Saqr ConsultingDesign sheets
Saqr Consulting

Nomenclature & Sign Conventions

What every symbol means, and what its minus sign means
Reference

A signed number is meaningless without the convention behind it. The sheets hand you several, and they do not all mean the same thing by a minus sign. This page says which is which, in one place, so you never have to infer it.

Sign conventions

This is the half of the page that matters. Four of the quantities below are quoted with a sign, and a negative value means something different in each case — for one it is nose-down, for another a download, for a third it is good and for a fourth it is bad. The two shaded rows are the pair that catches people most often, because they sit next to each other on the same sheet and their signs run opposite ways.

SymbolQuantityPositive meansNegative meansNotes
Cm0section pitching momentnose-upnose-downAlmost every cambered section is negative. A reflexed section is positive, which is what a flying wing needs. Sheets 02, 03.
CLttail lift coefficient at trimthe tail is liftingthe tail is pushing downOn a conventional model with a cambered wing it is negative: the tail carries a download and the wing has to make up the difference. Sheet 03.
Cnβweathercock stabilitystable — it points into the windunstable in yawSound practice is roughly +0.04 to +0.10 per radian. Sheet 12.
Clβdihedral effectunstable — a sideslip rolls it further instable — a sideslip rolls it back levelThe opposite sense to the line above, and the single commonest place to get lost. Sound practice is roughly −0.05 to −0.15 per radian. Sheet 12.
nload factorlift upward, the usual caselift downward, inverted or pushing overThe V-n envelope runs to about half the positive limit on the negative side. Sheet 10.
Γdihedral angletips above the roottips below the root, anhedralWing position adds an equivalent ±3°: positive for a high wing, negative for a low one. Sheet 12.
Λsweep angleswept backswept forwardMeasured at the leading edge on Sheet 03 and at the quarter chord on Sheet 12, which is stated on both. Sheets 03, 12.
static margindistance from CG to neutral pointstable — the CG is ahead of the neutral pointunstable in pitchQuoted as a fraction of the mean chord. Sound practice is 5–15% for a tailed model and 2–8% for a flying wing. Sheet 03.

The pair that catches everyone. On Sheet 12 you are given Cnβ and Clβ side by side. Weathercock stability is good when it is positive; dihedral effect is good when it is negative. Both conventions are standard, both are older than any of us, and neither is going to change — so the sheet prints the word as well as the number, and so does this page.

The reason they differ is that they are moments about different axes with a shared right-handed convention behind them, not an inconsistency anyone chose. A yawing moment that turns the nose into the sideslip is positive; a rolling moment that lifts the windward wing is positive, and lifting the windward wing is exactly what you do not want.

Symbols

Grouped by what they are about rather than alphabetically, because that is how you look one up. The last column says which sheets use it, so you can go and see it in context.

Geometry

SymbolMeansUnitUsed on
bwingspan, tip to tipmm01, 03, 10, 11, 12, 13, 14, 16
Swing reference areadm²most sheets
ARaspect ratio, b²/S—01, 03, 04, 06
cr, ctroot and tip chordmm01, 03, 10, 11, 12
λtaper ratio, ct/cr—01, 03
MACmean aerodynamic chordmm01, 03, 07, Reynolds tool
Λsweep angle°03, 12
Γdihedral angle°12
Vh, Vvhorizontal and vertical tail volume—03, 11, 12
lttail arm, wing to tail quarter chordmm03, 11

Mass and loading

SymbolMeansUnitUsed on
mall-up massg01, 04, 05, 06, 10, 13, 14, 15, 16
Wweight, m × gNinternal to every sheet
W/Swing loadingg/dm²01, 05, 06
gstandard gravity, 9.80665 exactlym/s²everywhere
nload factor—10, 14

Aerodynamics

SymbolMeansUnitUsed on
CLwhole-aircraft or finite-wing lift coefficient—most sheets
Cltwo-dimensional section lift coefficient—02
CLmaxmaximum finite-wing lift coefficient—01, 04, 06, 10, 11, 13, 14, 16
CD0parasite drag coefficient, at zero lift—04, 06, 07, 13, 14, 16
kinduced drag factor, 1/(π e AR)—04, 06, 13, 14, 16
espan efficiency, Oswald—04, 06, 13, 14, 16
Cm0section pitching moment at zero lift—02, 03, 11
ReReynolds number, ρVL/μ—01, 02, 07, Reynolds tool
Cfskin friction coefficient—07, Reynolds tool
L/Dlift-to-drag ratio, the glide ratio—04, 14

Stability and control

SymbolMeansUnitUsed on
NPneutral point, as a fraction of MAC—03
SMstatic margin, (NP − CG)/MAC—03
Cnβweathercock stability derivativeper rad11, 12
Clβdihedral effect derivativeper rad12
ηttail dynamic pressure ratio—03, 11, 12
dε/dαdownwash gradient at the tail—03
Chcontrol surface hinge moment coefficient—11
pb/2Vroll helix anglerad11
τcontrol surface effectiveness, from the chord ratio—11
CLt maxtail lift coefficient at full elevator throw—11
hfwdforward balance-point limit, fraction of MAC—11
Cnδrrudder yawing moment derivativeper rad11
βsideslip angle the rudder can trim°11
ARt, ARvtailplane and fin aspect ratio—11, 12

Propulsion and electrical

SymbolMeansUnitUsed on
Jadvance ratio, V/(nD)—08
ηppropeller efficiency—04, 06, 08, 16
T0static thrustN08, 13
Vppitch speedkm/h08, 13
Dppropeller diametermm08, 15, Reynolds tool
Kvmotor speed constant, no-load rpm per voltrpm/V04
Ripack internal resistancemΩ09
Cdischarge rate, multiples of capacity per hour—09
Photelavionics and payload draw — everything that is not the propellerW16
DoDdepth of discharge — how far down the pack is taken%09, 16

Atmosphere

SymbolMeansUnitUsed on
ρair densitykg/m³every sheet that touches air
μdynamic viscosity, from SutherlandPa·s07, Reynolds tool
νkinematic viscosity, μ/ρm²/sReynolds tool
aspeed of soundm/s08, Atmosphere tool
hρdensity altitudemAtmosphere tool, and named on every sheet
RHrelative humidity%every sheet that touches air

Performance

SymbolMeansUnitUsed on
Vsstall speed, wings levelkm/h01, 06, 10, 13, 14, 16
Vamanoeuvre speedkm/h10
Vc, Vdcruise and dive speedkm/h10
Vlolift-off speed, 1.15 Vskm/h13
ROCrate of climbm/s06, 16
γclimb or glide angle°13, 14
μrolling resistance coefficient — not viscosity—13
Vlaunchspeed the aeroplane is released at, thrown or off a bungeekm/h13
wsink rate, power offm/s14, 16
MCMacCready setting: the climb you expect in the next thermalm/s14
Vxccross-country speed over the climb-and-glide cyclekm/h14
Vxcrosswind component the rudder can hold on approachkm/h11

Do the units come out?

Twenty-three of the equations behind these sheets, with everything in them reduced to kilograms, metres, seconds, amperes and kelvin, and the cancellation worked through. It is worth doing once for each of them: an equation whose units do not balance is wrong before any number goes into it, and the commonest error on this site’s subject — putting a mass where a weight belongs — shows up here and nowhere else.

The right-hand column is computed from the dimensions of the symbols, not written: tools/build-dimensions.py multiplies the exponents out, and tools/check-dimensions.py does it again independently and fails on anything that does not land on its left-hand side.

Sheet 01

Wing area

S = c · b

[c] = m [b] = m

which multiplies out to m² — wing area.

The one that needs no arithmetic, and the one everything else is divided by.

Sheet 01

Aspect ratio

AR = b² / S

[b] = m [S] = m²

which multiplies out to 1 — aspect ratio.

A length squared over an area: aspect ratio is a pure number, which is why it compares a glider with an airliner.

Sheet 01

Stall speed

V = √( 2W / (ρ · S · C_L) )

[W] = kg·m·s⁻² [ρ] = kg·m⁻³ [S] = m² [C_L] = 1

the quantities combine to m²·s⁻², and the square root of that is m·s⁻¹ — airspeed.

