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CELE Hydraulics & Fluid MechanicsRelative Equilibrium of LiquidsCheat Sheet

A printable cheat sheet for Relative Equilibrium of Liquids, built for CELE reviewers who want one go-to reference in the final stretch. Covers formulas, key definitions, common question types, and the Professional Regulation Commission (PRC) — Board of Civil Engineering-specific twists you will see on CELE day.

Exam context

On the CELE 2026, the Hydraulics & Fluid Mechanics subtest carries a "Core" weight in Professional Regulation Commission (PRC) — Board of Civil Engineering's pattern. Relative Equilibrium of Liquids lands at position 4th out of 10 in the standard review order. Target score is 70% weighted average, no sub-test below 50%, and roughly a meaningful share of items come from Hydraulics & Fluid Mechanics on a typical CELE paper.

Relative Equilibrium of Liquids - Cheat Sheet

Your final 30-minute reference for relative equilibrium problems: horizontal acceleration, vertical acceleration, rotation, and pressure distribution. Master the three core scenarios and their formulas.

Sections

Formulas

Formula

tan θ = a/g

Meaning

θ = angle of free surface tilt from horizontal; a = horizontal acceleration (m/s²); g = 9.81 m/s²

Watch Out

Surface slopes DOWN in the direction of acceleration. If a/g > 1, θ > 45° (steep slope). Never use sin or cos—only tangent.

When To Use

Tank or container accelerating horizontally; find surface slope angle

Formula

p = γ h_v

Meaning

p = pressure (kPa); γ = unit weight of water ≈ 9.81 kN/m³; h_v = vertical depth below tilted surface

Watch Out

Pressure depends on VERTICAL depth below the tilted surface, not normal to surface. Misidentifying h_v causes major errors.

When To Use

Calculate pressure at any point after finding the tilted surface orientation

Formula

h_rise = (a/g) × L_horizontal

Meaning

Rise of surface at one end of tank; L = horizontal distance traveled along tank length

Watch Out

This is a derived relation—use tan θ and geometry. Not all problems ask for this directly.

When To Use

Find how much higher the surface is at one end vs. the other in a rectangular tank

Common Values

Value

9.81 m/s²

Symbol

g

Quantity

Gravitational acceleration

Value

9.81 kN/m³

Symbol

γ

Quantity

Unit weight of water (fresh)

Value

10.05 kN/m³

Symbol

γ_salt

Quantity

Unit weight of water (salt, approximate)

Section Title

Horizontal Acceleration (Linear Motion)

Important Facts

  • Free surface remains a plane in horizontal acceleration (no curvature).
  • Pressure is hydrostatic relative to the tilted surface: p = γ × (vertical depth below surface).
  • The lowest point of the surface is in the direction OPPOSITE to acceleration.
  • In a closed tank, pressure increases in the direction of acceleration.
  • The depth at one end rises by h_rise = (a/g) × L while the other end drops by the same amount (if tank is symmetric).
  • Maximum acceleration before spillage: a_max occurs when surface reaches tank rim at steepest corner.
  • For a = 0 (no acceleration), θ = 0—surface is horizontal, normal hydrostatic pressure applies.

Key Definitions

Term

Relative Equilibrium

Example

Water in an accelerating truck bed—no slosh, just tilted surface.

Definition

Liquid moving as a rigid body with zero relative motion between particles; no shear stress; free surface adjusts to new shape.

Term

Free Surface Tilt Angle (θ)

Example

a = 2 m/s², g = 9.81 m/s² ⟹ θ = arctan(2/9.81) ≈ 11.5°

Definition

Angle between tilted liquid surface and horizontal plane during horizontal acceleration.

Term

Effective Gravity

Example

Horizontal acceleration creates an apparent sideways gravity component.

Definition

In a non-inertial frame, the combination of true gravity and pseudo-force due to acceleration.

Diagrams To Know

  • Tilted free surface in rectangular tank showing angle θ from horizontal
  • Pressure distribution diagram showing iso-pressure lines perpendicular to tilted surface
  • Tank end-view showing liquid height difference from front to back

Formulas

Formula

p = γ h (1 + a/g) [upward acceleration]

Meaning

p = gauge pressure; a = upward acceleration; h = vertical depth; + sign for upward

Watch Out

Sign: +a for upward. Pressure > γh. If a = g (free fall down), use p = γ h (1 − 1) = 0 gauge pressure.

