Terminal Velocity

8 MCQs2 revision cards9-step worked example
Source: NCERT Properties of Bulk MatterPYQ coverage: NEET 2020, 2021, 2022, 2023, 2024, 2025Official key: NTA-verifiedLast reviewed: May 2026

Lesson

A sphere dropped into a viscous liquid does not accelerate forever. As it speeds up, the viscous drag force (Stokes' law: F = 6πηrv) grows until it, together with buoyancy, exactly balances the gravitational pull. From that instant onward, the net force is zero and the sphere falls at a constant speed called terminal velocity.

The expression follows directly from setting weight equal to buoyancy plus drag:

v_t = (2r²g(ρ_s − ρ_f)) / (9η)

where r is the sphere radius, ρ_s and ρ_f are the densities of the sphere and fluid, η is the fluid viscosity, and g is the acceleration due to gravity (NCERT Class 11 Physics, Chapter 10 — Mechanical Properties of Fluids, page 10).

The high-frequency trap in this topic: treating terminal velocity as proportional to r (linear) instead of r². Stokes' drag is proportional to r·v, but gravitational minus buoyant force is proportional to r³ (volume). When you balance them, v_t comes out proportional to r². Doubling the radius quadruples the terminal velocity — not doubles it.

Shape of the v–t curve. The sphere starts from rest with maximum acceleration (g_eff). As v increases, drag increases, so acceleration decreases continuously. The curve is concave-down, asymptotically approaching v_t. It is NOT a straight line followed by a flat line — there is no sharp kink.

Watch-out for negative (ρ_s − ρ_f). If the sphere is less dense than the fluid, the "terminal velocity" is upward (the sphere rises). The formula still applies; the direction reverses.


Practice MCQs

Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.

MCQ 1Easy RecallPractice

At terminal velocity, the net force on a sphere falling through a viscous fluid is:

MCQ 2Easy RecallPractice

The SI unit of coefficient of viscosity (η) is:

MCQ 3Easy RecallPractice

Stokes' law for viscous drag on a sphere is valid when:

MCQ 4Direct ApplicationPractice

A metal sphere of radius r falls through a viscous liquid and reaches terminal velocity v_t. A second sphere of the same material and density but radius 2r falls through the same liquid. Its terminal velocity is:

MCQ 5Direct ApplicationPractice

Two identical spheres fall through two different viscous liquids. Liquid A has viscosity η and liquid B has viscosity 3η. Both liquids have the same density. The ratio of terminal velocities v_A : v_B is:

MCQ 6Direct ApplicationPractice

A sphere of density 2.5 × 10³ kg/m³ falls through a liquid of density 1.5 × 10³ kg/m³. If the liquid density were changed to 2.0 × 10³ kg/m³ (same viscosity, same sphere), the terminal velocity would become:

MCQ 7Concept TrapPractice

A sphere is released from rest in a viscous liquid. Which of the following best describes the velocity–time graph?

MCQ 8CalculationPractice

A sphere of radius 1.0 × 10⁻³ m and density 8.0 × 10³ kg/m³ falls through oil of density 1.0 × 10³ kg/m³ and viscosity 9.8 Pa·s. Taking g = 9.8 m/s² (exact for this problem), the terminal velocity is approximately:

Quick recall before you leave

Worked Example

Pattern: Terminal velocity scaling (based on PYQ pattern NEET pattern: terminal velocity scaling — observed in NEET 2021, 2022)

  1. 1

    Given

    A steel ball of radius r₁ = 2.0 × 10⁻³ m reaches terminal velocity v₁ = 4.0 × 10⁻² m/s in a viscous liquid. A second steel ball of radius r₂ = 4.0 × 10⁻³ m is dropped into the same liquid.

  2. 2

    Required

    Terminal velocity v₂ of the second ball.

  3. 3

    Concept

    Terminal velocity is proportional to r² (from v_t = (2r²g(ρ_s − ρ_f))/(9η)). When the material (ρ_s), fluid (ρ_f, η), and g are all the same, the ratio v₂/v₁ = (r₂/r₁)².