Weight is a force, not a mass — that is the error this one catches. Put kilograms in where newtons belong and the root returns something that is not a speed.

Sheet 01

Dynamic pressure

q = ½ · ρ · V²

[ρ] = kg·m⁻³ [V] = m·s⁻¹

which multiplies out to kg·m⁻¹·s⁻² (Pa) — dynamic pressure.

Density times a speed squared is a pressure. Every aerodynamic force on the site is this multiplied by an area and a coefficient.

Sheet 01

Lift

L = q · S · C_L

[q] = kg·m⁻¹·s⁻² [S] = m² [C_L] = 1

which multiplies out to kg·m·s⁻² (N) — lift.

Pressure times area is force, and the coefficient carries no dimensions at all — which is the whole reason coefficients exist.

Sheet 13

Reynolds number

Re = ρ · V · L / μ

[ρ] = kg·m⁻³ [V] = m·s⁻¹ [l] = m [μ] = kg·m⁻¹·s⁻¹

which multiplies out to 1 — a pure number.

Four dimensional quantities that cancel completely. A Reynolds number with units on it has been worked out wrongly.

Sheet 13

Reynolds number again

Re = V · L / ν

[V] = m·s⁻¹ [l] = m [ν] = m²·s⁻¹

which multiplies out to 1 — a pure number.

The same number through kinematic viscosity, which is μ/ρ and carries the density already. Two roads, one dimensionless answer.

Sheet 04

Induced drag coefficient

C_Di = C_L² / (π · e · AR)

[C_L] = 1 [e] = 1 [AR] = 1

which multiplies out to 1 — drag coefficient.

Dimensionless throughout. Nothing here can tell you whether π belongs in it — which is the limit of the method.

Sheet 04

Power required

P = D · V

[D] = kg·m·s⁻² [V] = m·s⁻¹

which multiplies out to kg·m²·s⁻³ (W) — power.

Force times speed. The most useful identity on the site: it turns a drag count into watts and a watt-hour into a flight.

Sheet 14

Sink rate

w = V · C_D / C_L

[V] = m·s⁻¹ [C_D] = 1 [C_L] = 1

which multiplies out to m·s⁻¹ — airspeed.

A speed multiplied by a ratio of two dimensionless numbers is still a speed. The glide ratio is that ratio upside down.

Sheet 08

Static thrust

T = ( P · FM · √(2 · ρ · A) )^⅔

[P] = kg·m²·s⁻³ [ρ] = kg·m⁻³ [A] = m²

the quantities combine to kg³·m³·s⁻⁶, and the cube root of that is kg·m·s⁻² (N) — thrust.

The fractional powers are the interesting part: two thirds of a power times a third of a density times a third of an area lands exactly on a force.

Sheet 08

Induced velocity

T = 2 · ρ · A · v_i · (V + v_i)

[ρ] = kg·m⁻³ [A] = m² [V] = m·s⁻¹

which multiplies out to kg·m·s⁻² (N) — thrust.

Momentum flux: density times area times a speed squared is a force. That is the actuator disc in one line.

Sheet 13

Ground roll

s = 1.44 · W² / (g · ρ · S · C_L · F)

[W] = kg·m·s⁻² [g] = m·s⁻² [ρ] = kg·m⁻³ [S] = m² [C_L] = 1 [T] = kg·m·s⁻²

which multiplies out to m — a length.

Two forces on top, and a length comes out. Worth checking by hand: it is the closed form the sheet does not use, and it is easy to drop a factor in.

Sheet 10

Root bending moment

M = (n · W / 2) · y

[n] = 1 [W] = kg·m·s⁻² [l] = m

which multiplies out to kg·m²·s⁻² (N·m) — a moment.

Force times arm. The load factor is a pure number, so it changes the answer without changing what the answer is.

Sheet 10

Spar cap area

A = M / (σ · h)

[M] = kg·m²·s⁻² [σ] = kg·m⁻¹·s⁻² [h] = m

which multiplies out to m² — cap area.

A moment over a stress and a depth. Cap area falls in direct proportion to depth, which the dimensions show before any arithmetic does.

