Pressure

Pressure in liquids

Pressure in liquids Core 2 min read

Pressure in liquids

Pressure in a liquid increases with depth and depends on the density of the liquid. It acts equally in all directions at a given depth. \[ P = h\rho g \]
SymbolQuantityUnit
\( P \)Pressure at depth \( h \)pascal, Pa
\( h \)Depth below the liquid surfacemetre, m
\( \rho \)Density of the liquidkg/m³
\( g \)Gravitational field strengthN/kg (= 10 N/kg near Earth's surface)
This formula gives the additional pressure due to the liquid column — it does not include atmospheric pressure acting on the surface.
Key properties of liquid pressure:
  • Pressure increases with depth — the greater the depth, the greater the weight of liquid above.
  • Pressure depends on the liquid's density — mercury (13 600 kg/m³) produces far greater pressure at a given depth than water (1000 kg/m³).
  • Pressure is independent of the shape of the container — only the vertical depth matters.
  • Pressure at a given depth acts equally in all directions — upward, downward, and sideways.
surface h₁ h₂ h₃ depth increases

Worked examples

Example 1 — pressure at depth in water

Calculate the pressure due to the water at a depth of 5.0 m in a swimming pool. (ρ_water = 1000 kg/m³, g = 10 N/kg)

\( P = h\rho g = 5.0 \times 1000 \times 10 = 50\,000\,\text{Pa} = 50\,\text{kPa} \)

Example 2 — find depth from pressure

The pressure at the bottom of a tank of mercury is 65 000 Pa. Find the depth of the mercury. (ρ_mercury = 13 600 kg/m³, g = 10 N/kg)

\( h = \dfrac{P}{\rho g} = \dfrac{65\,000}{13\,600 \times 10} = \dfrac{65\,000}{136\,000} = 0.478\,\text{m} \approx 0.48\,\text{m} \)

Example 3 — compare two liquids at the same depth

A diver is at a depth of 10 m in fresh water (ρ = 1000 kg/m³) and in sea water (ρ = 1025 kg/m³). Compare the pressures from each liquid alone.

Fresh water: \( P = 10 \times 1000 \times 10 = 100\,000\,\text{Pa} \)

Sea water: \( P = 10 \times 1025 \times 10 = 102\,500\,\text{Pa} \)

Sea water exerts 2500 Pa more pressure at the same depth due to its higher density.

Applications

  • Dams — built thicker at the base because pressure increases with depth; the base must withstand greater force.
  • Submarines — designed with reinforced hulls to withstand increasing pressure at depth.
  • Hydraulic systems — liquid transmits pressure equally in all directions (Pascal's principle), used in car brakes and hydraulic presses.
  • U-tube manometer — liquid levels show relative pressure; the side with higher pressure is lower.
\( P = h\rho g \) gives only the pressure from the liquid column. The total pressure at depth is \( P_\text{total} = P_\text{atm} + h\rho g \). Questions usually ask for the pressure due to the liquid only — read carefully whether atmospheric pressure should be included.