Capillary Rise

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

Surface 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.


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

The excess pressure inside a soap bubble of radius r and surface tension T is:

MCQ 2Easy RecallPractice

The excess pressure inside a spherical liquid drop of radius r in air is:

MCQ 3Easy RecallPractice

Water rises in a glass capillary tube because the contact angle θ between water and glass satisfies:

MCQ 4Direct ApplicationPractice

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:

MCQ 5Direct ApplicationPractice

The work done in blowing a soap bubble of radius R from soap solution of surface tension T is:

MCQ 6Direct ApplicationPractice

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:

MCQ 7Concept TrapPractice

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:

MCQ 8CalculationPractice

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:

Quick recall before you leave

Worked Example

  1. 1

    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)

  2. 2

    Required

    (a) Excess pressure ΔP inside the bubble (b) Work W done in forming the bubble

  3. 3

    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).

  4. 4

    Formula

    (a) ΔP = 4T/r (b) W = T × 2 × 4πr²

  5. 5

    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

  6. 6

    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.

  7. 7

    Final answer

    (a) ΔP = 10 Pa (b) W ≈ 6.3 × 10⁻⁵ J

  8. 8

    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.

  9. 9

    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) ---

Before solving, remember these

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. 15

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

Sources

NCERT refs: Class 11 Physics Chapter 9, p.14 | Class 11 Physics Chapter 9, p.15

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