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Question #42083

Difficulty: 8/10 | 🟢 Free

The Question

A large closed tank contains a liquid of density ρ\rho. The liquid level is at a height HH above a small hole in the side of the tank. The gas above the liquid is maintained at a constant gauge pressure P0P_0. A spherical droplet of radius rr and density ρ\rho emerges horizontally from the hole into the surrounding air. The droplet experiences a viscous drag force F⃗d=−6πηrv⃗\vec{F}_d = -6\pi\eta r \vec{v}, where η\eta is the viscosity of air and v⃗\vec{v} is the droplet's velocity vector. Neglecting the buoyant force from the air, what is the horizontal displacement xx of the droplet at the exact instant its downward vertical velocity reaches vyv_y? (Assume acceleration due to gravity is gg).

Options

  • A.

    vyg2gH+2P0ρ\frac{v_y}{g} \sqrt{2gH + \frac{2P_0}{\rho}}

  • B.

    2r2ρ9η2gH+2P0ρ\frac{2r^2\rho}{9\eta} \sqrt{2gH + \frac{2P_0}{\rho}}

  • C.

    vyg2gH\frac{v_y}{g} \sqrt{2gH}

  • D.

    2r2ρ9ηvy\frac{2r^2\rho}{9\eta} v_y

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

Projectile on Inclined Plane|Torricelli’s Efflux Velocity|Viscosity and Stokes' Law

Why This Question Is Tricky

Common Mistakes

This question tests the transition from fluid dynamics (Torricelli's law with gauge pressure) to kinematics under non-conservative, velocity-dependent forces (Stokes' drag).

The primary trap lies in the assumption that the presence of a complex drag force (F=−6πηrvF = -6\pi\eta r v) must explicitly manifest in the final kinematic relationship between xx and vyv_y.

Students often get bogged down attempting to solve the coupled non-linear differential equations or incorrectly apply conservation of energy.

By isolating the time-dependent exponential decay factor in both orthogonal directions, the drag coefficient and mass elegantly cancel out, revealing a purely kinematic geometric constraint independent of the fluid's viscosity or the droplet's radius.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMotion in a Plane - Class 11 Part 1
ConceptProjectile on Inclined Plane
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree