Pressure due to fluid column
P = P_0 + ρ g h, where P_0 is atmospheric pressure, ρ is fluid density, h is depth. Pressure increases linearly with depth in a static fluid.
-- NCERT, p. 3The pressure at any point inside a static fluid increases with depth. This is one of those topics where the formula looks simple — P = P₀ + ρgh — but NEET questions test whether you truly understand what each symbol means and what conditions make the formula valid.
The core idea. Consider a horizontal surface at depth h below the free surface of a fluid at rest. The weight of the fluid column above that surface creates additional pressure beyond whatever pressure acts on the free surface. NCERT Class 11 Physics Chapter 9 (Mechanical Properties of Fluids), page 3, derives this by balancing forces on a thin fluid element: the pressure difference between top and bottom faces equals the weight of the fluid slab per unit area.
The result: P = P₀ + ρgh, where P₀ is the pressure at the free surface (usually atmospheric pressure), ρ is the fluid density, g is gravitational acceleration, and h is the vertical depth below the free surface.
Three conditions that must hold:
What to watch for in NEET questions:
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
The pressure at a point inside a static liquid depends on which of the following?
What is the SI unit of pressure?
Gauge pressure at a depth h in a liquid of density ρ is:
A tank contains water (ρ = 1.0 × 10³ kg/m³) open to the atmosphere. What is the gauge pressure at a depth of 5.0 m? (Take g = 10 m/s², exact.)
A U-tube manometer contains mercury (ρ = 13.6 × 10³ kg/m³). The difference in mercury levels between the two arms is 20.0 cm. What is the pressure difference being measured? (Take g = 9.8 m/s².)
Two connected vessels contain the same liquid at rest. Vessel A has a narrow neck and vessel B has a wide base. The liquid level in both vessels is the same. Which statement is correct about the pressure at the bottom of each vessel?
A closed tank is completely filled with water and pressurised so that the pressure at the top surface is 2.0 × 10⁵ Pa. The tank is 3.0 m deep. What is the absolute pressure at the bottom? (ρ_water = 1.0 × 10³ kg/m³, g = 9.8 m/s².)
A swimming pool has fresh water (ρ = 1.00 × 10³ kg/m³) to a depth of 4.0 m. A layer of oil (ρ = 8.0 × 10² kg/m³) of thickness 1.0 m floats on top. What is the gauge pressure at the bottom of the pool? (Take g = 10 m/s², exact.)
Given
A cylindrical vessel contains two immiscible liquids. The bottom layer is mercury (ρ₁ = 13.6 × 10³ kg/m³) of height h₁ = 5.00 cm. The top layer is water (ρ₂ = 1.00 × 10³ kg/m³) of height h₂ = 40.0 cm. The vessel is open to the atmosphere (P₀ = 1.013 × 10⁵ Pa). Take g = 9.80 m/s².
Required
Find the absolute pressure at the bottom of the vessel.
Concept
For two immiscible fluid layers stacked vertically, the pressure at the bottom is the sum of atmospheric pressure and the ρgh contributions of each layer: P = P₀ + ρ₂gh₂ + ρ₁gh₁.
Formula
P = P₀ + ρ₂gh₂ + ρ₁gh₁
Substitution
Convert heights to metres: h₁ = 5.00 cm = 5.00 × 10⁻² m; h₂ = 40.0 cm = 4.00 × 10⁻¹ m. P = 1.013 × 10⁵ + (1.00 × 10³)(9.80)(4.00 × 10⁻¹) + (13.6 × 10³)(9.80)(5.00 × 10⁻²)
Calculation
Water contribution: (1.00 × 10³)(9.80)(4.00 × 10⁻¹) = 3.920 × 10³ Pa Mercury contribution: (13.6 × 10³)(9.80)(5.00 × 10⁻²) = 6.664 × 10³ Pa Total gauge pressure: 3.920 × 10³ + 6.664 × 10³ = 1.0584 × 10⁴ Pa Absolute pressure: 1.013 × 10⁵ + 1.058 × 10⁴ = 1.119 × 10⁵ Pa Note on significant figures: g = 9.80 m/s² is given to 3 significant figures. All given quantities have 3 significant figures, so the final answer is reported to 3 significant figures.
Final answer
**P ≈ 1.12 × 10⁵ Pa** (3 significant figures).
Common trap
A frequent error is forgetting to convert centimetres to metres before substituting into ρgh. Using h = 40.0 (without converting) gives an answer 100 times too large. Another common error: treating the two-layer system as a single fluid by using only one density — each layer must have its own ρgh term.
Similar NEET-style question
A vessel open to the atmosphere contains oil (ρ = 9.00 × 10² kg/m³, height 30.0 cm) on top of water (ρ = 1.00 × 10³ kg/m³, height 20.0 cm). Find the gauge pressure at the bottom. Answer: ρ_oil × g × h_oil + ρ_water × g × h_water = (9.00 × 10²)(9.80)(0.300) + (1.00 × 10³)(9.80)(0.200) = 2.646 × 10³ + 1.960 × 10³ = 4.61 × 10³ Pa. ---
P = P_0 + ρ g h, where P_0 is atmospheric pressure, ρ is fluid density, h is depth. Pressure increases linearly with depth in a static fluid.
-- NCERT, p. 3Conservation 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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