
As shown in the figure water squirts horizontally out of two small holes in the side of the cylinder and the two streams strike the ground at the same point. If hole Q is at height ‘h’ above ground and level of water stands to a height H, then the height of p above the ground level is.

A) 2h
B) H/h
C) (H-h)
D) None
Answer
220.8k+ views
Hint: Here we have to apply the concept of conservation of energy. The net external energy applied to the system is conserved. So, by this relation the potential energy and the kinetic energy of the system is equal and also the range of squirting water of the two holes are at the same place (Range is equal). Apply the formula of kinematics and conservation of energy (P.E + K.E) and solve.
Complete step by step solution:
Apply conservation of energy
$mg{h_2} = \dfrac{1}{2}m{v_1}^2$ ;
The mass are same so it will cancel out each other,
$g{h_2} = \dfrac{1}{2}{v_1}^2$;
Simplify the above equation
$g{h_2} \times 2 = {v_1}^2$;
${v_1} = {\sqrt {2gh} _2}$;
For hole P
$mg(H - h) = \dfrac{1}{2}m{v_2}^2$;
$g(H - h) = \dfrac{1}{2}{v_2}^2$;
$2g(H - h) = {v_2}^2$;
${v_2} = \sqrt {2g(H - h)} $;
Step 2:
Find out the time taken to reach the surface at the same place for both the holes.
Apply equations of kinematics:
$S = ut + \dfrac{1}{2}a{t^2}$ ;
No initial vertical velocity:
$S = \dfrac{1}{2}g{t^2}$;
For hole P, assume the distance to be${h_2}$.
\[(H - {h_2}) = \dfrac{1}{2}g{t_1}^2\];
$2(H - {h_2}) = g{t_1}^2$;
\[\dfrac{{2(H - {h_2})}}{g} = {t_1}^2\];
\[{t_1} = \sqrt {\dfrac{{2(H - {h_2})}}{g}} \];
For hole Q,
$S = ut + \dfrac{1}{2}a{t^2}$;
Here also the initial velocity is zero:
$S = \dfrac{1}{2}g{t_2}^2$;
$h = \dfrac{1}{2}g{t_2}^2$;
$\dfrac{{2h}}{g} = {t_2}^2$;
${t_2} = \sqrt {\dfrac{{2h}}{g}} $;
Step 3: Here the range of the holes are the same ${R_1} = {R_2}$
$R = vt + \dfrac{1}{2}a{t^2}$.
Here there is no horizontal acceleration so a = 0.
The equation becomes
$R = vt$;
${R_1} = {R_2}$;
${v_1}{t_1} = {v_2}{t_2}$;
Put the values in the above equation:
$\sqrt {2g{h_2}} \times \sqrt {\dfrac{{2(H - {h_2})}}{g}} = \sqrt {2g(H - h)} \times \sqrt {\dfrac{{2h}}{g}} $;
Solve the above equation:
$2g{h_2} \times \dfrac{{2(H - {h_2})}}{g} = 2g(H - h) \times \dfrac{{2h}}{g}$;
Simplify
$2{h_2} \times 2(H - {h_2}) = 2(H - h) \times 2h$;
Simplify it further,
$\Rightarrow {h_2} \times (H - {h_2}) = (H - h) \times h$;
$\Rightarrow (H{h_2} - {h_2}^2) = (Hh - {h^2})$;
$\Rightarrow (H{h_2} - {h_2}^2 - Hh + {h^2}) = 0$;
$\Rightarrow (H{h_2} - Hh) + ( - {h^2} + {h_2}^2) = 0$;
$\Rightarrow H({h_2} - h) + ( - {h^2} + {h_2}^2) = 0$;
Solving the above equation we get,
$\Rightarrow {h_2} = (H - h)$
Option (C) is correct. The height of p above the ground level is $(H - h)$.
Note: Here we have to find out the velocity as well as time taken and then equate the two values together as the distance i.e. the range of the two holes squirting the water is equal. After equating there would be a relation of height H and h.
Complete step by step solution:
Apply conservation of energy
$mg{h_2} = \dfrac{1}{2}m{v_1}^2$ ;
The mass are same so it will cancel out each other,
$g{h_2} = \dfrac{1}{2}{v_1}^2$;
Simplify the above equation
$g{h_2} \times 2 = {v_1}^2$;
${v_1} = {\sqrt {2gh} _2}$;
For hole P
$mg(H - h) = \dfrac{1}{2}m{v_2}^2$;
$g(H - h) = \dfrac{1}{2}{v_2}^2$;
$2g(H - h) = {v_2}^2$;
${v_2} = \sqrt {2g(H - h)} $;
Step 2:
Find out the time taken to reach the surface at the same place for both the holes.
Apply equations of kinematics:
$S = ut + \dfrac{1}{2}a{t^2}$ ;
No initial vertical velocity:
$S = \dfrac{1}{2}g{t^2}$;
For hole P, assume the distance to be${h_2}$.
\[(H - {h_2}) = \dfrac{1}{2}g{t_1}^2\];
$2(H - {h_2}) = g{t_1}^2$;
\[\dfrac{{2(H - {h_2})}}{g} = {t_1}^2\];
\[{t_1} = \sqrt {\dfrac{{2(H - {h_2})}}{g}} \];
For hole Q,
$S = ut + \dfrac{1}{2}a{t^2}$;
Here also the initial velocity is zero:
$S = \dfrac{1}{2}g{t_2}^2$;
$h = \dfrac{1}{2}g{t_2}^2$;
$\dfrac{{2h}}{g} = {t_2}^2$;
${t_2} = \sqrt {\dfrac{{2h}}{g}} $;
Step 3: Here the range of the holes are the same ${R_1} = {R_2}$
$R = vt + \dfrac{1}{2}a{t^2}$.
Here there is no horizontal acceleration so a = 0.
The equation becomes
$R = vt$;
${R_1} = {R_2}$;
${v_1}{t_1} = {v_2}{t_2}$;
Put the values in the above equation:
$\sqrt {2g{h_2}} \times \sqrt {\dfrac{{2(H - {h_2})}}{g}} = \sqrt {2g(H - h)} \times \sqrt {\dfrac{{2h}}{g}} $;
Solve the above equation:
$2g{h_2} \times \dfrac{{2(H - {h_2})}}{g} = 2g(H - h) \times \dfrac{{2h}}{g}$;
Simplify
$2{h_2} \times 2(H - {h_2}) = 2(H - h) \times 2h$;
Simplify it further,
$\Rightarrow {h_2} \times (H - {h_2}) = (H - h) \times h$;
$\Rightarrow (H{h_2} - {h_2}^2) = (Hh - {h^2})$;
$\Rightarrow (H{h_2} - {h_2}^2 - Hh + {h^2}) = 0$;
$\Rightarrow (H{h_2} - Hh) + ( - {h^2} + {h_2}^2) = 0$;
$\Rightarrow H({h_2} - h) + ( - {h^2} + {h_2}^2) = 0$;
Solving the above equation we get,
$\Rightarrow {h_2} = (H - h)$
Option (C) is correct. The height of p above the ground level is $(H - h)$.
Note: Here we have to find out the velocity as well as time taken and then equate the two values together as the distance i.e. the range of the two holes squirting the water is equal. After equating there would be a relation of height H and h.
Recently Updated Pages
Two discs which are rotating about their respective class 11 physics JEE_Main