  4. 4

    Formula

    v₂ = v₁ × (r₂/r₁)²

  5. 5

    Substitution

    v₂ = 4.0 × 10⁻² × (4.0 × 10⁻³ / 2.0 × 10⁻³)²

  6. 6

    Calculation

    r₂/r₁ = 2.0 (exact ratio — both radii are given to 2 significant figures, and the ratio is a counting number) (r₂/r₁)² = 4.0 v₂ = 4.0 × 10⁻² × 4.0 = 16 × 10⁻² = 1.6 × 10⁻¹ m/s

  7. 7

    Final answer

    v₂ = 1.6 × 10⁻¹ m/s (= 0.16 m/s), reported to 2 significant figures matching the given data. The ratio 2.0 is exact (problem-defined integer ratio) and does not limit significant figures.

  8. 8

    Common trap

    Treating v_t as proportional to r (linear) gives v₂ = 2 × 4.0 × 10⁻² = 8.0 × 10⁻² m/s — exactly half the correct answer. This is the most common wrong-option pattern for terminal velocity scaling questions.

  9. 9

    Similar NEET-style question

    A raindrop of radius R falls at terminal velocity V through air. If a second raindrop has radius 3R (same density, same air conditions), what is its terminal velocity? *Answer: v_t ∝ r², so the new terminal velocity = V × (3R/R)² = 9V.* ---

Before solving, remember these

Sphere falling through viscous fluid reaches terminal velocity when net force = 0: v_t = (2/9) r² g (ρ_s - ρ_f) / η, where ρ_s, ρ_f are sphere and fluid densities.

-- NCERT, p. 10

Formulas

12 formulas — click to collapse

Bernoulli's equation

Conservation of energy along a streamline of incompressible non-viscous flow.

SymbolQuantitySI Unit
PpressurePa
rhodensitykg/m^3
vspeedm/s
ggravitym/s^2
hheightm

Valid when

  • Steady, non-viscous, incompressible flow
  • Along a single streamline
  • No work added/removed

Bulk modulus

Resistance of a material to uniform compression. Inverse: compressibility.

SymbolQuantitySI Unit
Kbulk modulusPa
Vvolumem^3
PpressurePa

Valid when

  • Isotropic compression
  • Within elastic regime

Capillary rise/depression

Height a liquid rises (or falls) in a capillary tube. cos(theta) > 0: rises (wetting); < 0: depresses.

SymbolQuantitySI Unit
hcapillary heightm
Tsurface tensionN/m
thetacontact anglerad
rhodensitykg/m^3
rtube radiusm

Valid when

  • Narrow tube (capillary regime)
  • Constant theta

Pressure in static fluid

Pressure at depth h below free surface of fluid of density rho.

SymbolQuantitySI Unit
Ptotal pressurePa
P0atmospheric/surface pressurePa
rhodensitykg/m^3
hdepthm

Valid when

  • Static fluid (no flow)
  • Constant g
  • Constant rho (incompressible)

Latent heat

Heat absorbed/released during phase change at constant T. L_fusion or L_vaporisation.

SymbolQuantitySI Unit
QheatJ
mmasskg
Llatent heatJ/kg

Valid when

  • Phase transition (constant T during)
  • All mass m undergoes the transition

Specific heat / heat capacity

Heat required to raise mass m by temperature Delta_T. Specific heat c is material property.

SymbolQuantitySI Unit
QheatJ
mmasskg
cspecific heatJ/kg/K
Delta_Ttemp changeK

Valid when

  • No phase change during heating
  • c approximately constant in temp range

Stefan-Boltzmann radiation law

Radiation power from a body. Black body epsilon=1; net to surroundings P = sigma*epsilon*A*(T^4 - T_s^4).

SymbolQuantitySI Unit
sigmaStefan-Boltzmann = 5.67e-8W/m^2/K^4
epsilonemissivity (0-1)-
Asurface aream^2
Tabsolute tempK

Valid when

  • Body in radiative equilibrium
  • T in kelvins

Stokes' law (viscous drag on sphere)

Drag force on a sphere of radius r moving with velocity v through viscous fluid (low Reynolds number).

SymbolQuantitySI Unit
Fdrag forceN
etaviscosityPa*s
rsphere radiusm
vvelocitym/s

Valid when

  • Smooth, slow flow (low Reynolds number)
  • Spherical body
  • Newtonian fluid

Excess pressure inside drop/bubble

Excess internal pressure due to surface tension. Bubble has 2 surfaces, hence factor 4.

SymbolQuantitySI Unit
Delta_Pexcess pressurePa
Tsurface tensionN/m
rradiusm

Valid when

  • Spherical drop or bubble
  • Constant T (one fluid pair)

Terminal velocity of sphere in viscous fluid

Constant velocity reached when net force is zero (gravity balanced by buoyancy + viscous drag).

