Stokes' law
Drag force on a sphere of radius r moving with velocity v through a viscous fluid (η): F = 6π η r v. Holds for low Reynolds number (smooth, slow flow).
-- NCERT, p. 9When a small sphere falls through a viscous fluid, the drag force on it is not proportional to velocity squared (as in turbulent flow) but linearly proportional to velocity. This is Stokes' law.
The formula: F = 6πηrv, where η is the fluid's dynamic viscosity, r is the sphere's radius, and v is its velocity. This holds strictly for smooth, slow flow — low Reynolds number — past a spherical body in a Newtonian fluid (NCERT Class 11 Physics, Chapter 10 "Mechanical Properties of Fluids," page 9).
Where NEET uses this: Stokes' law is the engine behind terminal velocity problems. A sphere released in a viscous liquid accelerates initially, but the drag force (∝ v) grows until it balances the net downward force (weight minus buoyancy). At that point, acceleration is zero and the sphere moves at constant terminal velocity:
v_t = (2r²g(ρ_s − ρ_f)) / (9η)
The high-frequency mistake: treating terminal velocity as proportional to r instead of r². Since Stokes drag scales as r·v while gravitational pull scales as r³, the balance yields v_t ∝ r². Doubling the radius quadruples — not doubles — the terminal velocity. This is a common distractor anchor in NEET.
The v(t) curve trap: the velocity-time graph for a falling sphere is not a straight line. It curves upward and asymptotically flattens at v_t. A distractor showing constant acceleration (straight line) or overshoot (oscillation) is wrong — viscous drag produces a smooth, monotonic approach to terminal velocity with no overshoot.
Watch-out: Stokes' law applies only at low Reynolds numbers. If a problem describes turbulent conditions or high-speed flow, this formula does not apply.
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
According to Stokes' law, the viscous drag force on a sphere moving through a fluid is proportional to which of the following?
What is the SI unit of dynamic viscosity (η) that appears in Stokes' law?
Which of the following is NOT a necessary condition for Stokes' law to be valid?
A steel ball is dropped into a tall cylinder of glycerine. The terminal velocity of the ball is v_t. If the radius of the ball is doubled while all other conditions remain unchanged, the new terminal velocity is:
Two spheres of the same material but radii r and 3r are dropped simultaneously into a viscous liquid. The ratio of their terminal velocities v₁ : v₂ is:
A small sphere falling through a viscous fluid reaches terminal velocity. At terminal velocity, the net force on the sphere is:
A sphere falls from rest into a tall column of viscous oil. Which velocity-time graph correctly represents its motion until it reaches terminal velocity?
A sphere of density 2.0 × 10³ kg/m³ and radius 1.0 × 10⁻³ m falls through a liquid of density 1.0 × 10³ kg/m³ and viscosity 1.0 Pa·s. Taking g = 10 m/s² (exact), the terminal velocity is closest to:
Pattern: Terminal velocity scaling (from PYQ pattern NEET pattern: terminal velocity scaling, observed in NEET 2021, 2022)
Given
- r = 2.0 × 10⁻³ m (2 sig figs) - ρ_s = 8.0 × 10³ kg/m³ (2 sig figs) - ρ_f = 1.2 × 10³ kg/m³ (2 sig figs) - η = 0.90 Pa·s (2 sig figs) - g = 9.8 m/s² (exact, problem-defined)
Required
Terminal velocity v_t.
Concept
At terminal velocity, the net force on the sphere is zero: weight = buoyant force + Stokes drag. The resulting expression for v_t follows from setting the net downward force equal to 6πηrv_t and solving for v_t.
Formula
v_t = 2r²g(ρ_s − ρ_f) / (9η)
Substitution
v_t = 2 × (2.0 × 10⁻³)² × 9.8 × (8.0 × 10³ − 1.2 × 10³) / (9 × 0.90)
Calculation
- r² = (2.0 × 10⁻³)² = 4.0 × 10⁻⁶ m² - (ρ_s − ρ_f) = 6.8 × 10³ kg/m³ - Numerator = 2 × 4.0 × 10⁻⁶ × 9.8 × 6.8 × 10³ = 2 × 4.0 × 9.8 × 6.8 × 10⁻⁶⁺³ = 2 × 4.0 × 9.8 × 6.8 × 10⁻³ = 2 × 266.56 × 10⁻³ = 533.12 × 10⁻³ = 0.53312 - Denominator = 9 × 0.90 = 8.1 - v_t = 0.53312 / 8.1 = 0.06582... m/s **Note on exact constants:** g = 9.8 m/s² is given as an exact problem-defined value and does not constrain significant figures. The numerical constants 2 and 9 in the formula are exact integers.
Final answer
v_t ≈ 6.6 × 10⁻² m/s (reported to 2 significant figures, matching the least precise given quantity).
Common trap
The most common error is treating v_t ∝ r instead of v_t ∝ r². If the problem asked "what happens when the radius is halved?", the trap answer is v_t/2, but the correct answer is v_t/4 (since v_t scales as r²). Always check the power of r before answering scaling questions.
Similar NEET-style question
A lead shot of radius r has terminal velocity v in glycerine. A second lead shot of radius 2r is dropped in the same glycerine. What is its terminal velocity? Answer: v_t ∝ r², so new v_t = (2r/r)² × v = 4v. ---
Drag force on a sphere of radius r moving with velocity v through a viscous fluid (η): F = 6π η r v. Holds for low Reynolds number (smooth, slow flow).
