Hydraulic Press Simulator — Pascal's Law | Physlabo
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Hydraulic Press

Work the pump of a hydraulic jack and lift a car with one hand — or crush an egg, a walnut, a can and even a brick. The colour of the oil shows the pressure: during the down-stroke it is the same in both cylinders, and that is Pascal's law. The gauges, the stroke counter and the bars below the scene show the 'golden rule' of mechanics: what you gain in force you lose in distance, by the same factor.

Mouse: left button rotates, right button or Shift pans, wheel zooms. Phone: one finger rotates, two fingers pan and zoom

0
↓F1— hand force on the small piston ↑F2— oil pressure force on the big piston ↓P— weight of the load ●K1, K2, K3— valves: green — open, red — closed

The colour of the liquid shows the pressure (scale at the bottom left). Force arrows are not to scale (∝ ∛F); the numbers are exact.

320 N
While the load rises steadily, the hand pushes with exactly the force the load requires: F₁ = P·S₁/S₂. Spare force lets you pump faster. The hand pushes with full force when the piston presses against an object.
4.0 cm²
200 cm²
S₂/S₁ = 50

Press: oil is incompressible, so S₁h₁ = S₂h₂, and during the down-stroke the pressure is the same in both cylinders (Pascal's law). The weight of the oil column (≈ 3 kPa) is small compared with the pressure in the press and is neglected. The numbers do not depend on the playback speed.

F1
force the hand pushes with now
S2 / S1
force gain
p = F1 / S1
oil pressure from the hand
F2 = p·S2
force on the big piston
P = mg
weight of the load
F1 min
least hand force: the load together with the platform (59 N) times S₁/S₂
h2 = h1·S1/S2
rise per stroke (h₁ = 15 cm)
p1
small cylinder gauge
p2
big cylinder gauge

Pump strokes
Σh1
distance moved by the hand
H2
distance the big piston moved up in all strokes
A1 = ΣF1Δh1
work done by the hand
A2 = ΣF2Δh2
work of the oil on the big piston

In his Treatise on the Equilibrium of Liquids (published in 1663) Blaise Pascal described a 'new machine for multiplying forces': a vessel with two pistons, one a hundred times larger than the other. One man pushing the small piston balances a hundred men pushing the large one. A working hydraulic press was built by the Englishman Joseph Bramah in 1795. The hard part was not the idea but the seal: under high pressure the water leaked past the piston. The solution was a leather cup that the pressure itself pushes against the cylinder wall — the higher the pressure, the tighter the seal. Jacks, car brakes, excavator buckets, garage lifts and the presses that stamp car bodies all work on the same principle today.

KEY FORMULAS

Pressure

$$p = \frac{F}{S}$$

F is the force acting perpendicular to the surface, N; S is the area of the surface, m²; p is the pressure, Pa (1 Pa = 1 N/m²)

▶ Detailed Explanation

Pressure tells how much force falls on each square metre of a surface. The same force spread over a smaller area creates a larger pressure. A hand pushing a 4 cm² piston with 300 N creates an oil pressure of 300 / 0.0004 = 750,000 Pa = 750 kPa.

1 Pa is a very small pressure — roughly what a sheet of paper lying on a table exerts. That is why kilopascals and megapascals are used in practice. Atmospheric pressure at the Earth's surface is about 101 kPa.

Pascal's law

$$\Delta p_A = \Delta p_B = \Delta p = \frac{F}{S}$$

Δp is the extra pressure created by the piston (Pa); A and B are any points in the liquid

▶ Detailed Explanation

Pressure applied to a liquid or gas is transmitted unchanged to every point of the fluid and in all directions. If the piston raises the pressure beneath it by 5 kPa, then at the bottom, at the side walls and at any hole the pressure has risen by exactly 5 kPa.

A solid cannot do this: it transmits a force only along its line of action. A liquid spreads pressure in all directions because its particles slide freely past one another. That is why the jets from Pascal's ball spurt equally in all directions, and why the oil pressure in the small and big cylinders of a press is the same.

