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Question: A tank, which is open at the top, contains a liquid up to a height \(H\) . A small hole is made in t...

A tank, which is open at the top, contains a liquid up to a height HH . A small hole is made in the side of a tank at a distance yy below the liquid surface. The liquid emerging from the hole lands at a distance xx from the tank.

(a)\left( a \right) If yy is increased from zero toHH . xx will first increase and then decrease.
(b)\left( b \right) xx is maximum for y=H2y = \dfrac{H}{2} .
(c)\left( c \right) The maximum value of xx isHH .
(d)\left( d \right) The maximum value of xx will depend on the density of the liquid.

Explanation

Solution

We are given with the level markings on the tank and are asked to find the change in basically the value xx as yy changes. Thus, we will take into account the efflux velocity of the liquid flowing out. Then, we will differentiate it with respect to the targeted variable.
Formulae Used:
v=2gyv = \sqrt {2gy}
Where, vv is the efflux velocity, gg is the acceleration due to gravity and yy is the reduced height of the liquid.

Complete Step by Step Solution:
Here,
The liquid coming out of the opening is a parabola.
Clearly,
The emerging liquid moves upwards as the projectile reaches the ground after time tt .
Thus,
We have
Hy=12gt2\Rightarrow H - y = \dfrac{1}{2}g{t^2}
Thus,
Targeting the time and rearranging the equation, we get
t=2(Hy)g\Rightarrow t = \sqrt {\dfrac{{2(H - y)}}{g}}
Thus,
We can say,
x=vtx = vt
Substituting the values, we get
x=2gy×2(Hy)g\Rightarrow x = \sqrt {2gy} \times \sqrt {\dfrac{{2(H - y)}}{g}}
Further, we can say
x=2(Hy)y\Rightarrow x = 2\sqrt {(H - y)y}
Now,
Differentiating both sides with respect to yy , we get
dxdy=(H2y)(Hy)y\Rightarrow \dfrac{{dx}}{{dy}} = \dfrac{{(H - 2y)}}{{\sqrt {(H - y)y} }}
Now,
Clearly,
dxdy>0\Rightarrow \dfrac{{dx}}{{dy}} > 0 If y<H2y < \dfrac{H}{2}
And,
dxdy<0\Rightarrow \dfrac{{dx}}{{dy}} < 0 If y>H2y > \dfrac{H}{2}
Thus, option (a)\left( a \right) is correct.
Also,
For maxima or minima,
dxdy=0\Rightarrow \dfrac{{dx}}{{dy}} = 0
Thus, we can say
H2y=0\Rightarrow H - 2y = 0
That means,
y=H2\Rightarrow y = \dfrac{H}{2}
Hence, the option (b)\left( b \right) is also correct.
Now,
The maximum value of xx is at y=H2y = \dfrac{H}{2}.
Thus,
xmax=2(HH2)×H2\Rightarrow {x_{\max }} = 2\sqrt {(H - \dfrac{H}{2}) \times \dfrac{H}{2}}
Thus, we get
xmax=H\Rightarrow {x_{\max }} = H
Hence, the option (c)\left( c \right) is also correct.
Now,

Option (d)\left( d \right) is clearly incorrect as the efflux itself is independent of the density of the liquid. Thus, it is not possible to have xx depending on the density of the liquid.

Note: As we have seen here, a question can have more than one correct answer. So, it is better to go through a generalized methodology to solve a problem otherwise we might end up overlooking the multiple correct possibility. We can also make a habit of cross checking all the given options before we finalize.