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Waves Test - 67

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Waves Test - 67
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  • Question 1
    1 / -0
    Two sine waves travel in the same direction in a medium. The amplitude of each wave is A and the phase difference between the two waves is 120120^{\circ}. The resultant amplitude will be
    Solution

  • Question 2
    1 / -0
    Two point lie on a ray are emerging from a source of simple harmonic wave having period 0.0450.045. The wave speed is 300 m/s300\ m/s and points are at 10 m10\ m and 16 m16\ m from the source. They differ in phase by :
    Solution

  • Question 3
    1 / -0
    A simple harmonic wavetrain of amplitude 5 cm5\ cm and frequency 100 Hz100\ Hz is travelling in the positive xx- direction with a velocity of 30 m/s30\ m/s. The displacement velocity and acceleration at t=3st=3s of a particle of the medium situated 100 cm100\ cm from the origin are respectively.
    Solution
    y=Asin(2πμv(vtx))y=A\sin (\dfrac{2\pi \mu}{v}(vt-x))

    y=5sin(2π1003000(3000×3100))=4.45cmy=5\sin (\dfrac{2\pi 100}{3000}(3000\times 3-100))=-4.45cm

    velocity= dydx=A×2πμcos(2πμv(vtx))=5×2π×100cos(2π×1003000(3000×3180))=1571cm/s\dfrac{dy}{dx}=A\times 2\pi\mu\cos(\dfrac{2\pi\mu}{v}(vt-x))=5\times 2\pi\times 100\cos(\dfrac{2\pi\times 100}{3000}(3000\times 3-180))=1571cm/s

    accleration=d2ydx2=A×4π2μ2sin(2πμv(vtx))=5×4π2×10000sin(2π×1003000(3000×3180))=171×104cm/s2\dfrac{d^2y}{dx^2}=-A\times 4\pi^2\mu^2sin(\dfrac{2\pi\mu}{v}(vt-x))=-5\times 4\pi^2\times 10000\sin(\dfrac{2\pi\times 100}{3000}(3000\times 3-180))=171\times 10^{4}cm/s^2

  • Question 4
    1 / -0
    Two identical pulses move in opposite directions with same uniform speeds on a stretched string. The width and kinetic energy of each pulse is LL and kk respectively. At the instant they completely overlap, the kinetic energy of the width LL of the string where they overlap is:

    Solution
    y1=asin(2πx/L)y_1=a\sin(2\pi x /L)
    When they get combined: y2=2asin(2πx/L)y_2=2asin(2\pi x/L)
    We know particle velocity= wave velocity x dy/dx
    As in both the cases wave velocities are the same
    v1v2=dy1dxdy2dx=12v2=2v1\dfrac{v_1}{v_2}=\dfrac{\dfrac{dy_1}{dx}}{\dfrac{dy_2}{dx}}=\dfrac{1}{2}\Rightarrow v_2=2v_1 

    KE1KE2=v12v22=14KE2=4×KE1=4k\dfrac{KE_1}{KE_2}=\dfrac{{v_1}^2}{{v_2}^2}=\dfrac{1}{4}\Rightarrow KE_2=4\times KE_1=4k
  • Question 5
    1 / -0
    A wave motion has the function Y=a0sin(ωtkx)Y=a_{0}\sin (\omega t-kx). The graph in the figure shows how the displacement yy at a fixed point varies with time tt. Which one of the labeled points shows a displacement equal to that at the position x=π/2kx=\pi/2k at time t=0t=0

    Solution
    Given ,
     Y=a0sin(ωtkx)Y=a_{0}\sin (\omega t-kx).
    Now,  at x=π2k and t=0x=\dfrac{\pi}{2k} \ and\ t=0
    we get,
     Y=a0sin(ω(0)k(π2k)Y=a_{0}\sin (\omega (0)-k(\dfrac{\pi }{2k}).

    Y=a0Y=-a_0
    from the figure point (Q) shows a displacement equal to (-a_0).
    hence, option B is correct
  • Question 6
    1 / -0
    A simple harmonic plane wave propagates along x-axis in a medium. The displacement of the particles as a function of time is shown in figure, for x=0x = 0 (curve 1) and x=7x = 7 (curve 2).
    The two particles are within a span of one wavelength.
    The speed of the wave is

