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SCIENCE · INVESTIGATE AND EXPLAIN

Calculate pressure force from both sides

Use pressure differences rather than one-sided absolute pressure to find a panel’s net load.

Learning outcome: Distinguish absolute and gauge pressure, convert pressure and area to force, and add opposing pressure forces with a consistent direction.

Starting recap

Pressure pushes normal to a surface. Equal pressures on opposite faces can produce large forces that cancel.

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Try

At the liquid surface the gauge reads zero. Does that mean neither side of a panel experiences a pressure force?

Open the experiment

Predict

At depth 2 m in density 1000 kg/m³, predict the downward liquid force, upward gas force and net pressure force on the 0.020 m² panel.

Experiment

Compare the two face forces and their difference at 2 m and at zero depth. Increase density at fixed depth and identify which force changes. Capture a nonzero net load and explain the required support reaction.

Measure pressure below a liquid surface

Worked teaching model · synthetic values · Uniform incompressible liquid at rest, constant teaching g=10 m/s² and surface absolute pressure 100 kPa. A thin horizontal 0.020 m² panel has liquid above and a separate gas compartment held at 100 kPa below. The panel remains supported at the selected depth. Panel weight, thickness, deformation, surface tension and flow are omitted. Depth zero is the surface limit. Density settings are ideal values, not identified substances.

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Static pressure on two sides · schematic, panel thickness not to scale0 m1 m2 m3 m4 mSurface: 100 kPaLiquid: 120.0 kPaGas below: 100 kPaPanel area: 0.020 m²Depth is measured vertically downward. The box represents a separate gas compartment.
Pressure (kPa) · blue: absolute · dashed: gauge0408012016001234Depth below surface (m)
Pressure references and opposing panel forces
QuantityValue
Gauge pressure at selected depth20.000 kPa
Absolute liquid pressure120.000 kPa
Compartment absolute pressure100.000 kPa
Liquid force on upper face2400.0 N downward
Gas force on lower face2000.0 N upward
Net pressure force400.0 N downward

A hypothetical liquid column with this area and depth has mass 40.0 kg and weight 400.0 N. Its weight explains the pressure increment; it is not an extra force to add to the liquid pressure force. The panel needs an opposing support force; its motion and strength are not modeled.

Gauge pressure 20.000 kPa; absolute pressure 120.000 kPa.

Liquid pushes down with 2400.0 N; compartment gas pushes up with 2000.0 N. Net pressure force 400.0 N downward. Equal pressure contributions on opposite sides cancel in net force, not in absolute pressure.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

A zero gauge reading can hide two large forces

At the free surface the model’s gauge pressure is zero. Predict whether this means a panel there experiences no pressure force on either face. Gauge pressure describes a difference from a reference; it does not erase the physical pressure represented by that reference.

The experiment uses a thin horizontal panel of area 0.020 m². Liquid pushes on its upper face. A separate gas compartment beneath it is held at an absolute pressure of 100 kPa, equal to the pressure at the liquid’s free surface. The panel remains supported at the selected depth. Its weight, thickness, deformation and motion are omitted. The box in the diagram identifies the compartment; its width does not determine the stated area.

Distinguish the pressure references

Absolute pressure uses a vacuum reference. Gauge pressure here means liquid absolute pressure minus the specified 100 kPa reference. p_absolute = p_gauge + p_reference. Both are legitimate readings when their reference is stated. OpenStax measuring pressure distinguishes these conventions and the role of a reference pressure.

At depth 2 m and density 1000 kg/m³, the liquid has 20 kPa gauge pressure and 120 kPa absolute pressure. The compartment gas has 100 kPa absolute pressure and zero gauge pressure relative to the same reference. The pressure difference across the panel is 20 kPa.

If the compartment pressure were changed independently, the net panel load would change even with the same liquid depth and density. The current widget fixes this compartment pressure. Treating it as an arbitrary unknown would make gauge pressure alone insufficient to determine the net load.

Calculate each face force

For uniform pressure on a flat face, F = pA, with p in Pa and A in m², gives force magnitude in N. Pressure pushes normal to each face: the liquid force is downward, while the gas force on the lower face is upward.

At the default setting, the liquid force is 120000 Pa × 0.020 m² = 2400 N downward. The gas force is 100000 Pa × 0.020 m² = 2000 N upward. Choosing downward positive, the net pressure force is 2400 − 2000 = 400 N downward.

The equivalent calculation uses the pressure difference: (120000 − 100000) × 0.020 = 400 N. Here gauge pressure times area gives the same answer because the opposite face is at the gauge reference pressure. That shortcut is conditional, not a universal rule for every two-sided surface.

Check the force ledger before reading the summary. A correct liquid force of 2400 N is still an incorrect net-force answer if the opposing gas force is omitted. Pressure and force also have different units: a result in kPa cannot be called a force in newtons.

Use the surface limit as a check

Set depth to zero. Both absolute pressures are 100 kPa. Each face experiences a force of magnitude 2000 N, but the forces oppose and the net pressure force is zero. This example distinguishes zero resultant force from absent interactions.

Now increase depth to 4 m at density 1000 kg/m³. Liquid absolute pressure becomes 140 kPa, the downward liquid force 2800 N and the net pressure force 800 N. The upward gas force remains 2000 N. Capture both depths and identify exactly which force changes.

At fixed depth, increasing density changes the liquid pressure and force but not the prescribed gas pressure. The hypothetical liquid column above a panel-sized area has weight ρAhg, equal to the net pressure force in this specific arrangement. That column weight explains the pressure increment; it is not an additional load to add again to the already calculated liquid pressure force.

Separate load from motion and strength

Because the panel is held in place, its support must supply a force opposing the net pressure force, in addition to any omitted weight in a real design. A net pressure load does not by itself give the panel’s acceleration or establish whether it will bend or fail. Those questions require mass, material properties, geometry and a support model.

The horizontal-panel condition makes pressure uniform over the face at a single depth. A tall vertical panel spans different depths; its pressure varies across the area. One must account for that variation to find total force and its point of action. Multiplying the deepest pressure by the full area generally overestimates the resultant. This lab does not calculate bending moments or a center of pressure.

Transfer to a different compartment pressure

A horizontal panel has area 0.030 m², liquid absolute pressure 150 kPa above and gas absolute pressure 110 kPa below. Calculate each face force and the net pressure force. A nearby gauge is referenced to 100 kPa; explain why its reading times area would give the wrong net load.

Check the pressure force transfer

The liquid pushes down with 150000 × 0.030 = 4500 N; the gas pushes up with 110000 × 0.030 = 3300 N. Net pressure force is 1200 N downward. The gauge reads 50 kPa, but multiplying that by area gives 1500 N because its 100 kPa reference is not the actual 110 kPa pressure on the other face. Use the actual pressure difference of 40 kPa.

Apply

Liquid pressure is 120 kPa above a 0.020 m² panel; gas below is at 100 kPa. The net pressure force is:

Public practice checks a specific claim. It does not establish independent mastery.

Explain when gauge pressure times area gives the net force and why the other-side pressure must be known. Distinguish a pressure load from a structural strength or motion prediction.

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