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Waves Test - 34

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Waves Test - 34
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  • Question 1
    1 / -0
    A broadcasting station transmits waves of frequency $$71 \times 10^4 Hz$$ with a speed of $$3 \times 10^8 m/s$$. The wavelength of the wave is :
    Solution
    We have,   $$v=n\lambda$$ ,
    where $$v=$$ speed of the wave ,
               $$n=$$ frequency of the wave ,
               $$\lambda=$$ wavelength of the wave ,
    given   $$n=71\times10^{4}Hz   ,  v=3\times10^{8}m/s$$ ,
    therefore ,  $$\lambda=v/n=\dfrac{3\times10^{8}}{71\times10^{4}}=422.5m$$
  • Question 2
    1 / -0
    A certain transverse sinusoidal wave of wavelength $$20\ cm$$ is moving in the positive $$x-$$ direction. The transverse velocity of the particle at $$x = 0$$ as a function of time is shown. The amplitude of the motion is

    Solution
    $$\lambda =20cm,\quad T=4s$$
    From the figure
    $${ V }_{ max }=5cm/s=A\omega \\ A=\frac { 5 }{ \omega  } \\ A=\frac { 5 }{ { 2\pi  }/{ T } } =\frac { 5\times 4 }{ 2\pi  } \\ \left[ A=\frac { 10 }{ \pi  } cm \right] $$
    Hence option (C) is correct.
  • Question 3
    1 / -0
    An open pipe of length $$33$$cm resonates with frequency of $$1000Hz$$. If the speed of sound is $$330ms^{-1}$$, then this frequency is
    Solution
    Fundamental frequency (first harmonic frequency) of an open organ pipe is given by ,
                      $$n_{1}=v/\lambda=v/2l$$ ,
    where $$v=$$speed of sound in air ($$=330m/s , given$$),
               $$\lambda=$$ wavelength ,
               $$l=$$ length of organ pipe ($$=33cm=0.33m$$  , given) ,
    therefore ,  $$n_{1}=330/(2\times0.33)=500Hz$$ ,
    as an open pipe produces even and odd harmonics , and given frequency is 1000Hz , it is 2 times of the first harmonic frequency , therefore it is second harmonic frequency of the pipe .
  • Question 4
    1 / -0
    A particle of mass $$0\cdot 50\ kg$$ executes a simple harmonic motion under a force $$F = -(50\ N/m)x$$. If it crosses the centre of oscillation with a speed of $$10\ m/s$$, then the amplitude of the motion is
    Solution
    A particle executing S.H.M acted upon by a force 
    F = -(50N/m)$$x$$
    it mess m= 0.5kg
    so, a = F/m = acceleration 
    $$\Rightarrow a = -100 x$$
    $$\Rightarrow a+{\omega}^{2} x = 0$$
    $$\omega$$ = angular frequency $$=\sqrt { 100 } =10 rad/s$$
    velocity at mean position 
    $$\omega A = 10/s$$    A = amplitude of oscillation
    $$\Rightarrow A = \dfrac{10}{10} = 1m$$
  • Question 5
    1 / -0
    A broadcasting station transmits waves of frequency $$71\times 10^4Hz$$ with speed of $$3\times 10^8m/s$$. The wavelength of the wave is :
    Solution
    We have,   $$v=n\lambda$$ ,
    where $$v=$$ speed of the wave ,
               $$n=$$ frequency of the wave ,
               $$\lambda=$$ wavelength of the wave ,
    given   $$n=71\times10^{4}Hz   ,  v=3\times10^{8}m/s$$ ,
    therefore ,  $$\lambda=v/n=\dfrac{3\times10^{8}}{71\times10^{4}}=422.5m$$
  • Question 6
    1 / -0
    Two wave pulses travel in opposite directions on a string and approach each other. The shape of the one pulse is the invert with respect to the other, then
    Solution
    As the two wave pulses approach each other on the same string, they do not affect the shape of one another and will pass as they are invert of each other.

    when the wave pulses overlap the wave function is the sum of individual wave functions. AT the point where two waves pulses meet, net displacement will be zero.

    Option $$D$$ is correct.
  • Question 7
    1 / -0
    Speed of sound in air is $$350ms^{-1}$$, fundamental frequency of an open organ pipe of $$50$$cm length will be
    Solution
    Fundamental frequency of an open organ pipe is given by ,
                      $$n_{1}=v/\lambda=v/2l$$ ,
    where $$v=$$speed of sound in air ($$=350m/s , given$$),
               $$\lambda=$$ wavelength ,
               $$l=$$ length of organ pipe ($$=50cm=0.50m$$  , given) ,
    therefore ,  $$n_{1}=350/(2\times0.50)=350Hz$$
  • Question 8
    1 / -0
    The amplitude of an oscillating simple pendulum is 10 cm and its time period is 4 s. Its speed after 1 s when it passes through its equilibrium position is:
    Solution
    In case of SHM, when motion is considered from the equilibrium position, displacement is, y = a sin $$\omega$$t.

    So velocity, $$\displaystyle v = \dfrac{dy}{dt} = a\omega  cos  \omega t$$

    $$= a \displaystyle \left ( \frac{2 \pi}{T} \right ) cos \left ( \frac{2 \pi}{T} \right ) t$$

    $$= 0.1 \displaystyle \left ( \frac{2 \pi}{4} \right ) cos \left ( \frac{2 \pi}{4} \right ) \times 1 = 0.05 cos \frac{\pi}{2} = 0$$
  • Question 9
    1 / -0
    Unit of frequency is........................
    Solution

  • Question 10
    1 / -0
    Energy is not propagated by
    Solution
    standing wave patterns are produced as the result of the repeated interference of two waves of identical frequency while moving in opposite directions along the same medium. so in standing waves particles are stationary so propogation of energy cannot take place.
    so answer is A.
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