© examsnet.com
Question : 24 of 27
Marks: +1, -0
One end of a long string of linear mass density 8.0×103kgm18.0 \times 10^{-3} \, \mathrm{kg} \, \mathrm{m}^{-1} is connected to an electrically driven tuning fork of frequency 256 Hz. The other end passes over a pulley and is tied to a pan containing a mass of 90 kg. The pulley end absorbs all the incoming energy so that reflected waves at this end have negligible amplitude. At t=0t = 0, the left end (fork end) of the string x=0x = 0 has zero transverse displacement (y=0)(y = 0) and is moving along positive y-direction. The amplitude of the wave is 5.0 cm. Write down the transverse displacement y as function of xx and tt that describes the wave on the string.
Solution:  
Here, m=8.0×103kgm1m = 8.0 \times 10^{-3} \, \mathrm{kg} \, \mathrm{m}^{-1}, υ=256\upsilon = 256 Hz,
T = 90 kg = 90×9.890 \times 9.8 = 882 N
Amplitude of wave, A = 5.0 cm = 0.05 m.
As, the wave propagating along the string is a transverse travelling wave, the velocity of the wave is given by
v=Tμ=8828.0×103v = \sqrt{ \frac{T}{\mu} } = \sqrt{ \frac{882}{8.0 \times 10^{-3}} } =3.32×102ms1= 3.32 \times 10^{2} \, \mathrm{m} \, \mathrm{s}^{-1}
ω=2πυ=2×227×256\omega = 2 \pi \upsilon = 2 \times \frac{22}{7} \times 256 =1.61×103rads1= 1.61 \times 10^{3} \, \mathrm{rad} \, \mathrm{s}^{-1}
λ=vυ=3.32×102256m\lambda = \frac{v}{\upsilon} = \frac{3.32 \times 10^{2}}{256} \, \mathrm{m}
Propagation constant,
k=2πλ=2×3.142×2563.32×102=4.84radm1k = \frac{2 \pi}{\lambda} = \frac{2 \times 3.142 \times 256}{3.32 \times 10^{2}} = 4.84 \, \mathrm{rad} \, \mathrm{m}^{-1}
As, the wave is propagating along positive x direction, the equation of the wave is
y(x,t)=Asin(ωtkx)y(x, t) = A \sin (\omega t - k x)
=0.05sin(1.61×103t4.84x)= 0.05 \sin (1.61 \times 10^{3} t - 4.84 x)
Here, x, y are in metre and t is in second.
© examsnet.com
Go to Question: