The Hong Kong Polytechnic UniversityDepartment of Aeronautical and Aviation Engineering

THE SOUND BARRIER, WITHOUT A THROAT

Compressible Ducts

Two different processes. One sonic limit.

ANALYTICAL 1D MODELConstant area · fixed inlet · perfect gas
WALL FRICTION

Friction can accelerate a gas.

A subsonic stream gains speed as friction lowers its pressure. A supersonic stream slows. Both move towards Mach 1.

MASS FLOW · CONSTANTTOTAL TEMPERATURE · CONSTANTENTROPY · NON-DECREASING
CONSTANT-AREA SECTIONGeometry shown schematically
Mach number

01

Solving…

Exit Mach—At x / L = 1
Total-pressure change—Inlet to exit
Total-temperature change—No heat added
Mass flow—Fixed by inlet and diameter

Preparing the visual time scale…

FOLLOW THE SAME STATION THROUGH EVERY CURVE

One flow, several signatures.

B · liveA · frozenSolid: static / dashed: total

01 / MACH NUMBER

Moving towards sonic flow

Swipe the chart sideways, or focus it and use the arrow keys.

The dotted horizontal line is M = 1. A smooth branch ends there; it does not cross to the other side.

02 / STATIC AND TOTAL PRESSURE

A pressure rise can hide a loss

Swipe the chart sideways, or focus it and use the arrow keys.

Static pressure can rise in a supersonic duct while total pressure falls. Each pressure is normalised by its own inlet value.

03 / STATIC AND TOTAL TEMPERATURE

Temperature is not total energy

Swipe the chart sideways, or focus it and use the arrow keys.

Friction redistributes static enthalpy and kinetic energy. The adiabatic duct retains its total temperature.

04 / ENTROPY

The approach to a limiting state

Swipe the chart sideways, or focus it and use the arrow keys.

Entropy is measured from each case’s inlet. The maximum on this branch occurs at M = 1.

Checking mass and energy consistency…

OBSERVE

Watch the inlet branch.

Compare the subsonic and supersonic presets. Friction always opposes motion, but the compressible pressure and density response determines whether speed rises or falls.

CHANGE

Find the boundary.

Choose “Sonic at exit”, then “Beyond the limit”. The hatched section has no continuation on this fixed-inlet branch. The solver does not silently change the inlet or insert a shock.

EXPLAIN

Separate energy from pressure.

Freeze a case as A, then change the loading in B. Total temperature stays fixed in Fanno flow, while irreversible friction reduces total pressure. “Energy conserved” does not mean “isentropic”.

READ THE BOUNDARY OF THE MODEL

Equations, assumptions and evidence.

These are steady one-dimensional analytical states. Moving tracers illustrate an already solved flow; they are not a time-dependent CFD simulation.

Mass and energy

ρu=G=constantcpT0=cpT+u22

A fixed inlet determines mass flux. A subsonic or supersonic branch is selected explicitly.

Fanno · adiabatic wall friction

F(M1)−F(M)=fDxDdp+ρudu+fDρu22Ddx=0

F(M) is the remaining friction exposure to sonic flow. At the limit, fDL*/D = F(M₁). The Darcy factor is four times the Fanning factor.

Static and stagnation properties

p0=p(1+γ−12M2)γγ−1Δs=cplnTT1−Rlnpp1

Stagnation pressure is the pressure reached by a hypothetical local isentropic deceleration. It is not the duct’s static pressure.

What this model includes

Steady flow of a calorically perfect gas; circular constant-area duct; cross-section averages; no shaft work; one effect at a time. Air constants are γ = 1.4, R = 287.05 J kg⁻¹ K⁻¹ and cₚ = 1004.675 J kg⁻¹ K⁻¹.

The limit applies to the specified inlet, not to every possible flow through the same pipe. A real system may change inlet mass flow, develop shocks or become unsteady.

What remains outside it

Friction and heat are not combined. Boundary layers, entrance losses, variable heat capacity, chemistry, heat-transfer coefficients, wall temperature and shock location are omitted. A high-temperature warning marks where the constant-air-property approximation becomes less representative.

Analytical and numerical consistency checks do not establish experimental accuracy or suitability for engineering design.

Sources, implementation and verification record

The equations were independently implemented from conservation laws and checked against university teaching references. All diagrams are original. No third-party software or figure has been bundled.

Model ledger and equations · Source scope and attribution · Recorded analytical checks · JSON

Recorded checks include 29,160 sampled states, mass and energy closure, Rayleigh momentum, Fanno wall-shear momentum, an independent Rayleigh quadratic, and Fanno differential-equation refinement. See the record for tolerances and scope.