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Oscillations Test - 36

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Oscillations Test - 36
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  • Question 1
    1 / -0
    The maximum velocity of a particle, executing simple harmonic motion with an amplitude $$7$$ mm, is $$4.4$$ m/s. The period of oscillation is :
    Solution
    $$v= \omega A =\frac{2\pi}{T}A$$
    Take $$\pi \approx 22/7$$
  • Question 2
    1 / -0
    A particle is executing SHM with amplitude of 4 cm and has a maximum velocity of 10 cm/sec.
    (a) At what displacement its velocity is 4 cm/sec?
    (b) What is its velocity at displacement 2 cm?
    Solution
    (a) In SHM velocity at any position y is given by
    v = $$\omega$$ $$\sqrt{A^{2} - y^{2}}$$
    $$V_{max} = A \omega$$ at y = 0
    10 = 4 $$\omega$$ $$\omega$$ = 5/2 rad/sec.
    Now V = 4 cm/sec.at
    4 = 5/2 $$\sqrt{4^{2} - y^{2}}$$
    16 - $$y^{2}$$ = 2.56
    $$y^{2}$$ = 13.46
    y = $$\pm$$ $$\sqrt{13.46}$$ cm = $$\pm$$3.66cm
    (b) At y = 2cm
    v = 5/2 $$\sqrt{4^{2} - 2^{2}}$$ = 5/2 x 2$$\sqrt{3}$$ = 5 $$\sqrt{3}$$ = 8.66 cm
  • Question 3
    1 / -0
    If two springs of spring constant $$k_1$$ and $$k_2$$ are connected together in parallel, the effective spring constant will be
    Solution
    the effective spring constant = $$k_1+k_2$$

    the correct option is (a)
  • Question 4
    1 / -0
    A small solid cylinder of mass M attached to a horizontal massless spring can roll without slipping along a horizontal surface. find its time period.
    Solution
    At any instant of rolling the cylinder has rotational and translational kinetic energy.
    $$K_{rot}$$ = 1/2 l$$\omega^{2}$$ = 1/2 1/2M$$R^{2}$$ $$v^{2}$$/$$R^{2}$$ = 1/4 M$$v^{2}$$.
    $$K_{trans}$$ = 1/2 $$Mv^{2}$$
    $$U_{potential}$$ = 1/2 $$Kx^{2}$$ 
    Total energy E = $$k_{rot}$$ + $$K_{trans}$$ + U
    E = 3/4 $$Mv^{2}$$ + 1/2 $$Kx^{2}$$
    Here DE/dt = 3/4M(2v) dV/dt $$\div$$ 1/2 k2x dx/dt = 0
    Or, dv/dt = -2k 3M x
    Hence $$\alpha$$ = $$-\omega^{2}$$x
    Therefore the motion is simple harmonic
    $$\omega$$ = 2k/3M
    T = 2$$\pi$$ $$\sqrt{3M/2k}$$
  • Question 5
    1 / -0
    A body executing $$S.H.M.$$ along a straight line has a velocity of $$3\ ms^{-1}$$ when it is at a distance of $$4\ m$$ from its mean position and $$4\ ms^{-1}$$ when it is at  a distance of $$3\ m$$ from its mean position. Its angular frequency and amplitude are:
    Solution
    Velocity $$v=\omega \sqrt{A^2-X^2}$$
    $$3=\omega \sqrt{A^2-4^2}$$...(1)
    $$4=\omega\sqrt{A^2-3^2}$$...(2)
    $$\dfrac{3}{4} =\dfrac{\sqrt{A^2-4^2}}{\sqrt{A^2-3^2}}$$
    $$\dfrac{9}{16} =\dfrac{A^2-16}{A^2-9}$$
    $$16A^2-9A^2=16^2-9^2$$
    $$7A^2=175$$
    $$A^2=25$$
    $$A=5$$
    From (1), $$3=\omega \sqrt{5^2-4^2}$$
    $$\omega=1 rad/sec$$

  • Question 6
    1 / -0
    Two particles $$A$$ and $$B$$ of equal masses are suspended from two massless springs of spring constants $$k_1$$ and $$k_2$$ respectively. If the maximum velocities, during oscillations, are equal, the ratio of amplitudes of $$A$$ and $$B$$ is :
    Solution

  • Question 7
    1 / -0
    The acceleration displacement $$(a-x)$$ graph of a particle executing simple harmonic motion is shown in the figure. Find the frequency of oscillation.

    Solution
    Equation of given graph will be,
    $$a=-\dfrac{\beta}{\alpha}X$$....(1)
    $$a=-\omega^2X$$...(2)
    Comparing both equations, $$\omega=\sqrt{\dfrac{\beta}{\alpha}}$$
    So, frequency, $$f = \dfrac{\omega}{2\pi} = \dfrac{1}{2\pi}\sqrt{\dfrac{\beta}{\alpha}}$$
  • Question 8
    1 / -0
    A particle executes SHM with a time period of 12 s. Find the time taken by the particle to go directly from its mean position to half of its amplitude.
    Solution
    We know,
    Equation of SHM,

    $$y=A\sin\left(\dfrac{2\pi t}{T}\right)$$
     Where, A=Amplitude,T=time period

    At $$y=0$$ mean position,
    $$0=A\sin\left(\dfrac{\pi t}{6}\right)$$
    i.e $$t=0$$

    At $$y=\dfrac{A}{2}$$
    $$\dfrac{A}{2}=A\sin\left(\dfrac{\pi t}{6}\right)$$
    i.e $$t=1s$$

    Difference in times, is the time taken to reach from mean to half of the Amplitude,
    i.e $$1\ sec$$

    Option $$\textbf B$$ is the correct answer.
  • Question 9
    1 / -0
    A simple harmonic motion along the $$x$$-axis has the following properties: amplitude = $$0.5\ m$$, the time to go from one extreme position to other is, $$2\ s$$ and $$x = 0.3\ m$$ at $$t = 0.5\ s$$. The general equation of the simple harmonic motion is
    Solution
    $$x=A \sin(\omega t+\phi)$$
    $$A=0.5$$
    Half time period $$\dfrac{T}{2}=2sec$$
    $$T=4sec$$
    $$\omega=\dfrac{2\pi}{T}=\dfrac{\pi}{2}$$
    $$x=0.5\sin(\dfrac{\pi}{2}t+\phi)$$....(1)
    At $$t=0.5 sec,x=0.3$$ putting in (1),
    $$0.3=0.5\sin(\dfrac{\pi}{2}\times 0.5+\phi)$$
    $$\dfrac{3}{5}=\sin(\dfrac{\pi}{4}+\phi)=\sin(45+\phi)$$
    $$45+\phi=37^\circ$$
    $$\phi=-8^\circ$$
    So, $$x=(0.5m)\sin(\dfrac{\pi}{2}t-8^\circ)$$
  • Question 10
    1 / -0
    The elastic potential energy of a stretched spring is given by $$E=50{x}^{2}$$ where $$x$$ is the displacement in meter and $$E$$ is in joule, then the force constant of the spring is
    Solution
    Let the force constant of the spring be $$k$$.
    Elastic potential energy of a spring is given by $$E$$ =$$\dfrac{1}{2}kx^{2}$$.                  ....(i)
    Given , elastic potential energy of stretched spring is $$E$$ = $$50$$ $$x^{2}$$      ....(ii)
    Comparing equations (i) and (ii) :
    $$\dfrac{1}{2}kx^{2}$$ = $$50$$ $$x^{2}$$
    We get $$k$$ = $$100$$ $$\dfrac{J}{m^{2}}$$ .
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