When To Use

Container accelerating upward (elevator going up, rocket launch); pressure increases

Formula

p = γ h (1 − a/g) [downward acceleration]

Meaning

p = gauge pressure; a = downward acceleration; − sign for downward

Watch Out

Sign: −a for downward. When a/g = 1 (free fall), p = 0 everywhere (liquid feels weightless).

When To Use

Container accelerating downward; pressure decreases

Formula

Effective gravity: g_eff = g ± a

Meaning

g_eff = effective gravitational acceleration felt by liquid

Watch Out

Not usually written this way in exams, but helps intuition: pressure ∝ effective weight.

When To Use

Conceptual understanding; pressure scales as γ_eff × h = γ(g_eff/g) × h

Formula

Free surface remains horizontal

Meaning

No tilt—surface stays parallel to ground even during vertical acceleration

Watch Out

Easy to confuse with horizontal acceleration. Vertical ⟹ horizontal surface; horizontal ⟹ tilted surface.

When To Use

Sketch diagrams: surface is always horizontal, only pressure changes with depth

Common Values

Value

9.81 m/s²

Symbol

g

Quantity

Gravitational acceleration

Value

1–2 m/s²

Symbol

a_elev

Quantity

Typical elevator acceleration (upward)

Value

9.81 m/s² (downward)

Symbol

a_ff

Quantity

Free-fall acceleration

Section Title

Vertical Acceleration (Up or Down)

Important Facts

  • Free surface stays HORIZONTAL during vertical acceleration—never tilts.
  • Upward acceleration (a > 0): effective gravity increases ⟹ pressure increases faster with depth.
  • Downward acceleration (a < 0): effective gravity decreases ⟹ pressure increases slower with depth.
  • At a = g (free fall): gauge pressure = 0 everywhere (liquid and container are weightless relative to each other).
  • Pressure always increases linearly with vertical depth in the accelerating frame.
  • In an elevator: at rest, p_bottom = γ h; accelerating up, p_bottom = γ h (1 + a/g); accelerating down, p_bottom = γ h (1 − a/g).
  • For closed tanks, the gas pressure above the liquid adjusts if the liquid depth is constant (fixed volume).

Key Definitions

Term

Free Fall (Special Case)

Example

Astronaut in orbit or a dropped bucket; water exerts no force on container walls (zero normal force).

Definition

Downward acceleration a = g; the liquid and container fall together; gauge pressure everywhere = 0.

Term

Effective Unit Weight

Example

Upward a = 5 m/s²: γ_eff = 9.81(1 + 5/9.81) ≈ 14.9 kN/m³

Definition

γ_eff = γ(1 ± a/g), the apparent weight per unit volume in the accelerating frame.

Term

Gauge Pressure vs Absolute Pressure

Example

Water 2 m deep with upward a = 3 m/s²: gauge p = 27.6 kPa; absolute ≈ 128.6 kPa.

Definition

Gauge = pressure above atmospheric (used in this chapter); Absolute = gauge + atmospheric ≈ 101 kPa.

Diagrams To Know

  • Vertical cross-section showing horizontal surface with pressure distribution increasing downward faster (upward a) or slower (downward a)
  • Effective gravity vector diagram showing g and a components combining
  • Free-fall scenario (a = g): liquid floating in container, no pressure

Formulas

Formula

z(r) = (ω² r²) / (2g)

Meaning

z = height of free surface above the lowest point (vertex) at radius r; ω = angular velocity (rad/s); r = radial distance from axis; g = 9.81 m/s²

Watch Out

Must convert rpm to rad/s: ω = (2π N) / 60. Omitting the factor 2 in denominator is a classic error.

When To Use

Open cylinder or vessel rotating about vertical axis; find surface shape at any radius

Formula

z_max = (ω² R²) / (2g)

Meaning

Maximum rise of surface at the rim (radius R) above the vertex (center, lowest point)

Watch Out

R is the OUTER radius of the vessel. If diameter D is given, use R = D/2.

When To Use

Find total rise from center to edge of a circular container

Formula

Paraboloid shape: Free surface is a paraboloid of revolution

Meaning

Surface equation in cylindrical coordinates: z = (ω² r²) / (2g)

Watch Out

Not a cone, not a hemisphere—strictly parabolic. Volume under paraboloid = 0.5 × (cylinder volume).

When To Use

Describe or sketch the rotating liquid surface; always parabolic profile

Formula

V_paraboloid = (1/2) × V_cylinder = (1/2) × π R² h_avg

Meaning

Volume of liquid under paraboloid = half the volume of the cylinder enclosing it

Watch Out

Assumes paraboloid doesn't touch the bottom or overflow. If it does, recalculate with spill/drain condition.

