Leaky Water Tank

A stream of water flows through a small hole at depth h = 10 \text{ cm} in a tank holding water to height H = 40 cm H =40 \text{ cm} . At what distance x x (in cm \text{ cm} ) does the stream strike the floor? (Neglect air resistance).


The answer is 34.64.

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3 solutions

Discussions for this problem are now closed

Christopher Boo
Feb 27, 2014

In this problem, we have to use Bernoulli's Equation and the Equation of Continuity .

Bernoulli's Equation: p 1 + ρ g h 1 + 1 2 ρ v 1 2 = p 2 + ρ g h 2 + 1 2 ρ v 2 2 p_1+\rho gh_1+\frac{1}{2}\rho{v_1}^2=p_2+\rho gh_2+\frac{1}{2}\rho{v_2}^2

Equation of Continuity: S 1 v 1 = S 2 v 2 S_1 v_1=S_2 v_2 where S v Sv is the Flow Rate .

LHS \text{LHS} is the case for the tank while RHS \text{RHS} is the case for the hole in the tank.

In this problem, we have to make some assumptions:

  1. As the surface area of the tank, S 1 S_1 is very large compare to the surface area of the hole S 2 S_2 , we assumed that v 1 0 v_1\approx0

  2. The pressure, p 1 p_1 and p 2 p_2 are the same as they both are in the same environment.

  3. We take h 2 h_2 as 0 0 for easier calculation. Relatively, h 1 h_1 will be 10 c m 10cm

  4. The density of the liquid inside the tank, ρ \rho is the same.

By these assumption, we can get a simpler equation:

g h 1 = 1 2 v 2 2 gh_1=\frac{1}{2}{v_2}^2

Substitute the given information we can get

v = 14 cms 1 v=14\text{ cms}^{-1}

The direction of the water coming out from the hole is horizontal, thus

s y = 1 2 g t s_y=\frac{1}{2}gt

t = 2.474 s t=2.474\text{ s}

Solve for x x ,

x = v t x=vt

x = 34.64 cm x=34.64\text{ cm}

dude use toricelli formula for it directly. it was derived by bernuolli equation only :)

Akash Omble - 7 years, 3 months ago

Use 2√hh'

Siddharth singh Rajawat - 7 years, 2 months ago

yeah...that came from toricelli formula. :)

Vaibhav Bhasin - 7 years, 2 months ago
Ramón Gondim
Mar 10, 2014

M ( d r o p ) g h = M ( d r o p ) v 2 2 t h u s v = 2 g h 2 t o c a l c u l a t e v , l e t s u s e c i n e m a t i c s : i n t h e x a x i s w e h a v e : x = v × t x = 2 g h 2 × t ( 1 ) i n t h e y a x i s : y = g t 2 2 = H h t h u s t = 2 ( H h ) g ( 2 ) S u b s t i t u t e ( 2 ) i n ( 1 ) : x = 2 g h 2 × 2 ( H h ) g = 2 × ( H h ) × h = 2 × ( 40 10 ) × 10 = 34.641 c m M(drop)gh\quad =\quad \frac{ M{ (drop)v }^{ 2 } }{ 2 } \quad thus\quad v\quad =\quad \sqrt [ 2 ]{ 2gh } \\ to\quad calculate\quad v,\quad lets\quad use\quad cinematics:\\ -\quad in\quad the\quad x\quad axis\quad we\quad have:\\ \quad x=\quad v\quad \times \quad t\quad \rightarrow \quad x\quad =\quad \sqrt [ 2 ]{ 2gh } \times \quad t\quad (1)\\ -\quad in\quad the\quad y\quad axis:\\ y=\quad g\frac { { t }^{ 2 } }{ 2 } \quad =\quad H-h\quad thus\quad t\quad =\sqrt { \frac { 2(H-h) }{ g } } \quad (2)\\ Substitute\quad (2)\quad in\quad (1):\\ x=\quad \sqrt [ 2 ]{ 2gh } \times \sqrt { \frac { 2(H-h) }{ g } } =\quad 2\times \sqrt { (H-h)\times h } \\ =\quad 2\times \sqrt { (40-10)\times 10 } =34.641\quad cm

Ajit Athle
May 18, 2014

For a water particle coming out with a velocity of u cm/sec, we may write: mgh = (1/2) mu² or u² = 2gh =20g since h=10 cm General eqn. of parabolic motion: y =xtan(θ) – gx²/(2u²cos²(θ)) where y = -30, θ = 0 so that – 30 = x²/(2*20) or x² =1200 or x~34.641 cm

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