$$. Its period will
    Solution
              $$T\propto \sqrt {l}$$

    $$\Rightarrow \dfrac {\Delta T}{T}=\dfrac {1}{2}\dfrac {\Delta l}{l}=\dfrac {1}{2}\times 1\% =0.5\%$$
  • Question 6
    1 / -0
    If a simple pendulum is taken to place where $$g$$ decreases by $$2\%$$ then the time period
    Solution
    Time period for simple pendulam,
    $$T=2\pi \sqrt{\dfrac{l}{g}}$$
    $$\Rightarrow T\propto \dfrac{1}{\sqrt{g}}$$

    $$\Rightarrow \dfrac{\Delta T}{T}\times 100=-\dfrac{1}{2}\left(\dfrac{\Delta g}{g}\right)\times 100=-\dfrac{1}{2}(-2\%)=1\%$$
  • Question 7
    1 / -0
    A simple pendulum is vibrating in an evacuated chamber, it will oscillate with
    Solution
    As it is clear that in vacuum, the bob will not experienced any frictional force. Hence therefore shall be no dissipation therefore, it will oscillation with constant amplitude.
  • Question 8
    1 / -0
    The amplitude of a particle performing S.H.M. is $$A$$. The displacement at which its velocity will be half of the maximum velocity is 
    Solution
    $$x = A sin \omega t$$
    $$V=\dfrac{dx}{dt}=A\omega cos \omega t$$
    $$V_{max} =A  \omega$$
    $$V=\dfrac{V_{max}}{2}= A \omega  cos \omega t$$
    $$\Rightarrow \dfrac{A  \omega }{2}=A  \omega cos \omega t$$
    $$\Rightarrow cos \omega t=\dfrac{1}{2}$$
    $$\Rightarrow \omega t =60^{0}$$
    $$x=A sin \omega t$$
    $$=A  sin  60^{0}$$
    $$=A \dfrac{\sqrt{3}}{2}$$
    so, amplitude is $$\dfrac{\sqrt{3}A}{2}$$
  • Question 9
    1 / -0
    Acceleration-displacement graph of a particle executing SHM is as shown in the figure. The time period of oscillation is (in sec)

    Solution
    In SHM
    $$a=-\omega^2x$$
    or
    $$a= \dfrac{-K}{m}x$$
    so, from graph
    $$-\dfrac{K}{m}= -1$$                   $$ ( \because slope\ is\ -1)$$
    $$\dfrac{K}{m}= 1$$
    Time period $$= 2\pi \sqrt{\dfrac{m}{K}}$$
    $$= 2\pi \sqrt{\dfrac{1}{1}}$$
    $$= 2\pi $$
  • Question 10
    1 / -0
    The equation of the displacement of two particles making SHM are represented by 
    $$ y_{1} $$ = a sin $$ \left ( \omega t +\phi \right ) $$ & $$ y_{2} $$ = a cos $$ \left ( \omega t \right ) $$. 
    The phase difference of the velocities of the two particles is :
    Solution
    $$y_{1}=a    sin (\omega t+\phi  )$$
    $$y_{2}=a   cos (\omega t)$$
    $$y_{1}=a   \omega cos (\omega t+\phi)=a \omega sin (\omega t+\phi +{\pi}/_{2})$$
    $$y_{2}=-a   \omega sin (\omega t)= a \omega sin (\pi + \omega t)$$
    therefore phase difference$$ = \omega t+\phi +{\pi}/_{2}-(\pi+\omega t)$$
    $$=\phi -{\pi}/_{2}$$

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