Water Column Resonance Time Interval Calculation

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SUMMARY

The discussion centers on calculating the water column resonance time interval in a cylindrical vessel with a cross-sectional area of 20 cm² and a length of 1 m. The fundamental frequency of resonance is established at 340 Hz, with the initial and final heights of the water column denoted as h1 and h2, respectively. The velocity of water exiting through a pinhole is derived from the equation \(\sqrt{2gx}\), leading to the integration of the rate of change of height over time. The final calculated time interval for resonance to occur again is approximately 307 seconds, with slight variations noted by participants.

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  • Understanding of fluid dynamics, specifically Torricelli's law
  • Knowledge of wave mechanics, particularly standing waves in closed pipes
  • Familiarity with calculus for integration and solving differential equations
  • Basic physics concepts including gravitational acceleration (g = 9.8 m/s²) and speed of sound in air (approximately 330 m/s)
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  • Learn about the properties of standing waves in closed organ pipes
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utkarshakash
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Homework Statement


There is a cylindrical vessel of cross-sectional area 20cm^2 and length 1m is initially filled with water to a certain height as shown. There is a very small pinhole of cross-sectional area 0.01cm^2 at the bottom of the cylinder which is initially plugged with a pin cork. The air column in the cylinder is resonating in fundamental mode with a tuning fork of frequency 340Hz. Suddenly the pin cork is pulled out and water starts flowing out of the cylinder. Find the time interval after which resonance occurs again.



The Attempt at a Solution


The setup is equivalent to a closed organ pipe. The fundamental frequency is given by nv/4L.
Let the initial height of water column be h1. At second resonance let the height change to h2.

h1-h2=v/4*340

The velocity of water coming out of hole is given by \sqrt{2gx}

Thus, rate of decrease of water column = 0.01v/20.

\dfrac{dx}{dt} = \dfrac{0.01\sqrt{2gx}}{20}

If I integrate this from h1 to h2, I am left with the expression \sqrt{h_1}-\sqrt{h_2}.

I already know the difference between the heights but not the difference between their square roots. How do I calculate it?
 
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utkarshakash said:
h1-h2=v/4*340

I don't think this is correct. If you haven't already done so, draw a diagram showing the nodes and antinodes of the standing sound wave for each of the two resonances.

\dfrac{dx}{dt} = \dfrac{0.01\sqrt{2gx}}{20}

This looks good except you should think about whether or not a negative sign needs to be included (x is decreasing as time increases).

If I integrate this from h1 to h2, I am left with the expression \sqrt{h_1}-\sqrt{h_2}.

I already know the difference between the heights but not the difference between their square roots. How do I calculate it?

From your diagrams of nodes and antinodes, you should be able to determine the heights h1 and h2.

By the way, what are you supposed to use for the speed of sound?
 
TSny said:
From your diagrams of nodes and antinodes, you should be able to determine the heights h1 and h2.

By the way, what are you supposed to use for the speed of sound?

Here is my attempt at the problem .

I am using g = 9.8ms-2 and speed of sound = 330 m/s

The length of air column l = nλ/4 = nv/4f , n=1,3,5...

l1 = 0.24m
l2 = 0.72m

Consequently h1 = 0.76m and h2 = 0.28m

##\dfrac{dx}{dt} = - \dfrac{0.01\sqrt{2gx}}{20}##

Integrating , t = 902.93 (√h1 - √h2)

Putting values of h1 and h2 , I am getting t ≈ 307 sec .

TSny ,are you getting the same answer ?

Many Thanks
 
That looks good. I get slightly different results for some of the numbers in your calculation. My final answer for t = 315 s ≈ 320 s to 2 significant figures.
 
Thanks a lot :smile:
 

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