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Oscillations Test - 35

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Oscillations Test - 35
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  • Question 1
    1 / -0
     The amplitude of a simple pendulum, oscillating in air with a small spherical bob, decreases from $$10\ cm$$ to $$8\ cm$$ in $$40$$ seconds. Assuming that Stokes law is valid, and ratio of the coefficient of viscosity of air to that of carbon dioxide is $$1.3$$, the time In which amplitude of this pendulum will reduce from $$10\ cm$$ to $$5\ cm$$ in carbon dioxide will be close to (ln $$5=1.601, \ln { 2 }  2=0.693$$)
    Solution
    $$\textbf{Solution}:$$
    We know that the amplitude of damped oscillation is 
    $$A=A_0 e^{\dfrac{-bt}{2m}}$$ 

    $$\implies 8=10e^{(-\dfrac{b_{air} \times 40}{2m})}$$ 

    and
    $$5=10e^{-(\dfrac{b_{co_2} \times t_2}{2m})}$$ 

    $$\implies  \dfrac{In\dfrac{5}{4}}{In2}=\dfrac{b_{air} \times 40}{b_{co_2} \times t_2}$$ 

    Therefore , 

    $$t_2=\dfrac{b_{air}}{b_{co}} \times \dfrac{40 \times In2}{In\dfrac{5}{4}}=161s$$


    $$\textbf{Hence C is the correct option}$$
  • Question 2
    1 / -0
    The potential energy of a particle of mass 10g varies as its displacement from its mean position given by $$U = 3x^2 + 3$$, then, the particle performs a
    Solution
    The force acting on the system is $$F = -dU/dx = -6x \implies a=-(6/0.01)x=-600x$$. The angular velocity of the particle is $$\omega= \sqrt{600}$$

    Thus, the motion of the particle is SHM with time period $$T=2 \pi/\sqrt{600} $$ or $$T = \pi/5\sqrt{6}$$ s

    The correct option is (c)
  • Question 3
    1 / -0
    A particle executes SHM along x axis and is at the mean position at t=0. What is its velocity at its mean position. The amplitude of SHM is 5 cm and angular frequency is 2 rad/s:
    Solution
    The particle has its maximum velocity at mean position and is given by $$v=A \omega = 10 $$ cm/s

    The correct option is (b)
  • Question 4
    1 / -0
    A particle executes SHM given by the equation $$x = 4 sin (2 \pi t +\pi/4)$$, what will be the velocity of the particle at t = (1/8)th sec; 
    Solution
    $$x = 4 sin (2 \pi t +\pi/4)$$
    Differentiating x w.r.t. t, we get, $$dx/dt =v = 8 \pi cos (2 \pi t +\pi/4)$$
    Substituting t = 1/8, we get, $$v=8 \pi cos (2 \pi t +\pi/4)= cos (\pi/2)=0$$

    At t = 1/8th of a sec, the particle's velocity will be zero . Thus we infer that the particle is at the extreme position

    The correct option is (a)

  • Question 5
    1 / -0
    The potential energy of a particle is directly proportional to its linear displacement from its mean position. Then, the particle performs a
    Solution
    Potential energy U = Kx. Thus the force acting is = -dU/dx = -K

    The force is a retarding constant force and the motion of the particle will be in a straight line

    The correct option is (a)
  • Question 6
    1 / -0
    At what position along a straight line will the velocity be zero for a particle executing SHM
    Solution
    The velocity and displacement follows an equation given by $$v^2=\omega (A^2-x^2)$$. If v has to be zero, then x=A.

    If the particle was at the extreme, the particle will have a zero velocity

    Thus the correct option is option(c)
  • Question 7
    1 / -0
    A particle performs simple harmonic motion with amplitude A. Its speed is tripled at the instant that is at a distance $$\dfrac{2A}{3}$$ from equilibrium position. The new amplitude of the motion is:
    Solution
    $$3\omega \sqrt {A^2-\left(\dfrac{2A}{3}\right)^2}=\omega \sqrt{A_1^2-\left(\dfrac{2A}{3}\right)^2}$$
    $$\therefore A_1=\dfrac{7A}{3}$$
  • Question 8
    1 / -0
    What type of curve do we get, if $$x^2$$ and $$v^2$$ are plotted for a particle executing SHM, x and v are the position and velocity of the particle:
    Solution
    The equation of SHM, when the particle started at the mean position at t = 0 is given by $$x=A sin (\omega t )$$ 

    Differentiating x w.r.t. t, we get $$v = A \omega cos \omega t $$

    To eliminate $$\theta$$, we can do
    $$(x/A)^2 + (v/A \omega)=1 \implies $$ , the plot will be a circle

    The correct option is (c)
  • Question 9
    1 / -0
    A particle executes SHM from its mean position at t=0 with an amplitude A, what will be its velocity at x=A/2, in its forward motion towards the extreme:
    Solution
    The equation of SHM, when the particle started at the mean position at t = 0 is given by $$x=A sin (\omega t )$$ 

    At x=(A/2), the particle reaches it at time t  given by $$sin \omega t=0.5. \implies \omega t = \pi/6$$.

    Differentiating x w.r.t. t, we get $$v = A \omega cos \omega t. $$. Substituting the value of $$\omega t$$, we get $$v =A \omega cos 30 = \sqrt(3)A \omega/2$$

    The correct option is (a)  
  • Question 10
    1 / -0
    The time period of oscillation of magnet in a vibrating magnetometer is $$1.5$$ sec. The time period of oscillation of another magnet similar in size and mass but having one-fourth the magnetic moment than that of the first magnet oscillating at the same place will be 
    Solution
    $$\begin{array}{l} \dfrac { { { T_{ 1 } } } }{ { { T_{ 2 } } } } =\sqrt { \dfrac { { { M_{ 2 } } } }{ { { M_{ 1 } } } }  } =\sqrt { \dfrac { { { M_{ 1 } } } }{ { \dfrac { 4 }{ { { M_{ 1 } } } }  } }  } =\dfrac { { { T_{ 1 } } } }{ { { T_{ 2 } } } } =\dfrac { 1 }{ 2 }  \\ \Rightarrow { T_{ 2 } }=3 \end{array}$$
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