When To Use

Check if liquid spills or to find average depth during rotation

Formula

Pressure: p = γ × h_vertical

Meaning

Pressure at any point = unit weight × vertical depth below curved surface (measured vertically, not radially)

Watch Out

Depth is VERTICAL (downward) from the paraboloid surface, not perpendicular to surface or radial distance.

When To Use

Find pressure at any point in rotating liquid

Common Values

Value

9.81 m/s²

Symbol

g

Quantity

Gravitational acceleration

Value

2π/60 ≈ 0.1047

Symbol

conversion factor

Quantity

Conversion: 1 rpm to rad/s

Value

1000–3000 rpm

Symbol

N_centrifuge

Quantity

Typical centrifuge speed

Section Title

Rotation (Constant Angular Velocity)

Important Facts

  • Rotating liquid forms a paraboloid (parabolic profile), not a cone or cone frustum.
  • The vertex (center, r = 0) is the LOWEST point of the surface.
  • Surface rises quadratically with radius: z ∝ r² (doubling r → 4× rise).
  • Volume of rotating liquid = 0.5 × volume of the enclosing cylinder (conserved).
  • Pressure is hydrostatic: depends only on vertical depth below the curved surface.
  • Isobar (constant-pressure) surfaces are also paraboloids (rotated versions of the free surface).
  • If the paraboloid reaches the bottom (z at center < 0), liquid at the center is exposed (exposed axis condition).
  • If the paraboloid exceeds the rim, liquid spills (need to recompute with reduced liquid volume).
  • In the rotating frame, an effective 'gravity' acts: g_eff combines true gravity g (downward) and centrifugal acceleration ω² r (outward).
  • Particle trajectories in the rotating frame are straight lines perpendicular to effective gravity.

Key Definitions

Term

Paraboloid of Revolution

Example

Coffee in a spinning cup; swirled honey in a bowl.

Definition

3D surface generated by rotating a parabola about its axis; the free surface of a rotating open liquid.

Term

Angular Velocity (ω)

Example

1000 rpm = 1000 × 2π/60 ≈ 104.7 rad/s

Definition

Rate of rotation in radians per second (rad/s); related to rpm by ω = 2πN/60.

Term

Vertex (of Paraboloid)

Example

In a spinning cup, the vertex is the deepest point at the center.

Definition

The lowest point of the rotating free surface, located at the axis of rotation (r = 0).

Term

Rim (of Rotating Vessel)

Example

Edge of a spinning centrifuge tube.

Definition

The outer edge of the container at radius R; where the surface rises to maximum height z_max.

Diagrams To Know

  • Vertical cross-section of rotating cylinder showing parabolic free surface profile
  • Top-view (plan view) showing circles (isobars) at the free surface
  • Cylindrical coordinates (r, θ, z) with paraboloid surface labeled
  • Comparison: vertex (low), rim (high), and center axis
  • Pressure distribution in the vertical plane (parabolic isobars)

Formulas

Formula

Pressure = γ × h_vertical (all scenarios)

Meaning

Fundamental: gauge pressure always equals unit weight times vertical depth below free surface

Watch Out

h is measured VERTICALLY (downward), not along the surface or any other direction. This is the #1 source of errors.

When To Use

Any relative equilibrium problem after identifying the free surface shape

Formula

Effective gravity vector: g_eff = √[(g ± a_vertical)² + a_horizontal²]

Meaning

Magnitude of net acceleration in the non-inertial (moving) frame; conceptual only

Watch Out

This is derived thinking—actual exam problems ask for tan θ or pressure directly, not g_eff.

When To Use

Understand why surfaces tilt or curve the way they do (not often used directly in calculations)

Section Title

Pressure Distribution & Special Cases

Important Facts

  • In all relative equilibrium scenarios, the pressure at a point depends only on its VERTICAL distance below the free surface.
  • The free surface is always perpendicular to the direction of effective gravity (g_eff).
  • Horizontal acceleration ⟹ tilted plane surface (perpendicular to g_eff at angle θ).
  • Vertical acceleration only ⟹ horizontal plane surface (no tilt).
  • Rotation ⟹ paraboloid surface (perpendicular to combined g and centrifugal effect).
  • Closed tanks: air pressure above liquid adjusts; gauge pressure at liquid bottom = γ h (1 ± a/g) for vertical acceleration.
  • Open tanks: atmospheric pressure acts on free surface; gauge pressure starts at 0 on the surface.
  • At maximum spillage (tilted surface just reaches a corner or rotating surface just reaches rim/axis), volume of liquid is conserved.