-- NCERT, p. 9Conservation of energy along a streamline of incompressible non-viscous flow.
| Symbol | Quantity | SI Unit |
|---|---|---|
| P | pressure | Pa |
| rho | density | kg/m^3 |
| v | speed | m/s |
| g | gravity | m/s^2 |
| h | height | m |
Resistance of a material to uniform compression. Inverse: compressibility.
| Symbol | Quantity | SI Unit |
|---|---|---|
| K | bulk modulus | Pa |
| V | volume | m^3 |
| P | pressure | Pa |
Height a liquid rises (or falls) in a capillary tube. cos(theta) > 0: rises (wetting); < 0: depresses.
| Symbol | Quantity | SI Unit |
|---|---|---|
| h | capillary height | m |
| T | surface tension | N/m |
| theta | contact angle | rad |
| rho | density | kg/m^3 |
| r | tube radius | m |
Pressure at depth h below free surface of fluid of density rho.
| Symbol | Quantity | SI Unit |
|---|---|---|
| P | total pressure | Pa |
| P0 | atmospheric/surface pressure | Pa |
| rho | density | kg/m^3 |
| h | depth | m |
Heat absorbed/released during phase change at constant T. L_fusion or L_vaporisation.
| Symbol | Quantity | SI Unit |
|---|---|---|
| Q | heat | J |
| m | mass | kg |
| L | latent heat | J/kg |
Heat required to raise mass m by temperature Delta_T. Specific heat c is material property.
| Symbol | Quantity | SI Unit |
|---|---|---|
| Q | heat | J |
| m | mass | kg |
| c | specific heat | J/kg/K |
| Delta_T | temp change | K |
Radiation power from a body. Black body epsilon=1; net to surroundings P = sigma*epsilon*A*(T^4 - T_s^4).
| Symbol | Quantity | SI Unit |
|---|---|---|
| sigma | Stefan-Boltzmann = 5.67e-8 | W/m^2/K^4 |
| epsilon | emissivity (0-1) | - |
| A | surface area | m^2 |
| T | absolute temp | K |
Drag force on a sphere of radius r moving with velocity v through viscous fluid (low Reynolds number).
| Symbol | Quantity | SI Unit |
|---|---|---|
| F | drag force | N |
| eta | viscosity | Pa*s |
| r | sphere radius | m |
| v | velocity | m/s |
Excess internal pressure due to surface tension. Bubble has 2 surfaces, hence factor 4.
| Symbol | Quantity | SI Unit |
|---|---|---|
| Delta_P | excess pressure | Pa |
| T | surface tension | N/m |
| r | radius | m |
Constant velocity reached when net force is zero (gravity balanced by buoyancy + viscous drag).
| Symbol | Quantity | SI Unit |
|---|---|---|
| v_t | terminal velocity | m/s |
| r | sphere radius | m |
| rho_s | sphere density | kg/m^3 |
| rho_f | fluid density | kg/m^3 |
| eta | viscosity | Pa*s |
Fractional change in length, area, volume per degree temperature change.
| Symbol | Quantity | SI Unit |
|---|---|---|
| alpha | linear coefficient | 1/K |
| beta | volume coefficient | 1/K |
| Delta_T | temperature change | K |
Ratio of longitudinal stress to longitudinal strain in a stretched wire/rod within elastic limit.
| Symbol | Quantity | SI Unit |
|---|---|---|
| Y | Young's modulus | Pa |
| F | applied force | N |
| A | cross-section area | m^2 |
| L | original length | m |
| Delta_L | extension | m |
These are the exact patterns that cause wrong answers in NEET. Each trap includes when it triggers and how to avoid it.
Category: Similar Terms
Student uses 2T/r for soap bubble (drop formula). Bubble has 2 surfaces → 4T/r.
Question mentions soap bubble OR liquid drop OR air bubble in liquid.
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.
Problem describes longitudinal stretching (use Y), volumetric pressure (use K), or shear (use G).
Y: longitudinal stress/strain. K: volumetric. G: shear. Match modulus to deformation type.
Root cause: concept gap
Drop in air: 1 surface → ΔP = 2T/r. Soap bubble: 2 surfaces (inner + outer) → ΔP = 4T/r. Air bubble inside liquid: 1 surface → 2T/r.
Root cause: formula misuse
v_t ∝ r² (because Stokes drag ∝ r v, gravity ∝ r³ - r³ = r³_diff). Doubling radius quadruples terminal velocity, not doubles.
Root cause: formula misuse
Y for longitudinal stretch (FL/A·ΔL); K for volumetric compression (-V·dP/dV); G for shear. Match modulus type to deformation type before computing.
If a soap bubble expands, the pressure inside the bubble
forgets height term
Drops rho*g*h term
equates pressures incorrectly
Picks wrong reference points
ignores mass difference
Compares only specific heats, not masses
uses 2T r instead of 4T r for bubble
Treats soap bubble like a drop
expects linear acceleration
Default to constant acceleration without recognising drag-induced terminal v
uses bulk modulus formula
Confuses Y with K
Test yourself on this topic with real past-paper questions:
Practice this topic →Get a structured 30-day Mechanics plan and a complete formula booklet — delivered to your inbox instantly.