1.8CH1 Motion, Forces and Energy
Pressure — Cambridge O Level Physics 5054 Revision Notes & Topical Questions
10 min read 12 parts Lesson 8 of 8
Section 1 of 12Pressure and its equation
- Pressure
- the force acting normally per unit area, p = F ÷ A.What the symbols mean: p = pressure (Pa = N m−2) · F = force acting at right angles to the surface (N) · A = area (m2)
- (at right angles)
- Force is in N, area is in m2 and pressure is in pascals (Pa), where 1 Pa = 1 N/m2.
- the force acting normally per unit area, p = F ÷ A.
- Larger units
- 1 kPa = 1000 Pa and 1 MPa = 106 Pa.
- Reading the equation
- for a given force, a smaller area gives a larger pressure.
- For a given area, a larger force gives a larger pressure.
- Force from weight
- an object resting on a surface exerts a force equal to its weight, F = mg.
- A 60 kg student exerts about 590 N on the floor.
- Area units
- convert cm2 to m2 by dividing by 10 000, because 1 m2 = 10 000 cm2.
Section 2 of 12Changing pressure in everyday life
- Increase pressure
- make the area small.
- Knives, nails, needles and cutting wires have sharp edges so a modest force produces a large pressure.
- Decrease pressure
- make the area large.
- Snowshoes, wide tractor tyres, skis and the broad base of buildings spread the weight so the ground does not sink.
- Table of examples
- each links force, area and pressure.
| Situation | What changes | Result |
|---|---|---|
| Walking in snowshoes | Area is larger | Pressure is smaller, less sinking |
| Pressing a drawing pin | Tip area is tiny | Very large pressure, it enters wood |
| Caterpillar tracks | Area is large | Heavy vehicle does not sink |
| Stiletto heel | Area is small | Large pressure, can mark floors |
Section 3 of 12Pressure in liquids
- Pressure in a liquid
- it acts in all directions and increases with depth.
- A dam wall is thicker at the bottom because the pressure there is greatest.
- Equation
- the change in pressure with depth is Δp = ρgΔh.
- ρ is the density of the liquid in kg/m3, g is 9.8 N/kg and Δh is the vertical depth in metres.
- Where it comes from
- the pressure at depth h is the weight of the column of liquid above divided by the area, p = ρVg ÷ A = ρgh.
- Factors
- pressure depends on the depth and density but not on the shape of the container or the amount of liquid.
- A narrow tube and a wide lake with the same depth have the same pressure at the bottom.
- Total pressure
- the pressure at depth in an open liquid is the sum of atmospheric pressure and ρgh.
- Liquids are almost incompressible
- they transmit pressure through the whole liquid, which is used in hydraulics.
Section 4 of 12Atmospheric pressure and the barometer
- Atmospheric pressure
- the pressure caused by the weight of the air above us.
- At sea level it is about 100 000 Pa (1.0 × 105 Pa), or 760 mm of mercury.
- Variation with height
- it decreases as altitude increases because there is less air above.
- Climbers and aeroplanes experience lower pressure, which is why cabins are pressurised.
- Barometer
- an instrument that measures atmospheric pressure.
- A simple mercury barometer has a tube of mercury inverted in a dish and the column height, about 760 mm, shows the pressure.
- Why mercury is used
- it is very dense, so the column is a manageable height.
- With water the column would need to be about 10 m high.
- Aneroid barometer
- it uses a sealed metal box that changes shape with pressure and moves a pointer.
- Effects of atmospheric pressure
- a drinking straw works because suction lowers pressure and atmospheric pressure pushes the liquid up.
Section 5 of 12Manometer and pressure differences
- Manometer
- a U-tube containing liquid, used to measure the pressure of a gas supply or the difference between two pressures.
- How it works
- one side is connected to the gas and the other is open to the air.
- The liquid is pushed down on the gas side and rises on the other side until the pressures balance.
- Equation
- the gas pressure above atmospheric pressure equals ρgh, where h is the difference in the heights of the liquid levels.
- Using the manometer
- follow the steps.
- Connect one arm to the gas supply and leave the other open to the atmosphere.
- Measure the difference in heights of the liquid surfaces.
- Calculate Δp = ρgΔh.
- Add atmospheric pressure to find the absolute gas pressure.
- Same level rule
- points at the same height in the same continuous liquid have the same pressure.
Section 6 of 12Hydraulic machines
- Hydraulic system
- a closed system of liquid in connected cylinders that transmits pressure.
- The same pressure acts everywhere in the liquid because it is incompressible.
- Principle
- a small force on a small piston creates a pressure, p = F1 ÷ A1, which gives a large force on the large piston, F2 = p × A2.
- So F1 ÷ A1 = F2 ÷ A2.
- Force multiplier
- the large piston has a larger force but moves a shorter distance.
- The work done on both pistons is equal, so energy is conserved.
- Applications
- car brakes, hydraulic jacks, lifts and excavators.
- Brake fluid
- a liquid is used rather than a gas because it does not compress, so the force is transmitted immediately.
- Air bubbles in the pipes make brakes spongy because the air compresses.
Section 7 of 12Solving pressure problems
- Step-by-step method
- follow the same pattern for every pressure question.
- Write the known quantities with units.