A ladder rests against a frictionless vertical wall class 11 physics JEE_Main

Two simple pendulums of lengths 1 m and 16 m respectively class 11 physics JEE_Main

The slopes of isothermal and adiabatic curves are related class 11 physics JEE_Main

A trolly falling freely on an inclined plane as shown class 11 physics JEE_Main

The masses M1 and M2M2 M1 are released from rest Using class 11 physics JEE_Main

Trending doubts
JEE Main 2026: Application Form Open, Exam Dates, Syllabus, Eligibility & Question Papers

Derivation of Equation of Trajectory Explained for Students

Hybridisation in Chemistry – Concept, Types & Applications

Understanding the Angle of Deviation in a Prism

How to Convert a Galvanometer into an Ammeter or Voltmeter

Degree of Dissociation: Meaning, Formula, Calculation & Uses

Other Pages
Thermodynamics Class 11 Physics Chapter 11 CBSE Notes - 2025-26

JEE Advanced Marks vs Ranks 2025: Understanding Category-wise Qualifying Marks and Previous Year Cut-offs

Units And Measurements Class 11 Physics Chapter 1 CBSE Notes - 2025-26

NCERT Solutions For Class 11 Physics Chapter 8 Mechanical Properties Of Solids

Motion in a Straight Line Class 11 Physics Chapter 2 CBSE Notes - 2025-26

Laws of Motion Class 11 Physics Chapter 4 CBSE Notes - 2025-26

