h = 10 \text{ cm} in a tank holding water to height H = 4 0 cm . At what distance x (in cm ) does the stream strike the floor? (Neglect air resistance).
A stream of water flows through a small hole at depth
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dude use toricelli formula for it directly. it was derived by bernuolli equation only :)
Use 2√hh'
yeah...that came from toricelli formula. :)
M ( d r o p ) g h = 2 M ( d r o p ) v 2 t h u s v = 2 2 g h 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 2 g h × t ( 1 ) − i n t h e y a x i s : y = g 2 t 2 = H − h t h u s t = g 2 ( H − h ) ( 2 ) S u b s t i t u t e ( 2 ) i n ( 1 ) : x = 2 2 g h × g 2 ( H − h ) = 2 × ( H − h ) × h = 2 × ( 4 0 − 1 0 ) × 1 0 = 3 4 . 6 4 1 c m
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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In this problem, we have to use Bernoulli's Equation and the Equation of Continuity .
Bernoulli's Equation: p 1 + ρ g h 1 + 2 1 ρ v 1 2 = p 2 + ρ g h 2 + 2 1 ρ v 2 2
Equation of Continuity: S 1 v 1 = S 2 v 2 where S v is the Flow Rate .
LHS is the case for the tank while RHS is the case for the hole in the tank.
In this problem, we have to make some assumptions:
As the surface area of the tank, S 1 is very large compare to the surface area of the hole S 2 , we assumed that v 1 ≈ 0
The pressure, p 1 and p 2 are the same as they both are in the same environment.
We take h 2 as 0 for easier calculation. Relatively, h 1 will be 1 0 c m
The density of the liquid inside the tank, ρ is the same.
By these assumption, we can get a simpler equation:
g h 1 = 2 1 v 2 2
Substitute the given information we can get
v = 1 4 cms − 1
The direction of the water coming out from the hole is horizontal, thus
s y = 2 1 g t
t = 2 . 4 7 4 s
Solve for x ,
x = v t
x = 3 4 . 6 4 cm