Key Definitions

Term

Non-Inertial (Accelerating) Reference Frame

Example

Inside a braking car, everything 'falls' forward (pseudo-force backward).

Definition

A frame attached to the accelerating container; in this frame, pseudo-forces appear to act on the liquid.

Term

Hydrostatic Assumption in Relative Equilibrium

Example

Pressure p = γ × (vertical distance) applies in the accelerating frame, not the ground frame.

Definition

Even though the container moves, the liquid inside behaves hydrostatically relative to the new orientation—no turbulence or sloshing.

Term

Spillage Condition

Example

Spinning cup too fast ⟹ parabola reaches the axis at center, exposing the bottom; cup tilted too steeply ⟹ one corner runs dry.

Definition

When the free surface (tilted or curved) reaches the rim or bottom of the container, liquid is exposed to overpressure or underpressure.

Diagrams To Know

  • Schematic showing pressure increasing downward (at 90° to free surface normal in all three scenarios)
  • Diagram of spillage: tilted surface hitting the corner; rotating surface exposing the axis
  • Isopressure (isobar) contours in horizontal acceleration (parallel lines perpendicular to θ)
  • Isopressure contours in rotation (concentric circles above the paraboloid)

Section Title

Board Exam Strategy & Problem-Solving Flow

Important Facts

  • Step 1: Identify the motion type — horizontal, vertical, or rotational?
  • Step 2: Sketch the free surface (plane tilted at angle θ, horizontal, or paraboloid).
  • Step 3: Find the shape parameter (θ, ω, or a) using the given acceleration.
  • Step 4: Locate the point of interest (depth, radius, height).
  • Step 5: Calculate vertical distance from point to free surface.
  • Step 6: Apply p = γ × h_vertical.
  • For spillage problems: set surface at rim (max z_max) or axis (min z at center = 0); solve for ω or a.
  • For closed tanks: consider gas pressure above liquid in addition to liquid pressure.
  • For combined motions (e.g., horizontal + vertical): apply superposition carefully—use vector addition of accelerations.

Must Remember

  • 1. HORIZONTAL ACCELERATION: Surface tilts at angle tan θ = a/g DOWN in direction of acceleration. Pressure = γ × vertical depth below tilted surface. Never use sine or cosine—only tangent.
  • 2. VERTICAL ACCELERATION UP: Pressure increases as p = γ h (1 + a/g). Free surface stays HORIZONTAL—no tilt. Effective gravity increases.
  • 3. VERTICAL ACCELERATION DOWN: Pressure decreases as p = γ h (1 − a/g). Free fall (a = g) → gauge pressure = 0 everywhere. Effective gravity decreases.
  • 4. ROTATION: Free surface is a PARABOLOID z = ω² r² / (2g). Rise at rim = ω² R² / (2g). Convert rpm to rad/s using 2π/60. Pressure depends on vertical depth below the curved surface.
  • 5. PRESSURE RULE (ALL CASES): p = γ × h_vertical, where h_vertical is measured DOWNWARD from the free surface. This is the fundamental rule—never measure along the surface or at an angle.
  • 6. PARABOLOID VOLUME: Volume of rotating liquid = 0.5 × cylinder volume (conserved). If paraboloid reaches axis or rim, liquid is exposed (spillage condition).
  • 7. CLOSED vs. OPEN TANKS: Open tanks: gauge pressure starts at 0 on surface (atmospheric = reference). Closed tanks: air pressure above liquid must be considered; gauge pressure at bottom = γ h (1 ± a/g) for vertical.
  • 8. SPILLAGE: Tilted surface reaches corner or rim → solve by setting surface height at that location. Rotating surface reaches axis (z_center = 0) or rim (z_rim = tank height) → recalculate with boundary condition.
  • 9. EFFECTIVE GRAVITY CONCEPT: Horizontal a tilts surface perpendicular to combined g and a_horizontal. Vertical a changes magnitude of pressure. Rotation: surface perpendicular to combined g (down) and ω² r (outward).
  • 10. EXAM PITFALLS: Sign errors in vertical acceleration (+a up, −a down); forgetting to convert rpm to rad/s (multiply by 2π/60); measuring depth along surface instead of vertically; confusing which scenario applies. Read carefully: 'tank accelerates horizontally' vs. 'vertically' vs. 'spins.'