    Solution
    Let general wave equation is y=Asin(ωtkx+ϕ)y = A \,sin (\omega t - kx + \phi)
                                    v=dydt=Aωcos(ωtkx+ϕ)v = \dfrac {dy}{dt} = A \omega cos (\omega t - kx + \phi)
    for curve (1),x=0(1 ) , x = 0
    at                   t=0,x=0,t = 0, x = 0 , we have y=0 y = 0
                          0=Asin[ϕ]sinϕ=0\Rightarrow 0 = A \,sin[\phi] \Rightarrow sin \phi = 0
                          ϕ=0orπ\Rightarrow \phi = 0 \,or \,\pi
    here ϕ=π\phi = \pi (because velocity is negative)
    for curve (2),x=7cm(2), x = 7 \,cm
     at           t=0,x=7cm,y=1t = 0, x = 7 \,cm, y = -1
                  1=sin(k×7+π)-1 = sin(-k \times 7 + \pi)
                 sin(7k+π)=1/2\Rightarrow sin(-7k + \pi) = -1/2
               7k+π=2nπ+7π6\Rightarrow -7k + \pi = 2n\pi + \dfrac {7\pi}{6}  or   2nπ+11π62n\pi + \dfrac {11\pi}{6}
    here    7k+π=2nπ+11π6\Rightarrow -7k + \pi = 2n\pi + \dfrac {11\pi}{6}
    (because at t = 0, velocity is positive)
     7 (2πλ)=2nπ+5π6\Rightarrow  -7 \left ( \dfrac {2\pi}{\lambda} \right ) = 2n\pi + \dfrac {5\pi}{6}
    λ=14π5π/6+2nπ\Rightarrow \lambda = \dfrac {-14\pi}{5\pi/6 + 2n\pi}
    λ=8412n+5\Rightarrow \lambda = \dfrac {-84}{12n + 5}
    for   n=1,λ=12cmn = -1, \lambda = 12 \,cm
    for   n=2,λ=8419cmn = -2, \lambda = \dfrac {84}{19}cm (not possible)
    because λ>7cm\lambda > 7 \,cm
    v=fλ=100×12100=12m/sv = f\lambda = 100 \times \dfrac {12}{100} = 12 \,m/s
  • Question 7
    1 / -0
    Two separated sources emit sinusoidal travelling waves but have the same wavelength λ \lambda  and are in phase at their respective sources. One travels a distance  l1 l_{1}  to get to the observation point while the other travels a distance  l2 l_{2} . The amplitude is minimum at the observation point, if  l1l2 l_{1}-l_{2}  is an
    Solution

  • Question 8
    1 / -0
    Two vibration strings of the same material but lengths L and 2L have radii 2r and r, respectively. The are stretched  under the same tension. Both the strings vibrate in their fundamental modes, the one of length L with frequency n1n_1 and the other with frequency n2n_2. The ratio n1/n2n_1/n_2 is given by 
    Solution
    n1=12l[T4πr2ρ]n_{1}=\frac{1}{2l}\sqrt{\left [ \frac{T}{4\pi r^{2}\rho } \right ]}

    and n2=14l[Tπr2ρ]n_{2}=\frac{1}{4l}\sqrt{\left [ \frac{T}{\pi r^{2}\rho } \right ]}

    n1n2=2×12=1\therefore \frac{n_{1}}{n_{2}}=2\times \frac{1}{2}=1
  • Question 9
    1 / -0
    Figure 5.55 shows a student setting up wave on a long stretched string. The student's hand makes one complete up and down movement in 0.4s0.4 \,s and in each up and down movement the hand moves by a height of 0.3m.0.3 \,m. The wavelength of the waves on the string is 0.8m.0.8 \,m.
    The amplitude of the wave is

    Solution
    Frequency=1TimePeriod=10.4=2.5HzFrequency = \dfrac {1}{Time \,Period} = \dfrac {1}{0.4} = 2.5 \,Hz
    Amplitude=12×0.3m=0.15mAmplitude = \dfrac {1}{2} \times 0.3 \,m = 0.15 \,m

  • Question 10
    1 / -0
    Four pieces of string each of length L are joined end to end to make a long string of length 4L.4L. The linear mass density of the strings are μ,4μ,9μ\mu, 4\mu, 9\mu and 16μ,16\mu, respectively. One end of the combined string is tied to a fixed support and a transverse wave has been generated at the other end having frequency ff (ignore any reflection and absorptions). String has been stretched under a tension F.F.
    Find the ratio of wavelengths of the waves on four strings, starting from right hand side.

    Solution
    Frequency of wave is same on all the four strings. So,
                   λ1=v1f,\lambda_1 = \dfrac {v_1}{f},                 λ2=v2f,\lambda_2 = \dfrac {v_2}{f},
                    λ3=v3f,\lambda_3 = \dfrac {v_3}{f},                λ4=v4f,\lambda_4 = \dfrac {v_4}{f},
    λ4:λ3:λ2:λ1=14:13:12:1=3:4:6:12\lambda_4 : \lambda_3 : \lambda_2 : \lambda_1 = \dfrac {1}{4} : \dfrac {1}{3} : \dfrac {1}{2} : 1 = 3 : 4 : 6 : 12
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