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A container of large uniform cross secti...

A container of large uniform cross sectional area A resting on a horizontal surface holds two immiscible non-viscous and incompressible liquids of density d and 3d each of height H/2. The lower density liquid is open to the atmosphere having pressure `P_o`. A tiny hole of area a `(a lt lt A)` is punched on the vertical side of the lower container at a height `h (0 lt h lt H/2)` for which range is maximum.

A

h=H/3

B

Range R=2H/3

C

Range R=3H/2

D

velocity of efflux r `v=sqrt(2/3 gH)`

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To solve the problem, we need to find the height \( h \) at which the hole is punched in the lower liquid so that the range of the liquid that exits the hole is maximized. ### Step-by-Step Solution: 1. **Understanding the Setup**: - We have two immiscible liquids in a container. The lower liquid has density \( d \) and the upper liquid has density \( 3d \). - Both liquids have a height of \( \frac{H}{2} \). - The lower liquid is open to the atmosphere at pressure \( P_0 \). ...
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Fluids at rest exert a normal force to the walls of the container or to the sruface of the body immersed in the fluid. The pressure exerted by this force at a point inside the liqid is the sum of atmospheric pressure and a factor which depends on the density of the liquid, the acceleration due to gravity and the height of the liquid, above that point. The upthrust acting on a body immersed in a stationary liquid is the net force acting on the body in the upward direction. A number of phenomenon of liquids in motion can be explain by Bernoulli's theorem which relates the pressure, flow speed and height for flow of an ideal incompressible fluid. A container of large uniform cross sectional area. A resting on a horizontal surface holds two immiscible, non viscous and incompressile liquids of densities d and 2d , each of height H//2 as shown in the figure. The lower density liquid is open to the atmosphere having pressure P_(0) . Situation II: A cyliner is removed and the original arrangement is restored.A tiny hole of area s(slt ltA) is punched on the veritical sideof the containier at a height h(hltH//2) The initial speed of efflux of the liquid at the hole is

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A container of large uniform cross-sectional area A resting on a horizontal surface, holes two immiscible, non-viscon and incompressible liquids of densities d and 2d each of height H//2 as shown in the figure. The lower density liquid is open to the atmosphere having pressure P_(0) . A homogeneous solid cylinder of length L(LltH//2) and cross-sectional area A//5 is immeresed such that it floats with its axis vertical at the liquid-liquid interface with length L//4 in the denser liquid, The cylinder is then removed and the original arrangement is restroed. a tiny hole of area s(sltltA) is punched on the vertical side of the container at a height h(hltH//2) . As a result of this, liquid starts flowing out of the hole with a range x on the horizontal surface. The initial speed of efflux without cylinder is

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