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.
| Symbol | Quantity | Positive means | Negative means | Notes |
|---|---|---|---|---|
| Cm0 | section pitching moment | nose-up | nose-down | Almost every cambered section is negative. A reflexed section is positive, which is what a flying wing needs. Sheets 02, 03. |
| CLt | tail lift coefficient at trim | the tail is lifting | the tail is pushing down | On 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. |
| Cnβ | weathercock stability | stable — it points into the wind | unstable in yaw | Sound practice is roughly +0.04 to +0.10 per radian. Sheet 12. |
| Clβ | dihedral effect | unstable — a sideslip rolls it further in | stable — a sideslip rolls it back level | The 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. |
| n | load factor | lift upward, the usual case | lift downward, inverted or pushing over | The V-n envelope runs to about half the positive limit on the negative side. Sheet 10. |
| Γ | dihedral angle | tips above the root | tips below the root, anhedral | Wing position adds an equivalent ±3°: positive for a high wing, negative for a low one. Sheet 12. |
| Λ | sweep angle | swept back | swept forward | Measured at the leading edge on Sheet 03 and at the quarter chord on Sheet 12, which is stated on both. Sheets 03, 12. |
| static margin | distance from CG to neutral point | stable — the CG is ahead of the neutral point | unstable in pitch | Quoted 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
| Symbol | Means | Unit | Used on |
|---|---|---|---|
| b | wingspan, tip to tip | mm | 01, 03, 10, 11, 12, 13, 14, 16 |
| S | wing reference area | dm² | most sheets |
| AR | aspect ratio, b²/S | — | 01, 03, 04, 06 |
| cr, ct | root and tip chord | mm | 01, 03, 10, 11, 12 |
| λ | taper ratio, ct/cr | — | 01, 03 |
| MAC | mean aerodynamic chord | mm | 01, 03, 07, Reynolds tool |
| Λ | sweep angle | ° | 03, 12 |
| Γ | dihedral angle | ° | 12 |
| Vh, Vv | horizontal and vertical tail volume | — | 03, 11, 12 |
| lt | tail arm, wing to tail quarter chord | mm | 03, 11 |
Mass and loading
| Symbol | Means | Unit | Used on |
|---|---|---|---|
| m | all-up mass | g | 01, 04, 05, 06, 10, 13, 14, 15, 16 |
| W | weight, m × g | N | internal to every sheet |
| W/S | wing loading | g/dm² | 01, 05, 06 |
| g | standard gravity, 9.80665 exactly | m/s² | everywhere |
| n | load factor | — | 10, 14 |
Aerodynamics
| Symbol | Means | Unit | Used on |
|---|---|---|---|
| CL | whole-aircraft or finite-wing lift coefficient | — | most sheets |
| Cl | two-dimensional section lift coefficient | — | 02 |
| CLmax | maximum finite-wing lift coefficient | — | 01, 04, 06, 10, 11, 13, 14, 16 |
| CD0 | parasite drag coefficient, at zero lift | — | 04, 06, 07, 13, 14, 16 |
| k | induced drag factor, 1/(π e AR) | — | 04, 06, 13, 14, 16 |
| e | span efficiency, Oswald | — | 04, 06, 13, 14, 16 |
| Cm0 | section pitching moment at zero lift | — | 02, 03, 11 |
| Re | Reynolds number, ρVL/μ | — | 01, 02, 07, Reynolds tool |
| Cf | skin friction coefficient | — | 07, Reynolds tool |
| L/D | lift-to-drag ratio, the glide ratio | — | 04, 14 |
Stability and control
| Symbol | Means | Unit | Used on |
|---|---|---|---|
| NP | neutral point, as a fraction of MAC | — | 03 |
| SM | static margin, (NP − CG)/MAC | — | 03 |
| Cnβ | weathercock stability derivative | per rad | 11, 12 |
| Clβ | dihedral effect derivative | per rad | 12 |
| ηt | tail dynamic pressure ratio | — | 03, 11, 12 |
| dε/dα | downwash gradient at the tail | — | 03 |
| Ch | control surface hinge moment coefficient | — | 11 |
| pb/2V | roll helix angle | rad | 11 |
| τ | control surface effectiveness, from the chord ratio | — | 11 |
| CLt max | tail lift coefficient at full elevator throw | — | 11 |
| hfwd | forward balance-point limit, fraction of MAC | — | 11 |
| Cnδr | rudder yawing moment derivative | per rad | 11 |
| β | sideslip angle the rudder can trim | ° | 11 |
| ARt, ARv | tailplane and fin aspect ratio | — | 11, 12 |
Propulsion and electrical
| Symbol | Means | Unit | Used on |
|---|---|---|---|
| J | advance ratio, V/(nD) | — | 08 |
| ηp | propeller efficiency | — | 04, 06, 08, 16 |
| T0 | static thrust | N | 08, 13 |
| Vp | pitch speed | km/h | 08, 13 |
| Dp | propeller diameter | mm | 08, 15, Reynolds tool |
| Kv | motor speed constant, no-load rpm per volt | rpm/V | 04 |
| Ri | pack internal resistance | mΩ | 09 |
| C | discharge rate, multiples of capacity per hour | — | 09 |
| Photel | avionics and payload draw — everything that is not the propeller | W | 16 |
| DoD | depth of discharge — how far down the pack is taken | % | 09, 16 |
Atmosphere
| Symbol | Means | Unit | Used on |
|---|---|---|---|
| ρ | air density | kg/m³ | every sheet that touches air |
| μ | dynamic viscosity, from Sutherland | Pa·s | 07, Reynolds tool |
| ν | kinematic viscosity, μ/ρ | m²/s | Reynolds tool |
| a | speed of sound | m/s | 08, Atmosphere tool |
| hρ | density altitude | m | Atmosphere tool, and named on every sheet |
| RH | relative humidity | % | every sheet that touches air |
Performance
| Symbol | Means | Unit | Used on |
|---|---|---|---|
| Vs | stall speed, wings level | km/h | 01, 06, 10, 13, 14, 16 |
| Va | manoeuvre speed | km/h | 10 |
| Vc, Vd | cruise and dive speed | km/h | 10 |
| Vlo | lift-off speed, 1.15 Vs | km/h | 13 |
| ROC | rate of climb | m/s | 06, 16 |
| γ | climb or glide angle | ° | 13, 14 |
| μ | rolling resistance coefficient — not viscosity | — | 13 |
| Vlaunch | speed the aeroplane is released at, thrown or off a bungee | km/h | 13 |
| w | sink rate, power off | m/s | 14, 16 |
| MC | MacCready setting: the climb you expect in the next thermal | m/s | 14 |
| Vxc | cross-country speed over the climb-and-glide cycle | km/h | 14 |
| Vx | crosswind component the rudder can hold on approach | km/h | 11 |
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.