Bar to Foot Water (4 °C)

Europe adopted metric units broadly in the 19th and 20th centuries, and the bar (100,000 Pa) became the natural metric pressure unit for everyday engineering. The US never metricated, so pounds per square inch persisted. A car tire at 2.2 bar is the same as 32 psi — most modern tire placards list both. If you rent a car abroad and the pump reads bar, just divide your usual psi number by 14.5.

Standard aluminum scuba cylinders are rated to 200 bar (2,900 psi); steel tanks often go to 232 or 300 bar. At 200 bar, the air inside is compressed to 1/200th of its surface volume — a 12-liter tank holds 2,400 liters of breathing gas. Deep technical divers using trimix may use 300-bar steel tanks to maximize bottom time at extreme depths.

Close, but not quite. One bar is exactly 100,000 Pa; one standard atmosphere is 101,325 Pa — about 1.3% higher. The bar was designed as a round-number metric unit, not an exact atmospheric equivalent. For most practical purposes (cooking, tire inflation, diving rules of thumb) the difference is negligible, but in chemistry and calibration work the distinction matters.

Espresso machines run at 9 bar, car tires at 2–2.5 bar, a fire extinguisher at 12–15 bar, a garden pressure washer at 100–150 bar, and a diesel fuel injection rail at up to 2,500 bar. The range from gentle (carbonated water at 2–4 bar) to extreme (waterjet cutting at 4,000+ bar) makes the bar a versatile everyday engineering unit.

The SI only recognizes base and coherently derived units — pressure in SI is strictly the pascal (kg·m⁻¹·s⁻²). The bar is accepted "for use with SI" but is technically an outside unit, like the liter or the hour. The reason it thrives anyway is convenience: 2.2 bar is far friendlier than 220,000 Pa for a tire label, and industry adoption is too deep to reverse.

Because every foot of elevation equals exactly 1 ftH₂O of pressure at the tap below. 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 guarantee adequate pressure during peak demand. 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. So 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.