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BPS5234A Chap.1 Governing Equations for Building Airflow

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Chapter 1 of 12 · BPS5234A

Governing Equations for Building Airflow

The balance statements under every simulation

Every airflow result in this course is the numerical solution of a few conservation laws. Mass is neither created nor destroyed, so the air entering a room must leave it or accumulate. Momentum changes only when pressure, viscous stress or a body force such as gravity acts.

Energy is conserved, so heat carried in by supply air, conducted through walls or released by occupants appears as a temperature field.

Species such as carbon dioxide, water vapour and volatile organic compounds are carried and diffused by the air and added or removed at their sources.

Why buildings need the coupling between them

In most building flows density can be treated as constant, which keeps the continuity equation simple. Temperature still matters because warm air rises.

The Boussinesq approximation reconciles the two by allowing density to vary only where it multiplies gravity, so the energy equation feeds a buoyancy force into the momentum equations.

That single link is the difference between a model that can show a stack effect, a thermal plume or displacement ventilation and one that cannot.

One template, many physics

The lecture then shows that every equation has the same anatomy: storage, transport by the flow, diffusion and a source. Only the transported variable, its diffusion coefficient and its source change.

Seeing the template turns equation choice into a design decision, and the course states that decision as a rule: solve only what the governing physics requires.

Isothermal wind studies need flow alone; heated rooms add energy; air quality adds species; rain and aerosols add a particle phase.

What to be able to do

Expect to name the equations a given study needs and justify leaving others out, explain the Boussinesq coupling in words, and recognise the term in the generic equation that carries a particular effect.

These are short-answer skills, and they underpin the justification section of every assignment report.

In this chapter

What this chapter covers

  • 01

    Continuity in integral and differential form

  • 02

    The continuum assumption and the Knudsen number test

  • 03

    Momentum, pressure gradients and body forces

  • 04

    Energy in temperature form and buoyancy coupling

  • 05

    Species and humidity transport with sources

  • 06

    The generic transport equation and equation selection

Worked example · free

Checking that air behaves as a continuum near a louvre

Q [4 marks]. A facade louvre has 10 mm gaps between blades. Taking the mean free path of air molecules as about 68 nanometres, test whether a continuum CFD model is valid in the gaps. The step weighting shown here is an AskSia study allocation and is not a University marking scheme.
Figure 1.1.Figure 1.1. Each balance is activated by a design question rather than by habit. A wind comfort study needs the top two; a displacement ventilation study cannot run without the third. conservation laws mass, momentum, energy continuity momentum energy species turbulence airflow split, infiltration jets, wind, plume rise stratification, comfort CO2, humidity, VOCs mixing, wakes, closure
Figure 1.1. Each balance is activated by a design question rather than by habit. A wind comfort study needs the top two; a displacement ventilation study cannot run without the third.
  • 1Write the Knudsen number as mean free path over the characteristic length.
  • 2Substitute consistent units and evaluate it.
  • 1Compare with the continuum threshold and conclude.
The Knudsen number is the ratio of the molecular mean free path to the characteristic length of the flow, here the gap. In metres, 68 nanometres is 6.8 × 10−8 m and the gap is 0.01 m, so Kn = 6.8 × 10−8 / 0.01 = 6.8 × 10−6. The course treats flow as a continuum when Kn is 0.001 or less, and this value is about 150 times smaller than that threshold, since 0.001 / 6.8 × 10−6 ≈ 147. The continuum equations are therefore valid in the louvre gaps, and the gap size only matters for meshing, not for the physics.
Sia tip — Convert both lengths to metres before dividing; a nanometre slip of three orders of magnitude flips the conclusion.
Glossary

Key terms

Continuity Equation
The statement of mass conservation: whatever builds up inside a volume must have flowed in across its faces.
Knudsen Number
The ratio of molecular mean free path to a characteristic length, used to confirm that air can be treated as a continuum.
Body Force
A force acting on the whole volume of fluid, such as gravity, buoyancy or a fan, rather than on its surface.
Fick's Law
The rule that a species diffuses down its concentration gradient at a rate set by a diffusion coefficient.
Source Term
The part of a transport equation that adds or removes the transported quantity, such as occupant heat or a pollutant emission.
Generic Transport Equation
The single balance of storage, convection, diffusion and source from which every governing equation in the course can be written.
FAQ

Governing Equations for Building Airflow FAQ

Why does a building simulation treat air as incompressible when its density changes with temperature?

The density changes in rooms and streets are only a few per cent, too small to alter mass conservation noticeably. They are kept where they matter, in the gravity term of momentum, through the Boussinesq approximation, so buoyant plumes and stratification still appear while the continuity equation stays simple.

When can the energy equation be switched off?

Only when temperature differences cannot drive or modify the flow, as in a neutral wind study around buildings without heated surfaces. The urban array lab switches gravity off for exactly that reason. Rooms with occupants, equipment, solar gain or fire need energy solved.

What does the generic transport equation add beyond the individual equations?

It shows that heat, momentum, pollutants and turbulence quantities obey the same balance with different coefficients. That is why a single finite volume solver can handle all of them, and why switching physics on or off is a configuration decision rather than a new method.

How is humidity modelled?

As one more species: the water vapour mass fraction is carried by the flow, diffused, and given sources at occupants, wet surfaces, humidifiers and dehumidifiers, with condensation or evaporation at boundaries. It matters for comfort in warm, humid climates.

Is the integral or the differential form the one a solver uses?

A finite volume solver is built on the integral balance applied to each cell, while the differential form describes local behaviour at a point. Both express the same law; the integral form also remains meaningful across discontinuities.

Study strategy

Assessment move

For every working example you meet, write one line listing the equations it needs and one line naming any equation it could drop and why. Doing this before looking at the set-up sheet trains the selection rule that the reports and quizzes keep testing.

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