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Waves Test - 29

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Waves Test - 29
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  • Question 1
    1 / -0
    An ultrasonic scanner is used in a hospital to detect tumours in tissue. The working frequency of the scanner is 4.2 mega Hz. The velocity of sound in the tissue is $$1.7 kms^{-1}$$. The wavelength of sound in the tissue is nearest to 
    Solution
    Let,

    The working frequency of the scanner is $$\nu = 4.2 MHz = 4.2 \times 10^6 Hz$$. 

    The velocity of sound in the tissue is $$v = 1.7 kms^{-1} = 1.7 \times 10^3 ms^{-1}$$

    the wavelength of sound is given by

    $$\lambda = \dfrac{v}{\nu}$$

    $$\lambda = \dfrac{1.7 \times 10^3}{4.2 \times 10^6}$$

    $$\lambda = 0.404 \times 10^{-3}$$

    $$\lambda \approx 4 \times 10^{-4} m$$
  • Question 2
    1 / -0
    In a Kundt's tube experiment, the heaps of lycopodium powder are collected at $$20\ cm$$ separations. The frequency of tuning fork used is
    Solution
    The in kundt's tube powder is collected where nodes are formed. The separation between nodes is given as 

    $$d=\dfrac{\lambda}{2} =20 cm$$

    $$\lambda=40 cm$$

    $$f=\dfrac{c}{\lambda}$$$$=\dfrac{330}{.4} =825 \ Hz$$
  • Question 3
    1 / -0
    Two wires with different densities are joined at $$x = 0$$. An incident wave $$Y_i = A_i\sin(\omega t -k_1x)$$ travelling from left to right is partially reflected and partially transmitted $$(Y_t = A_t\sin(\omega t -k_2x))$$ at $$x = 0$$. If the amplitude of transmitted wave is $$A_t$$ then $$^{\Large A_t}/_{\Large A_i}$$ is
    Solution
    Let the equation of reflected wave be $$A_rsin(\omega t+k_1x)$$
    The sign is reversed to include the reversed direction of the reflected wave.
    From continuity of the wave at the interface $$x=0$$, we get,
    $$A_i+A_r=A_t$$
    Also the first derivative of the wave are continuous at the boundary, hence,
    $$k_1(A_i-A_r)=k_2A_t$$
    $$\implies A_i-A_r=\dfrac{k_2}{k_1}A_t$$
    Rearranging the two equations gives,
    $$\dfrac{A_t}{A_i}=\dfrac{2k_1}{k_1+k_2}$$
  • Question 4
    1 / -0
    The displacement $$y$$ in centimeters is given in terms of time $$t$$ in second by the equation: $$y=3\sin 3.14t+4\cos 3.14 t$$, then the amplitude of SHM is
    Solution
    When the displacement of a SHM is $$y=a\sin wt+b\cos wt$$, the amplitude of the SHM will be $$A=\sqrt{a^2+b^2}$$
    Here, $$a=3, b=4$$ so amplitude $$A=\sqrt{3^2+4^2}=5 $$ cm
  • Question 5
    1 / -0
    The equation of displacement of a harmonic oscillator is $$x=3\sin{\omega t}+4\cos{\omega t}$$. The amplitude of the particles will be
    Solution
    In the equation of superposition of SHMs or Harmonic oscillator, $$x=asin\omega t+bsin\omega t$$, the resultant amplitude is given by $$A=\sqrt{a^{2}+b^{2}}$$. Substituting a=3 and b=4, we get final answer as Option B, i.e. 5
  • Question 6
    1 / -0
    The wavelength of a sound wave is reduced by 50%. Then the percentage change in its frequency will be
    Solution
    The wavelength of sound wave is
    $$\lambda = \dfrac{v}{\nu}$$
    $$\nu = \dfrac{v}{\lambda}$$
    where, v is the velocity of sound waves and $$\nu$$ is the frequency of sound waves.
    When the wavelength of a sound wave is reduced by 50% 
    $$\lambda - \dfrac{50}{100}\lambda = \dfrac{v}{\nu'}$$
    $$\dfrac{1}{2}\lambda = \dfrac{v}{\nu'}$$
    $$\nu' = \dfrac{2v}{\lambda}$$
    The percent change in frequency is
    $$\dfrac{\nu - \nu'}{\nu} \times 100 = \dfrac{\dfrac{2v}{\lambda} - \dfrac{v}{\lambda}}{\dfrac{v}{\lambda}} \times 100$$
    $$\Rightarrow  (2 - 1) \times 100 = 100$$%
  • Question 7
    1 / -0
    If the frequency of a sound wave is increased by 25%, then the change in its wavelength will be
    Solution
    The frequency  of wave is given by

    $$\nu = \dfrac{v}{\lambda}$$

    $$\lambda = \dfrac{v}{\nu}$$

    When the frequency of a sound wave is increased by 25%, then the new 
    wavelength is

    $$\lambda' = \dfrac{v}{\nu+\dfrac{25}{100}\nu}$$

    $$\lambda' = \dfrac{v}{\nu+\dfrac{1}{4}\nu}$$

    $$\lambda' = \dfrac{v}{\dfrac{5}{4}\nu}$$

    $$\lambda' = \dfrac{4v}{5\nu}$$

    Hence, the percent change in wavelength is

    $$\dfrac{\lambda - \lambda'}{\lambda} \times 100 = \dfrac{\dfrac{v}{\nu} - \dfrac{4v}{5\nu}}{\dfrac{v}{\nu}} \times 100$$

    $$\Rightarrow -\dfrac{1}{4} \times 100 = -20$$%.

    Hence, wavelength decreases by 20%
  • Question 8
    1 / -0
    A sound wave of frequency $$500\ \text{Hz}$$ covers a distance of  $$1000\ \text{m}$$ in $$5\ \text{s}$$ between points $$\displaystyle x$$ and $$\displaystyle y$$. Then the number of waves between $$\displaystyle x$$ and $$\displaystyle y$$ are
    Solution
    $$\nu= 500\ \text{Hz}$$

    $$x= 1000$$

    $$t= 5\ \text{s}$$

    velocity of sound  $$v=\dfrac{x}{t} = 200\ \text{m/s}$$

    But $$v= \nu \lambda$$

    Hence, $$\lambda = \dfrac{2}{5}\ \text{m/s}$$

    Now $$n\lambda = x\ \text{or}\ n = 2500$$

    Ans: B
  • Question 9
    1 / -0
    A sonometer wire, $$100\ \text{cm}$$ in length has a fundamental frequency of $$330\ \text{Hz}$$. The velocity of propagation of transverse waves along this wire is :
    Solution
    For the fundamental frequency $$(f_0=330 Hz),\ \lambda=2 L=200\ \text{cm} = 2\ \text{m}$$

    then from the formula, $$v=f_0 \times \lambda= 330 \times 2.0= 660 \text{ms}^{-1}$$
  • Question 10
    1 / -0
    Interference event is observed
    Solution
    Interference occurs for both transverse and longitudinal waves.
    Interference does not indicate whether light is transverse or longitudinal since interference occurs for both types of waves.
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