Foot Water (4 °C) to Atmosphere

Each foot of water head provides about 1 ftH₂O of static pressure when water density and gravity are close to the unit's reference conditions; actual pressure at a tap also depends on pipe losses. A comfortable shower needs about 20–25 ftH₂O, and a fire hydrant demands 40–60 ftH₂O. So a water tower serving a flat town typically stands 40–60 feet above rooftop level to provide pressure. Taller buildings in the service area need even more height — or booster pumps — because each story above ground "uses up" about 10 ftH₂O of the tower's gravity-supplied head.

1 ftH₂O ≈ 0.4335 psi. For an estimate, divide psi by 0.4335 (or multiply by 2.31) to get feet of head. A city water main at 60 psi delivers about 138 ft of head — enough to reach the 12th floor of a building by gravity alone. This 2.31 factor is worth memorising if you work in US plumbing or fire-protection engineering; it pops up in every pipe-sizing calculation.

Because the physical setup is literally vertical — a well pump sits at the bottom of a hole and pushes water up. Saying "the pump needs 150 feet of head" maps directly to the well depth plus the elevation to the pressure tank. Converting to psi (65 psi) loses that physical clarity. Fire-sprinkler designers think the same way: "how high does water need to climb?" is answered in feet, not pounds.

1 ftH₂O = 12 inH₂O, just as 1 foot = 12 inches. Inches of water are used for low-pressure air systems (HVAC ducts at 0.1–4 inH₂O), while feet of water handle higher liquid pressures (municipal water at 40–140 ftH₂O). The two scales cover different engineering domains but share the same underlying physics — pressure from a column of water at 4 °C under standard gravity.

About 1 atmosphere (14.7 psi). Divers learn the "33 feet" rule: every 33 feet of seawater adds 1 atm of pressure. (Fresh water is slightly less dense, so the equivalent is about 34 feet.) At 100 feet, a diver is under roughly 4 atm total — 3 gauge plus 1 atmospheric. This is why recreational dive limits are set at 130 ft (about 5 atm) — beyond that, nitrogen narcosis becomes a serious risk.

The number preserves an established pressure reference rather than selecting a new round SI value. In 1954, the 10th General Conference on Weights and Measures adopted the standard atmosphere for general use as exactly 1,013,250 dynes per square centimeter, equivalent to 101,325 Pa. It is a fixed reference, not a measurement of today’s weather pressure. Because the torr is defined as 1/760 of a standard atmosphere, 1 atm equals exactly 760 torr, but only approximately 760 mmHg.

Boiling happens when a liquid's vapor pressure equals the surrounding atmospheric pressure. At 1 atm (sea level), water must reach 100 °C for its vapor pressure to match. At 0.7 atm (about 3,000 m in the Andes), the bar is lower — water boils at roughly 90 °C. At the top of Everest (~0.33 atm), it boils near 70 °C, which is too cool to brew decent tea or cook pasta properly. Pressure cookers reverse the trick: by raising internal pressure to ~2 atm, they push the boiling point to about 120 °C, cooking food faster.

At 2 atm (10 meters underwater), you feel pressure in your ears and must equalise. At 4 atm (30 m), nitrogen narcosis can impair judgement — "the rapture of the deep." At 6 atm, recreational divers hit their safety limit. A hyperbaric chamber for wound healing runs at 2–3 atm. Submarine crews live at 1 atm inside the hull while the ocean outside may press at 40–100 atm, held back by inches of steel.

Standard Temperature and Pressure (STP) is defined as 0 °C and 1 atm. The ideal gas law (PV = nRT) often uses atmospheres when the gas constant R = 0.0821 L·atm/(mol·K). Boiling points are listed "at 1 atm." Chemical equilibrium constants (Kp) for gas-phase reactions use partial pressures in atm. Despite not being an SI unit, the atmosphere remains deeply embedded in chemistry textbooks and lab practice.

The deepest ocean trench: ~1,100 atm. The center of Jupiter: ~40 million atm. The center of the Sun: ~250 billion atm. A neutron star surface: ~10 billion billion atm. At the other extreme, interstellar space is about 10⁻¹⁸ atm — so close to perfect vacuum that a cubic meter contains only a few hydrogen atoms. Earth's 1 atm is a remarkably thin sliver in the cosmic range of pressures.