SymbolQuantitySI Unit
v_tterminal velocitym/s
rsphere radiusm
rho_ssphere densitykg/m^3
rho_ffluid densitykg/m^3
etaviscosityPa*s

Valid when

  • Steady state (net force zero)
  • Stokes regime applicable

Thermal expansion (linear/area/volume)

Fractional change in length, area, volume per degree temperature change.

SymbolQuantitySI Unit
alphalinear coefficient1/K
betavolume coefficient1/K
Delta_Ttemperature changeK

Valid when

  • Isotropic material
  • Modest temperature range (alpha ~ constant)

Young's modulus

Ratio of longitudinal stress to longitudinal strain in a stretched wire/rod within elastic limit.

SymbolQuantitySI Unit
YYoung's modulusPa
Fapplied forceN
Across-section aream^2
Loriginal lengthm
Delta_Lextensionm

Valid when

  • Within elastic limit (Hooke's law region)
  • Uniform cross-section
  • Force along length

Exam Traps & Common Mistakes

These are the exact patterns that cause wrong answers in NEET. Each trap includes when it triggers and how to avoid it.

5 items — click to collapse

Category: Similar Terms

Student uses 2T/r for soap bubble (drop formula). Bubble has 2 surfaces → 4T/r.

When it triggers

Question mentions soap bubble OR liquid drop OR air bubble in liquid.

How to avoid

Drop in air: 1 surface → 2T/r. Soap bubble in air: 2 surfaces → 4T/r. Air bubble in liquid: 1 surface → 2T/r.

Category: Similar Terms

Student uses Y formula when problem is about volumetric compression (use K) or vice versa.

When it triggers

Problem describes longitudinal stretching (use Y), volumetric pressure (use K), or shear (use G).

How to avoid

Y: longitudinal stress/strain. K: volumetric. G: shear. Match modulus to deformation type.

Past Year Questions

15 questions from NEET 2020, 2021, 2022, 2023, 2024, 2025. Answers verified against NTA official keys. — click to collapse
NEET 2025

A balloon is made of a material of surface tension S and its inflation outlet (from where gas is filled in it) has small area A. It is filled with a gas of density ρ and takes a spherical shape of radius R. When the gas is allowed to flow freely out of it, its radius r changes from R to 0 (zero) in time T. If the speed v(r) of gas coming out of the balloon depends on r as ra and T ∝ Sα Aβ ργ Rδ then 1 1 1 1 7 1 1 3

1a= ,α= ,β=− ,γ= ,δ=
2a= ,α= ,β=−1,γ=+1,δ= 2 2 2 2 2 2 2 2 1 1 1 5 1 1 1 7
3a=− ,α=– ,β=−1,γ=− ,δ=
4a=− ,α=− ,β=−1,γ= ,δ= 2 2 2 2 2 2 2 2
NTA Answer: Option 4(final)
NEET 2025

Consider a water tank shown in the figure. It has one wall at x = L and can be taken to be very wide in the z direction. When filled with a liquid of surface tension S and density ρ, the liquid surface makes angle θ 0 (θ 0 << 1) with the x-axis at x = L. If y(x) is the height of the surface then the equation for y(x) is: dy (takeθ(x)=sinθ(x)=tanθ(x)= ,g is the acceleration due to gravity) dx dy ρg d2y ρg

1= x
2= x dx S dx2 S d2y ρg d2y ρg
3= y
4= dx2 S dx2 S
NTA Answer: Option 3(final)
NEET 2023

The venturi-meter works on

1Bernoulli’s principle
2The principle of parallel axes
3The principle of perpendicular axes
4Huygen’s principle
NTA Answer: Option 1(final)
NEET 2022

Given below are two statements : One is labelled as Assertion (A) and the other is labelled as Reason (R). Assertion (A): The stretching of a spring is determined by the shear modulus of the material of the spring. Reason (R): A coil spring of copper has more tensile strength than a steel spring of same dimensions. In the light of the above statements, choose the most appropriate answer from the options given below

1(A) is false but (R) is true
2Both (A) and (R) are true and (R) is the correct explanation of (A)
3Both (A) and (R) are true and (R) is not the correct explanation of (A)
4(A) is true but (R) is false
NTA Answer: Option 4(final)

How NEET usually asks this

5 recurring patterns from past papers — click to collapse

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