Sheet 10

Tip deflection

δ = ∬ M / (E · I) · dx · dx

[M] = kg·m²·s⁻² [E] = kg·m⁻¹·s⁻² [I] = m⁴ [l] = m

which multiplies out to m — a length.

M/EI is one over a length — a curvature. Integrating it twice along the span is what turns it into a deflection, and the dimensions are why there are two integrations rather than one.

Sheet 11

Hinge moment

H = C_h · q · S_f · c_f

[C_h] = 1 [q] = kg·m⁻¹·s⁻² [S] = m² [c] = m

which multiplies out to kg·m²·s⁻² (N·m) — a moment.

Pressure, area, arm. The chord appears twice — once inside the area and once as the arm — which is why hinge moment goes as the square of the chord fraction.

Sheet 03

Tail volume coefficient

V_H = S_h · l_h / (S_w · MAC)

[S] = m² [l] = m [c] = m

which multiplies out to 1 — a pure number.

An area times a length over an area times a length. Dimensionless, which is what lets one number describe a trainer and a transport.

Sheet 15

Turnover lever

lever = l_s · t / √(4B² + t²)

[l] = m [b] = m

which multiplies out to m — a length.

Length times length over a length. The root adds two squared lengths, so it is a length too — a sum whose terms did not match would be the error to look for.

Sheet 09

Pack energy

E = N · V · Q

[V] = kg·m²·s⁻³·A⁻¹ [Q] = s·A

which multiplies out to kg·m²·s⁻² (N·m) — energy.

Volts times coulombs is joules. A milliamp-hour is a charge with the hours hidden in it, which is why watt-hours and amp-hours are not interchangeable.

Sheet 09

Voltage sag

ΔV = I · R

[I] = A [R] = kg·m²·s⁻³·A⁻²

which multiplies out to kg·m²·s⁻³·A⁻¹ (V) — voltage.

Current times resistance is a voltage. Everything the battery sheet says about sag rests on this one line.

Sheet 09

The current quadratic

R·I² − V·I + P = 0

[R] = kg·m²·s⁻³·A⁻² [I] = A

which multiplies out to kg·m²·s⁻³ (W) — power.

Every term is a power: I²R, VI and P alike. That is what makes it a quadratic in current rather than a division, and it is a dimensional argument before it is an electrical one.

Sheet 13

Air density

ρ = p / (R · T)

[p] = kg·m⁻¹·s⁻² [R] = m²·s⁻²·K⁻¹ [T] = K

which multiplies out to kg·m⁻³ — air density.

The specific gas constant carries the temperature away and leaves a density. Its own units — J per kilogram per kelvin — are what make that work.

One name, one meaning

The short names in the address bar are part of this vocabulary too. When you move between sheets your figures travel in the query string, and a name means the same thing on every sheet in the set — cl is always the finite-wing maximum lift coefficient, never a cruise value, and cl2 is the two-dimensional section figure that would otherwise be confused with it.

That rule exists because it was broken once. A sheet was briefly written to read cl into its cruise lift coefficient; every value arrived correctly and every value was wrong, and the handoff test passed throughout, because it checks arrival rather than meaning. A sheet that wants a quantity nobody else publishes takes a new name, not a near-enough one.

Notation

Metric on the wire. Whatever units a sheet displays, every figure that travels between sheets is metric — millimetres, grams, square decimetres, km/h, newtons. The unit converter carries every pair the sheets use, with the exact factors.

Angles are degrees on the page and radians in the code. Anything you type or read is in degrees. The stability derivatives are the exception and are quoted per radian, as the literature quotes them; multiply by 0.01745 for per degree.

μ is two different things and there is no avoiding it: dynamic viscosity in anything to do with Reynolds number, and rolling resistance on Sheet 13. They never appear on the same page.

Spelling is British — aeroplane, metre, colour, licence, modelling. The one deliberate exception is airfoil, which is what the sections are called in every source the sheets cite.

Where the methods are

This page is the vocabulary. The methods themselves — every formula, its source, and where it stops being valid — are set out per sheet in the repository's CALCULATIONS.md, and each sheet carries its own scope statement saying what it does not model. About the set says where the methods come from.