The correct option is
C 7.2NSince area of a hole is very small in comparison to base area A of the cylinder, velocity of liquid inside the cylinder is negligible. Let velocity of efflux be v and atmospheric pressure be P0.
Consider two points A (inside the cylinder) and B (must outside the hole) in the same horizontal line as shown in the figure in question.
Pressure at A: PA=P0+hρ2g+(h−y)ρ1g
Pressure at A: PB=P0
Applying Bernoulli's theorem at points A and B
PA+12ρ2v22+(ρ2gh+ρ1g(h−y))=PB+12ρ1v21+(ρ2gh+ρ1g(h−y)) .....(1)
Substituting PA and PB in eqn(1) we get,
P0+hρ2g+(h−y)ρ1g+12ρ2v22+(ρ2gh+ρ1g(h−y))=P0+12ρ1v21+(ρ2gh+ρ1g(h−y)) ....(2)
Given,
A=0.5m2
a=5cm2=25×10−4m2
From continuity equation,
Av2=av1
∴v2v1=aA=25×10−40.5=50×10−4
Given h=60cm=0.6m
y=20cm=0.2m
ρ1=900kgm−3
ρ2=600kgm−3
P0+hρ2g+(h−y)ρ1g+12ρ2v22=P0+12ρ1v21
As given in the problem, we ignore v2 since a is very small.
∴P0+hρ2g+(h−y)ρ1g=P0+12ρ1v21
∴hρ2g+(h−y)ρ1g=12ρ1v21
Substituting the values, 0.6×600×10+(0.6−0.2)×900×10=12×900×v21
⇒v1=4ms−1
When the cylinder is on the smooth horizontal plane, force F required to keep the cylinder stationary equals horizontal thrust exerted by fluid jet. But that is equal to mass flowing per second change in velocity of this mass.
∴avρ1(v−0)=av2ρ1=5×10−442×900=7.2N