Last Minute Tips

  • TIP 1 — Identify the scenario first: Look for keywords 'accelerates horizontally' (tilt), 'accelerates vertically' (no tilt, pressure changes), 'rotates/spins' (paraboloid). This determines which formula family to use—don't guess.
  • TIP 2 — Always draw a rough sketch of the free surface (plane tilted, plane horizontal, or paraboloid) and mark the point where you need pressure. Sketching prevents sign and direction errors and saves time on complex problems.
  • TIP 3 — Double-check units for ω: If given in rpm, convert immediately to rad/s using ω = 2πN/60. Forgetting this factor causes the entire paraboloid calculation to be wrong by a factor ~4 (because it's squared in the formula).
  • TIP 4 — Remember the hierarchy: First find the free surface shape and parameters (θ, a, ω). Then identify the vertical depth of your point of interest below that surface. Only then apply p = γ h. Skipping steps leads to errors.
  • TIP 5 — For spill/boundary problems: If the problem states 'liquid just reaches the rim' or 'just exposes the axis,' that's your boundary condition—set z_max = tank height or z_center = 0, then solve for the unknown (ω or a). Don't over-complicate; use the constraint given.

Comparison Tables

Rows

Values

  • Linear, perpendicular to gravity
  • Tilted plane at angle θ
  • tan θ = a/g
  • p = γ h_vertical
  • a always positive; θ in direction of acceleration

Property

Horizontal Acceleration

Values

  • Linear, parallel to gravity (upward)
  • Horizontal plane (no tilt)
  • p = γ h (1 + a/g)
  • p = γ h (1 + a/g)
  • + sign for upward; pressure increases

Property

Vertical Acceleration (Up)

Values

  • Linear, parallel to gravity (downward)
  • Horizontal plane (no tilt)
  • p = γ h (1 − a/g)
  • p = γ h (1 − a/g)
  • − sign for downward; pressure decreases

Property

Vertical Acceleration (Down)

Values

  • Circular about vertical axis at ω
  • Paraboloid of revolution
  • z(r) = ω² r² / (2g)
  • p = γ × h_vertical (depth below paraboloid)
  • ω in rad/s; always positive; z increases outward

Property

Rotation (Angular)

Columns

  • Scenario
  • Motion Type
  • Free Surface Shape
  • Key Formula
  • Pressure Formula
  • Sign Convention

Table Title

Three Scenarios of Relative Equilibrium: Summary

Rows

Values

  • Horizontal plane
  • p = γ h
  • Standard hydrostatic pressure

Property

At Rest (a = 0, ω = 0)

Values

  • Tilted plane
  • p = γ h_v (h_v = vertical depth at point)
  • Pressure at bottom depends on vertical depth, not slant distance

Property

Horizontal Acceleration a

Values

  • Horizontal plane
  • p = γ h (1 + a/g)
  • Effective gravity increases; pressure amplified

Property

Vertical Acceleration a (up)

Values

  • Horizontal plane
  • p = γ h (1 − a/g)
  • Effective gravity decreases; pressure reduced

Property

Vertical Acceleration a (down)

Values

  • Horizontal plane
  • p = γ h (1 − 1) = 0
  • Gauge pressure zero everywhere; liquid weightless

Property

Free Fall (a = g down)

Values

  • Paraboloid
  • p = γ × (vertical depth from paraboloid to bottom)
  • Depth increases with r; pressure at center may be 0 if parabola touches axis

Property

Rotation ω at rim (r = R)

Columns

  • Condition
  • Surface Shape
  • Pressure at Bottom (depth h)
  • Notes

Table Title

Pressure Comparison: Rest vs. Motion

Rows

Values

  • m/s²
  • 9.81
  • Use 9.81 (or 10 for estimates); standard for PRC exams

Property

g (gravity)

Values

  • kN/m³
  • 9.81
  • Numerically equals g in SI; unit weight of fresh water

Property

γ (water)

Values

  • rad/s
  • ω = 2πN/60 from rpm
  • N in revolutions per minute; multiply by 2π/60 ≈ 0.1047

Property

Angular velocity

Values

  • rad/s
  • 2π/60 ≈ 0.1047 rad/s
  • Common conversion for rotating machinery problems

Property

1 rpm to rad/s

Values

  • kPa or Pa
  • 1 kPa = 1000 Pa
  • Use kPa for typical depths; Pa for very small pressures

Property

Pressure

Values

  • kPa or atm
  • 101.325 kPa ≈ 1 atm
  • Reference for gauge vs. absolute pressure; use 101 for quick calculations

Property

Atmospheric pressure

Columns

  • Quantity
  • SI Unit
  • Value / Conversion
  • Note

Table Title

Common Unit Conversions & Constants

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