Force gain of a hydraulic press

$$\frac{F_1}{S_1} = \frac{F_2}{S_2} \quad\Rightarrow\quad \frac{F_2}{F_1} = \frac{S_2}{S_1}$$

F₁, S₁ are the force on and area of the small piston; F₂, S₂ are those of the big piston

▶ Detailed Explanation

By Pascal's law the pressure under both pistons is the same, so the forces are in the ratio of the areas. If the big piston has 50 times the area, the force on it is 50 times larger: 300 N becomes 15 kN.

Note that the formula compares areas, not diameters. If the big piston's diameter is 10 times larger, its area is 100 times larger, and the force gain is 100.

The 'golden rule': loss in distance

$$S_1 h_1 = S_2 h_2, \qquad \frac{h_1}{h_2} = \frac{S_2}{S_1}, \qquad F_1 h_1 = F_2 h_2$$

h₁ is the distance moved by the small piston, h₂ by the big piston, m; F₁h₁ and F₂h₂ are the work done, J

▶ Detailed Explanation

Oil is practically incompressible: as much leaves the small cylinder as arrives in the big one. The volumes are equal, S₁h₁ = S₂h₂, so the big piston moves a distance as many times smaller as its area is larger. With S₂/S₁ = 50 a 15 cm stroke of the hand lifts the load by 3 mm.

Multiply the forces by the distances: F₁h₁ = F₂h₂. The work done by the hand equals the work done by the oil on the big piston. No machine gives a gain in work: what we gain in force we lose in distance, by the same factor.

Pressure. Pressure is the force acting perpendicular to a surface divided by the area of that surface: p = F/S. Its unit is the pascal: 1 Pa = 1 N/m². The same force presses harder on a smaller area. In the press the hand pushes a small piston, so even a modest force creates a large pressure in the oil: 300 N on 4 cm² is 750 kPa, seven and a half times atmospheric pressure.

Pascal's law in the press. Pressure applied to a liquid is transmitted unchanged to every point of it. So the pressure created by the hand in the small cylinder is the same under the big piston. In the simulator you can see it in the colour of the oil: during the down-stroke both cylinders have the same colour, and the gauges p₁ and p₂ read the same number.

Force gain. Since the pressure under the pistons is the same, F₁/S₁ = F₂/S₂, and the force on the big piston is F₂ = F₁·S₂/S₁. The press multiplies force by the ratio of the big piston's area to the small one's. With S₁ = 4 cm² and S₂ = 200 cm² the gain is 50: a 300 N push produces 15 kN — enough to lift a 1.5-tonne car (its weight is 14.7 kN). Compare areas, not diameters: a piston with twice the diameter has four times the area.

How a jack works. A real jack is a pump with two check valves. On the down-stroke valve K2 lets oil from the small cylinder into the big one — at that moment the cylinders are connected, exactly like the textbook press. On the up-stroke K2 closes and holds the load while the small cylinder draws oil from the tank through valve K1. The release valve K3 lets the oil back into the tank, and the load goes down smoothly. The p(t) graph shows the valves at work: on the down-stroke the pressures in the cylinders are equal, on the up-stroke the pressure in the small cylinder drops to zero while the big one keeps it.

The 'golden rule' of mechanics. Oil is practically incompressible, so the volume that leaves the small cylinder arrives in the big one: S₁h₁ = S₂h₂. The big piston moves a distance as many times smaller as the force is larger: one 15 cm stroke of the hand lifts the car by only 3 mm. Lifting it by 12 cm takes 40 strokes, and the hand travels 6 m. The work done by the hand equals the work done by the oil on the big piston: F₁h₁ = F₂h₂. A press gives no gain in work — the Force, Distance and Work bars below the scene show this at a glance.

Try it yourself. Set the hand force to 200 N and try to lift the car — the press stops, and the hint tells you how much force is missing. Increase S₂ and watch the force gain grow while the load rises more slowly. Choose the brick: it withstands about 78 kN, and to crush it with a 300 N push you need an area ratio above 260. The egg has a catch: with S₂/S₁ = 2 a 50 N push will not crush it — part of F₂ goes into holding up the platform itself, which weighs about 59 N.