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JEE Advanced 2021 Paper 2 · Physics · Fluid Mechanics, Elasticity and Surface Tension · medium

JEE Advanced 2021 Paper 2 Physics: Paragraph 2

A wide cylindrical tank of cross-sectional area 0.50 m20.50\ \mathrm{m^2} stands upright and has a small circular hole of area 2.0 cm22.0\ \mathrm{cm^2} in its bottom. A tap supplies water at a constant rate of 4.0×10−4 m3 s−14.0\times10^{-4}\ \mathrm{m^3\,s^{-1}}. Water leaves the hole as an ideal jet (Torricelli's law, no contraction of the jet) and the water level is always well above the hole. Take g=10 m s−2g=10\ \mathrm{m\,s^{-2}} and treat the speed of the water surface as negligible compared with the exit speed whenever Bernoulli's equation is applied.

Question 1

Numerical answer

Find the steady height (in m\mathrm{m}) of the water level above the hole when the tap is on and the level no longer changes. Give the answer correct to two decimal places.
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Answer: 0.20

In steady state inflow equals outflow, so Q=a2ghQ=a\sqrt{2gh} by Torricelli's law. Squaring, h=Q22g a2h=\dfrac{Q^2}{2g\,a^2}. With Q=4.0×10−4 m3 s−1Q=4.0\times10^{-4}\ \mathrm{m^3\,s^{-1}}, a=2.0×10−4 m2a=2.0\times10^{-4}\ \mathrm{m^2} and g=10g=10, h=16×10−82×10×4×10−8=1680=0.20 mh=\dfrac{16\times10^{-8}}{2\times10\times4\times10^{-8}}=\dfrac{16}{80}=0.20\ \mathrm{m}. The tank area does not appear because the level is stationary. The exit speed is then 2gh=2 m s−1\sqrt{2gh}=2\ \mathrm{m\,s^{-1}}, and a×2=4×10−4 m3 s−1a\times2=4\times10^{-4}\ \mathrm{m^3\,s^{-1}} equals the inflow, confirming the result. This steady level is stable, because a higher level gives a larger outflow and a lower level a smaller outflow. Therefore the answer is 0.200.20 metres above the hole, a small value compared with the initial filling height used in the next part, so the level would otherwise keep falling towards it.

Question 2

Numerical answer

The tank is now filled to a height of 1.8 m1.8\ \mathrm{m}, the tap is closed, and the water drains through the hole. Find the time (in seconds) taken for the level to fall to 0.20 m0.20\ \mathrm{m}. Give the answer correct to two decimal places.
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Answer: 1000

With the tap closed, volume conservation gives −Adhdt=a2gh-A\dfrac{dh}{dt}=a\sqrt{2gh}. Separating variables, t=Aa2g∫h2h1dhh=2Aa2g(h1−h2)=Aa2g(h1−h2)\displaystyle t=\dfrac{A}{a\sqrt{2g}}\int_{h_2}^{h_1}\dfrac{dh}{\sqrt h}=\dfrac{2A}{a\sqrt{2g}}\left(\sqrt{h_1}-\sqrt{h_2}\right)=\dfrac{A}{a}\sqrt{\dfrac2g}\left(\sqrt{h_1}-\sqrt{h_2}\right). Here A/a=0.50/(2.0×10−4)=2500A/a=0.50/(2.0\times10^{-4})=2500 and 2/g=0.4472\sqrt{2/g}=0.4472. Also 1.8−0.2=1.3416−0.4472=0.8944\sqrt{1.8}-\sqrt{0.2}=1.3416-0.4472=0.8944. Then t=2500×0.4472×0.8944=2500×0.4=1000 st=2500\times0.4472\times0.8944=2500\times0.4=1000\ \mathrm{s}. The product 0.4472×0.89440.4472\times0.8944 equals exactly 0.40.4, so the time is exactly 10001000 s, about 16.716.7 minutes. Treating the surface speed as zero is justified because a/A=4×10−4a/A=4\times10^{-4}. The same result follows by noting that the surface speed is v=2gh (a/A)v=\sqrt{2gh}\,(a/A), so hh falls with a time dependence h=h1−aAg2 t\sqrt h=\sqrt{h_1}-\frac{a}{A}\sqrt{\frac g2}\,t, which is linear in time for the square root of height; setting h=0.2\sqrt h=\sqrt{0.2} gives the same tt.
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