Density
Density — The mass per unit volume of a substance, ρ = m/V. Measured in kg m⁻³ or g cm⁻³.
Density is a property of the material rather than of the object. A steel pin and a steel bridge have identical densities; they differ only in how much steel there is. This is why density is useful for identifying a substance when you cannot tell by looking.
Water has a density of 1000 kg m⁻³, which is the same as 1.0 g cm⁻³. That number is worth knowing, because it is the reference point for whether something floats. Anything less dense than water floats in it; anything denser sinks.
A steel ship floats even though steel is eight times denser than water, because the relevant density is that of the whole ship — steel plus the large volume of air inside the hull. Fill the hull with water and the average density rises above that of water, and the ship sinks.
- ρ
- densitykg m⁻³
- m
- masskg
- V
- volumem³
A metal block measures 4.0 cm × 3.0 cm × 2.0 cm and has a mass of 216 g. Calculate its density in g cm⁻³ and state whether it would float in water.
- Volume
= 4.0 × 3.0 × 2.0 = 24 cm³. ρ = m/V = 216 / 24.ρ = 9.0 g cm⁻³.- Water is 1.0 g cm⁻³, so the block is nine times denser and sinks.Compare with water rather than guessing.
9.0 g cm⁻³ — it sinks
Pressure
Pressure — The force acting per unit area, at right angles to a surface, p = F/A. Measured in pascals, where one pascal is one newton per square metre.
The same force spread over a different area produces a very different pressure, and that single idea explains a long list of everyday designs.
A drawing pin has a broad head and a sharp point. Your thumb pushes with a modest force over the large area of the head, so the pressure on your thumb is small and it does not hurt. That same force acts through the tiny area of the point, giving an enormous pressure that pushes into the wood.
The reverse trick is used to reduce pressure. Skis, snowshoes and the wide tracks of a tractor all spread the same weight over a much larger area, so the pressure on soft ground is low enough that the vehicle does not sink. Camels have broad feet for the same reason.
Pressure acts at right angles to whatever surface it meets, and in a fluid it acts in all directions equally.
- p
- pressurePa
- F
- force at right angles to the surfaceN
- A
- aream²
Convert areas before substituting
A square centimetre is 10⁻⁴ m², not 10⁻² m². The prefix gets squared along with the unit. Substituting cm² directly into p = F/A makes the pressure ten thousand times too small, and the answer still looks like a number.
Pressure in a liquid
Pressure in a liquid increases with depth, because the deeper you go the greater the weight of liquid above pressing down. It does not depend on the shape of the container or on how much liquid there is in total — only on the depth, the density and the gravitational field strength.
That is why a dam is built much thicker at the bottom than at the top, and why a diver feels increasing pressure on the ears as they descend. It is also why water squirts furthest from the lowest hole in a punctured can.
At a given depth the pressure acts equally in all directions, not just downwards. This is what makes hydraulic systems possible: pressure applied at one point in an enclosed liquid is transmitted undiminished throughout it, so a small force on a small piston produces a large force on a large one.
- p
- pressurePa
- ρ
- density of the liquidkg m⁻³
- g
- gravitational field strengthN kg⁻¹
- h
- depthm
A diver is 25 m below the surface of the sea, where the water has density 1030 kg m⁻³. Calculate the pressure due to the water. Take g = 9.8 N kg⁻¹.
- Use
p = ρgh.All three quantities are given. p = 1030 × 9.8 × 25.p = 252 350 Pa.≈ 2.5 × 10⁵ Pa, about two and a half atmospheres.Adding atmospheric pressure would give the total pressure on the diver.
2.5 × 10⁵ Pa from the water alone
Move the depth slider and watch the pressure climb in a straight line — p = ρgh. Switch to mercury and the line tilts sharply: 13.6 times the density means 13.6 times the pressure at the same depth. Notice the arrows at the marker: pressure acts equally in every direction.
Atmospheric pressure and the manometer
The atmosphere is a layer of air several kilometres deep, and its weight presses on everything at the surface at about 1.0 × 10⁵ Pa. We do not notice it because it acts equally in all directions, including from inside our bodies outwards.
Atmospheric pressure falls with altitude, because there is less air above you. This is why aircraft cabins are pressurised and why water boils at a lower temperature on a mountain.
A manometer measures the pressure of a gas supply by connecting it to a U-tube containing liquid. The gas pushes the liquid down on one side and up on the other, and the difference in the two levels gives the pressure difference directly through p = ρgh. If the levels are equal, the gas is at exactly atmospheric pressure.
A mercury barometer works on the same principle to measure atmospheric pressure itself. Atmospheric pressure supports a column of mercury about 760 mm tall — and mercury is used rather than water precisely because it is so dense that the column is a manageable height. A water barometer would need to be over ten metres tall.
Key points
- Density is mass per unit volume and identifies the material.
- Pressure is force per unit area — a sharp point concentrates it, a broad foot spreads it.
- Pressure in a liquid depends on depth and density, not on the shape of the container.
- At a given depth, pressure acts equally in all directions.
- Convert cm² to m² by
10⁻⁴and cm³ to m³ by10⁻⁶.