Capillary rise
h = 2 T cos θ / (ρ g r), where θ is contact angle, r is capillary tube radius. Rises if θ < 90° (wetting), depresses if θ > 90° (e.g. mercury in glass).
-- NCERT, p. 15Surface tension applications — drops, bubbles, and capillary rise
The high-frequency trap in this topic is confusing the factor in the excess-pressure formula: drops have one free surface (ΔP = 2T/r), soap bubbles have two (ΔP = 4T/r), and an air bubble inside a liquid has one surface again (ΔP = 2T/r). NEET has tested this distinction repeatedly (2022, 2023, 2025).
Excess pressure inside curved surfaces. A spherical liquid drop in air encloses fluid behind a single curved surface. The inward pull of surface tension creates an excess internal pressure ΔP = 2T/r, where T is surface tension and r is the drop radius. A soap bubble floating in air, however, has an inner surface and an outer surface — both contribute, giving ΔP = 4T/r. An air bubble trapped inside a liquid has only the liquid-air interface (one surface), so it follows the drop formula: 2T/r. This three-way classification is the direct source of wrong options in NEET (NCERT Class 11 Physics, Chapter 9, page 14).
Capillary rise. When a narrow tube is dipped into a liquid, the liquid rises (or depresses) by:
h = 2T cos θ / (ρgr)
where θ is the contact angle, ρ is the liquid density, and r is the tube radius (NCERT Class 11 Physics, Chapter 9, page 15). For water-glass (θ ≈ 0°, cos θ = 1), the liquid rises. For mercury-glass (θ > 90°, cos θ < 0), the meniscus depresses. Smaller radius → greater rise — this inverse proportionality (h ∝ 1/r) is a common numerical test point.
Watch out: When a problem says "bubble," identify which kind — soap bubble in air (two surfaces, factor 4) or air bubble in liquid (one surface, factor 2). The word "bubble" alone is the trigger for this trap.
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
The excess pressure inside a soap bubble of radius r and surface tension T is:
The excess pressure inside a spherical liquid drop of radius r in air is:
Water rises in a glass capillary tube because the contact angle θ between water and glass satisfies:
A capillary tube of radius 0.5 mm is dipped in water (surface tension T = 7.0 × 10⁻² N/m, density ρ = 1.0 × 10³ kg/m³, contact angle θ = 0°). Taking g = 10 m/s² (exact), the height of capillary rise is:
The work done in blowing a soap bubble of radius R from soap solution of surface tension T is:
Two capillary tubes of radii r and 2r are dipped in the same liquid. If h₁ and h₂ are the respective heights of rise, then h₁/h₂ is:
An air bubble of radius r is formed inside a liquid of surface tension T. The excess pressure inside this bubble compared to the surrounding liquid is:
A soap bubble of radius 2.0 cm has surface tension T = 3.0 × 10⁻² N/m. The excess pressure inside the bubble and the total work done in forming it from flat film are, respectively:
Given
- Radius: r = 1.0 × 10⁻² m - Surface tension: T = 2.5 × 10⁻² N/m - Configuration: soap bubble in air (two free surfaces)
Required
(a) Excess pressure ΔP inside the bubble (b) Work W done in forming the bubble
Concept
A soap bubble has two surfaces (inner and outer). Excess pressure uses the factor 4T/r. Work done equals surface tension × total new surface area created (two spherical surfaces).
Formula
(a) ΔP = 4T/r (b) W = T × 2 × 4πr²
Substitution
(a) ΔP = 4 × 2.5 × 10⁻² / (1.0 × 10⁻²) (b) W = 2.5 × 10⁻² × 2 × 4π × (1.0 × 10⁻²)²
Calculation
(a) ΔP = 10.0 × 10⁻² / 1.0 × 10⁻² = 10 Pa (b) W = 2.5 × 10⁻² × 2 × 4π × 1.0 × 10⁻⁴ W = 2.5 × 10⁻² × 8π × 10⁻⁴ W = 2.5 × 10⁻² × 2.513 × 10⁻³ W = 6.28 × 10⁻⁵ J ≈ 6.3 × 10⁻⁵ J Note on exact constants: the factor 4 in the pressure formula and the factors 2 and 4π in the work formula are exact (geometric constants); they do not limit significant figures. The result is reported to 2 significant figures, matching the given data.
Final answer
(a) ΔP = 10 Pa (b) W ≈ 6.3 × 10⁻⁵ J
Common trap
Using 2T/r instead of 4T/r gives ΔP = 5 Pa (half the correct value) and W = 3.1 × 10⁻⁵ J (half the correct work). This is the drop formula applied to a bubble — wrong because a soap bubble has two surfaces, not one. Similarly, for part (b), using only one spherical area (4πr²) instead of two (8πr²) halves the work.
Similar NEET-style question
A soap bubble has radius 5.0 × 10⁻³ m and surface tension 4.0 × 10⁻² N/m. What is the gauge pressure inside the bubble? (Answer: ΔP = 4 × 4.0 × 10⁻² / 5.0 × 10⁻³ = 32 Pa) ---
h = 2 T cos θ / (ρ g r), where θ is contact angle, r is capillary tube radius. Rises if θ < 90° (wetting), depresses if θ > 90° (e.g. mercury in glass).
-- NCERT, p. 15Conservation 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
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