CIVL2131 Formulas, Units, Constants and Variables

0.0(0)
Studied by 0 people
call kaiCall Kai
Locked
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/15

encourage image

There's no tags or description

Looks like no tags are added yet.

Last updated 12:59 AM on 6/11/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai
Chat

No analytics yet

Send a link to your students to track their progress

16 Terms

1
New cards

Q=UAQ=UA

Discharge or Volume Flow Rate (m3/s) = Velocity x

2
New cards

F=maF=ma

Force = mass x acceleration

3
New cards

F=ρQΔUF=\rho Q\Delta U

Force = Density (mass/volume) x Flow Rate (m³/s) x Velocity (m/s)

4
New cards
term image

Kinetic Head = Velocity² / 2 * gravity

The height a column of fluid would rise if all it’s kinetic energy were converted into potential energy → Represents the energy a fluid possesses due to its motion.

5
New cards
term image

Pressure Head = Pressure / {rho} * gravity

It’s the pressure that must be overcome to move fluid from one place to another. It is the static head (vertical distance the fluid must be pushed against gravity) + friction head (resistance caused by fluid rubbing against insides of pipes, valves and fittings).

6
New cards
term image

Total Head = Pressure Head + Kinetic Head + Potential Head

7
New cards

τ\tau

Shear Stress

The force per unit area exerted on the fluid by the boundary and vice versa is the shear stress.

<p>Shear Stress</p><p></p><p><em>The force per </em><strong><em>unit area</em></strong><em> exerted on the fluid by </em><strong><em>the boundary</em></strong><em> and vice versa is the </em><strong><em>shear stress</em></strong>.</p>
8
New cards

μ\mu

Dynamic Viscosity, (Ns/m²)

A measure of how easily a fluid flows.

9
New cards

F/A=mudu/dyF/A={mu}\cdot du/dy

Newton’s Law of Viscosity

Fluids that don’t obey this are Non-Newtonian fluids, which change their viscosity depending on amount of force or pressure applied. They act like a fluid at rest and solid when struck or squeezed.

<p>Newton’s Law of Viscosity</p><p></p><p><em>Fluids that don’t obey this are </em><strong><em>Non-Newtonian fluids</em></strong><em>, which change their viscosity depending on amount of force or pressure applied. They act like a fluid at rest and solid when struck or squeezed.</em></p>
10
New cards

σ\sigma

Surface Tension (N/m)

Arises from the elasticity of the surface and causes capillary rise in tubes. (You then have to measure the meniscus (bottom of the round bit))

<p>Surface Tension (N/m)</p><p></p><p><em>Arises from the elasticity of the surface and causes capillary rise in tubes. (You then have to measure the meniscus (bottom of the round bit))</em></p>
11
New cards
term image

Wetted Length

Equating weight of column of fluid to surface tension force acting on wetted length

<p><strong>Wetted Length</strong></p><p></p><p><em>Equating </em><strong><em>weight of column of fluid</em></strong><em> to </em><strong><em>surface tension</em></strong><em> force acting on wetted length</em></p>
12
New cards

Flow Variations

Describes flow variation with time and space

Temporal variation:

  • Steady Flows - Velocity and Depth constant with time

  • Unsteady Flows - Velocity and Depth vary with time

Spatial variation:

  • Uniform - Flow properties constant in flow direction

  • Non-Uniform - Flow properties vary in flow direction

13
New cards

Governing Principles

  • Continuity

  • Momentum

  • Energy

<ul><li><p>Continuity</p></li><li><p>Momentum</p></li><li><p>Energy</p></li></ul><p></p>
14
New cards

Continuity

Conservation of Mass

ρQ1=ρQ2{\rho}Q_1={\rho}Q_2

or for incompressible fluids / no change in density:

Q1=U1A1=U2A2=Q2Q_{1} = U_{1}A_{1} = U_{2}A_{2} = Q_{2}

15
New cards

Momentum

Conservation of Momentum (Newton’s 2nd Law)

Rate of change of momentum = sum of forces

Momentum flux (or rate at which momentum passes through a cross-section) is the mass flow rate x velocity

ρQU=(ρUA)U\rho QU=\left(\rho UA\right)U

  • The rate of change between cross-sections is ρQΔU\rho Q\Delta U

This requires a resultant force F in the direction of motion.
Momentum equation

F=ρQΔU=ρQ(U2U1)\sum F=\rho Q\Delta U=\rho Q\left(U_2-U_1\right)

16
New cards

Energy

Total head (or head), H

Sum of three forms of energy
The energy of a flow is the sum of potential energy, kinetic energy and pressure energy and is conserved if there are no energy losses.

p1+12ρU12+ρgz1=constp_1+\frac12\rho U_1^2+\rho gz_1=constEnergy equation {E}

  • Considers all energy inputs, losses and changes

H=p1ρg+U122g+z1=constH=\frac{p_1}{\rho g}+\frac{U_1^2}{2g}+z_1=constBernoulli equation {B}

  • Simplified version of energy equation that only applies to ideal, frictionless flows where no energy is added or removed

<p>Total head (or head), H</p><p><strong>Sum of three forms of energy</strong><br><em>The energy of a flow is the sum of potential energy, kinetic energy and pressure energy and is conserved if there are no energy losses</em>.</p><p> $$p_1+\frac12\rho U_1^2+\rho gz_1=const$$ ← <strong>Energy equation {E}</strong></p><ul><li><p>Considers all energy inputs, losses and changes</p></li></ul><p></p><p> $$H=\frac{p_1}{\rho g}+\frac{U_1^2}{2g}+z_1=const$$ ← <strong>Bernoulli equation {B}</strong></p><ul><li><p>Simplified version of energy equation that only applies to <em>ideal, frictionless</em> flows where no energy is added or removed</p></li></ul><p></p>