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Waves question

2010 · Shift 2 · Q44
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Waves question

2010 · Shift 2 · Q44

JEE AdvancedPhysicsWavesMCQ+5 / −1.25
A hollow pipe of length 0.8 m is closed at one end. At its open end a 0.5 m long uniform string is vibrating in its second harmonic and it resonates with the fundamental frequency of the pipe. If the tension in the wire is 50 N and the speed of sound is 320 ms−1, the mass of the string is
  1. A
    5 grams
  2. B
    10 grams
  3. C
    20 grams
  4. D
    40 grams
View written solutionFree

Correct answer: B

Step-by-step Solution:

  1. Find the fundamental frequency of the closed pipe. A hollow pipe closed at one end forms a standing wave with a node at the closed end and an antinode at the open end. For the fundamental frequency (first harmonic), the length of the pipe LpL_pLp​ is equal to one-quarter of the wavelength λpλ_pλp​. Lp=λp4L_p = \frac{\lambda_p}{4}Lp​=4λp​​ The frequency fpf_pfp​ is related to the speed of sound vsoundv_{sound}vsound​ and wavelength λpλ_pλp​ by vsound=fpλpv_{sound} = f_p \lambda_pvsound​=fp​λp​. Substituting λp=4Lpλ_p = 4 L_pλp​=4Lp​, we get the fundamental frequency of the closed pipe: fp=vsound4Lpf_p = \frac{v_{sound}}{4 L_p}fp​=4Lp​vsound​​ Given: Lp=0.8L_p = 0.8Lp​=0.8 m and vsound=320v_{sound} = 320vsound​=320 m/s. fp=3204×0.8=3203.2=100 Hzf_p = \frac{320}{4 \times 0.8} = \frac{320}{3.2} = 100 \text{ Hz}fp​=4×0.8320​=3.2320​=100 Hz

  2. Determine the frequency of the string. The problem states that the string resonates with the fundamental frequency of the pipe. This means the frequency of the string's vibration fsf_sfs​ is equal to the fundamental frequency of the pipe fpf_pfp​. fs=fp=100 Hzf_s = f_p = 100 \text{ Hz}fs​=fp​=100 Hz

  3. Relate the string's frequency to its properties. The string is vibrating in its second harmonic (n=2). The frequency of the n-th harmonic of a string fixed at both ends is given by: fs=n2Lsvsf_s = \frac{n}{2L_s} v_sfs​=2Ls​n​vs​ where LsL_sLs​ is the length of the string and vsv_svs​ is the speed of the wave on the string. For the second harmonic (n=2): fs=22Lsvs=vsLsf_s = \frac{2}{2L_s} v_s = \frac{v_s}{L_s}fs​=2Ls​2​vs​=Ls​vs​​ Given: fs=100f_s = 100fs​=100 Hz and Ls=0.5L_s = 0.5Ls​=0.5 m. We can find the speed of the wave on the string, vsv_svs​: 100=vs0.5100 = \frac{v_s}{0.5}100=0.5vs​​ vs=100×0.5=50 m/sv_s = 100 \times 0.5 = 50 \text{ m/s}vs​=100×0.5=50 m/s

  4. Calculate the linear mass density of the string. The speed of a wave on a string is also given by the formula: vs=Tμv_s = \sqrt{\frac{T}{\mu}}vs​=μT​​ where T is the tension in the string and μ is the linear mass density (mass per unit length). Squaring both sides: vs2=Tμv_s^2 = \frac{T}{\mu}vs2​=μT​ Rearranging to solve for μ: μ=Tvs2\mu = \frac{T}{v_s^2}μ=vs2​T​ Given: T = 50 N and we calculated vs=50v_s = 50vs​=50 m/s. μ=50502=502500=150 kg/m\mu = \frac{50}{50^2} = \frac{50}{2500} = \frac{1}{50} \text{ kg/m}μ=50250​=250050​=501​ kg/m

  5. Calculate the total mass of the string. The linear mass density μ is defined as the total mass of the string msm_sms​ divided by its length LsL_sLs​. μ=msLs\mu = \frac{m_s}{L_s}μ=Ls​ms​​ So, the mass of the string is: ms=μ×Lsm_s = \mu \times L_sms​=μ×Ls​ Substituting the values we found: ms=150 kg/m×0.5 m=0.550=1100=0.01 kgm_s = \frac{1}{50} \text{ kg/m} \times 0.5 \text{ m} = \frac{0.5}{50} = \frac{1}{100} = 0.01 \text{ kg}ms​=501​ kg/m×0.5 m=500.5​=1001​=0.01 kg

  6. Convert the mass to grams. Since the options are in grams, we convert the mass from kilograms to grams. ms=0.01 kg×1000 g1 kg=10 gm_s = 0.01 \text{ kg} \times \frac{1000 \text{ g}}{1 \text{ kg}} = 10 \text{ g}ms​=0.01 kg×1 kg1000 g​=10 g

Comparing our result with the options: (A) 5 grams (B) 10 grams (C) 20 grams (D) 40 grams

The calculated mass of the string is 10 grams, which corresponds to option B.

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