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JEE Advanced 2017Paper 2
Exam
JEE Advanced
Year
2017
Paper
Paper 2
Subject
Physics
Chapter
Mathematics in Physics

JEE Advanced 2017 · Paper 2 · Physics · Mathematics in Physics

A person measures the depth of a well by measuring the time...

A person measures the depth of a well by measuring the time interval between dropping a stone and receiving the sound of impact with the bottom of the well. The error in his measurement of time is \deltaT=0.01\deltaT = 0.01 seconds and he measures the depth of the well to be L = 20 meters. Take the acceleration due to gravity g=10ms−2g = 10m{s}^{- 2} and the velocity of sound is 300ms−1300m{s}^{- 1} . Then the fractional error in the measurement, \deltaLL\dfrac{\deltaL}{L} , is closest to

Options

  1. A0.2%
  2. B5%
  3. C3%
  4. D1%

Correct answer

D. 1%

Step-by-step solution

Total time taken,

T=2Lg+LcT = \sqrt{\dfrac{2L}{g}} + \dfrac{L}{c}, cc is the sound speed in air.

Now, for an error \deltaL\deltaL in L,

We have an error \deltaT\deltaT in T

So, T+\deltaT=2(L+\deltaL)g+(L+\deltaL)cT + \deltaT = \sqrt{\dfrac{2\left(L + \deltaL\right)}{g}} + \dfrac{\left(L + \deltaL\right)}{c}

=2Lg(1+\deltaLL)+Lc(1+\deltaLL)= \sqrt{\dfrac{2L}{g}\left(1 + \dfrac{\deltaL}{L}\right)} + \dfrac{L}{c}\left(1 + \dfrac{\deltaL}{L}\right)

Since, \deltaTT\dfrac{\deltaT}{T} is very small, hence

\deltaLL\dfrac{\deltaL}{L} is also small, so taking binomial approximation

T+\deltaT=2Lg(1+12\deltaLL)+Lc(1+\deltaLL)T + \deltaT = \sqrt{\dfrac{2L}{g}}\left(1 + \dfrac{1}{2}\dfrac{\deltaL}{L}\right) + \dfrac{L}{c}\left(1 + \dfrac{\deltaL}{L}\right)

⇒T+\deltaT=(2Lg)+2Lg(12\deltaLL)+(Lc)+Lc(\deltaLL)⇒ T + \deltaT = \left(\sqrt{\dfrac{2L}{g}}\right) + \sqrt{\dfrac{2L}{g}}\left(\dfrac{1}{2}\dfrac{\deltaL}{L}\right) + \left(\dfrac{L}{c}\right) + \dfrac{L}{c}\left(\dfrac{\deltaL}{L}\right)

⇒\deltaT=2Lg(12\deltaLL)+Lc(\deltaLL)⇒ \deltaT = \sqrt{\dfrac{2L}{g}}\left(\dfrac{1}{2}\dfrac{\deltaL}{L}\right) + \dfrac{L}{c}\left(\dfrac{\deltaL}{L}\right)

⇒\deltaT=[L2g+(Lc)]\deltaLL⇒ \deltaT = \left[\sqrt{\dfrac{L}{2g}} + \left(\dfrac{L}{c}\right)\right]\dfrac{\deltaL}{L}

⇒0.01=[202×10+(20300)]\deltaLL⇒ 0 . 01 = \left[\sqrt{\dfrac{20}{2 \times 10}} + \left(\dfrac{20}{300}\right)\right]\dfrac{\deltaL}{L}

⇒0.01=[1+115]\deltaLL⇒\deltaLL=0.1516⇒ 0 . 01 = \left[1 + \dfrac{1}{15}\right]\dfrac{\deltaL}{L} ⇒ \dfrac{\deltaL}{L} = \dfrac{0 . 15}{16}

%error = \left(\dfrac{\deltaL}{L}\right) \times 100%

=1516= \dfrac{15}{16}%

≈1\approx 1%

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