- Identify whether the pressure is due to force on an area or liquid depth.
- Convert areas to m2 and depths to metres.
- Substitute into p = F ÷ A or p = ρgh.
- Give the answer in Pa or kPa.
- Link to density
- liquid pressure questions usually need a density from the table: water 1000 kg/m3, mercury 13 600 kg/m3.
- Link to forces
- once you know the pressure and area, the force on a surface is F = pA.
- A submarine window of area 0.20 m2 at 5.0 × 105 Pa carries a force of 1.0 × 105 N.
Section 8 of 12Direction of pressure and a demonstration
- Pressure acts at right angles
- the pressure at a surface produces a force at 90° to that surface.
- A liquid pushes outward on the walls of its container perpendicular to the wall at each point.
- Experiment to show it
- a tall can of water with small holes at different depths.
- Make three holes in a vertical line down the side of a plastic bottle and cover them with tape.
- Fill the bottle with water and keep it topped up.
- Remove the tape and watch the water jets.
- Each jet leaves at right angles to the wall, and the lowest jet goes farthest because the pressure there is greatest.
- Second demonstration
- a thin rubber sheet over a funnel bulges outward in every direction when the funnel is lowered into water.
- The bulge is greater at greater depth.
- Everyday link
- water towers are built high so that the pressure in the pipes at the bottom is large enough to push water to taps.
Section 9 of 12Reading a barometer
- Method
- follow the steps to find the atmospheric pressure from a mercury barometer.
- Fill a long glass tube with mercury and invert it in a dish of mercury.
- The mercury falls until its column is held up by the atmosphere, and a vacuum forms at the top.
- Measure the vertical height h of the column above the mercury surface in the dish.
- Atmospheric pressure = ρgh, or the height of the column in mm of mercury.
-- A column of 760 mm of mercury gives 13 600 × 9.8 × 0.760 = 1.01 × 105 Pa.
- Tilting the tube
- it does not change the vertical height, so the pressure reading stays the same.
Section 10 of 12Worked examples
A 70 kg man stands on both feet, each with an area of 0.020 m2. Find the pressure he exerts on the ground (g = 9.8 N/kg). [3]3 marks
- Weight = 70 × 9.8 = 686 N.
- Area = 2 × 0.020 = 0.040 m2.
- p = 686 ÷ 0.040 = 17 150 Pa.
Calculate the pressure at a depth of 25 m in the sea of density 1030 kg/m3, and the total pressure if atmospheric pressure is 1.0 × 105 Pa (g = 9.8 N/kg). [4]4 marks
- Δp = ρgh = 1030 × 9.8 × 25 = 2.52 × 105 Pa.
- Total pressure = 1.0 × 105 + 2.52 × 105 = 3.5 × 105 Pa.
In a hydraulic jack the small piston has an area of 4.0 cm2 and the large piston 100 cm2. A force of 50 N is applied to the small piston. Find the force on the large piston. [3]3 marks
- Pressure is the same, so F2 = F1 × A2 ÷ A1.
- F2 = 50 × 100 ÷ 4.0.
- F2 = 1250 N.
The mercury levels in a manometer connected to a gas supply differ by 80 mm. Find the gas pressure above atmospheric (ρ = 13 600 kg/m3, g = 9.8 N/kg). [3]3 marks
- h = 80 mm = 0.080 m.
- Δp = 13 600 × 9.8 × 0.080 = 10 660 Pa.
- The gas pressure is about 1.1 × 104 Pa above atmospheric.
Explain why a camel can walk on sand but a person with narrow shoes sinks in. [2]2 marks
- The camel's wide feet give a large contact area, so its weight produces a small pressure.
- The narrow shoes concentrate the weight on a small area, giving a larger pressure.
A mercury barometer column is 745 mm high. Find the atmospheric pressure in pascals (ρ = 13 600 kg/m3, g = 9.8 N/kg). [3]3 marks
- h = 745 mm = 0.745 m.
- p = ρgh = 13 600 × 9.8 × 0.745.What the symbols mean: p = pressure due to the liquid (Pa) · ρ = density of the liquid (kg m−3) · g = 9.81 N kg−1 · h = depth (m)
- p = 9.93 × 104 Pa, about 99 kPa.
Section 11 of 12Key terms
| Term | Meaning |
|---|---|
| Pressure | The force acting normally per unit area, p = F ÷ A, in pascals. |
| Pascal | The unit of pressure, 1 N/m2. |
| Atmospheric pressure | The pressure due to the weight of the air above, about 1.0 × 105 Pa at sea level. |
| Barometer | An instrument that measures atmospheric pressure. |
| Manometer | A U-tube liquid gauge used to measure pressure differences. |
| Hydraulic system | A liquid-filled system that transmits pressure to multiply a force. |
| Incompressible | Cannot easily be squashed into a smaller volume, as with liquids. |
Section 12 of 12Exam technique
- Using cm2 directly with N to get Pa — convert area to m2 first.
- Saying liquid pressure depends on the volume of liquid — it depends on depth, density and g only.
- Forgetting atmospheric pressure when asked for the total pressure at depth — add it to ρgh.
- Thinking hydraulic systems give free energy — the larger force moves a proportionally smaller distance.
- Measuring manometer height along the tube — use the vertical difference between levels.
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