More than one input

The steps are not free

A gearbox is supposed to have equal steps between its gears, so that the engine returns to the same speed after every shift. A gearset has one or two numbers to spend on three or four gears, so from the third one the steps are a consequence rather than a choice — and asking for them to be equal turns out to be a quadratic whose root is the golden ratio, realised in tooth counts by consecutive Fibonacci numbers.

Assumes Four speeds from two numbers.

There is a design rule about gearbox ratios that everybody states and nobody quite justifies in the same words. The steps between the gears should be equal in ratio, so that a shift always drops the engine by the same proportion and the driver — or the controller — is always handed back the same operating point. Equal ratios between consecutive gears means the ladder is a geometric progression, and the number quoted for a gearbox, its spread, is the top gear divided by the bottom one.

It is a good rule. It is also, for a planetary automatic, mostly unavailable, and the reason is the reduction from the previous essay: the ladder is a function of one or two numbers. A three-speed Simpson gearbox has one proportion to spend on three gears. A four-speed Ravigneaux has two to spend on four. Choose the ends and the middle is decided.

The steps, against the ones the rule asks for. The design rule everybody quotes is that the steps between gears should be equal in ratio, so that the engine returns to the same speed after every shift. That makes the sequence geometric, and the ideal step for this spread over this many gears is 1.5324, marked. The steps a gearset actually gives are not free: the whole sequence is a function of the tooth counts, so once the top and bottom are chosen there is nothing left to spend on the middle. The worst step here is off the ideal by 10.8%.
Fig. 1 The three steps of the four-speed from the previous essay, against the equal step its own spread and gear count ask for. The bottom step is 1.699 where the ideal is 1.532 — 10.8% too big — and the other two are almost exactly equal to each other and both too small. Nobody chose that shape; it is what 2.48 and −2.22 left over.

How much is actually chosen

Work the accounting through explicitly, because it is the whole argument.

A Ravigneaux’s ratios, with K1K_1 and K2K_2 the two ring-over-sun proportions, are 1+K21+K_2, 1+K2/K11+K_2/K_1, 11, and 11/K11-1/K_1. Four gears; two parameters; and the third gear is 1 whatever anyone does, because direct drive is a clutch and a clutch does not know about tooth counts.

So really there are two free numbers and two free gears, and the other two are determined. Ask for first at 2.48 and K2=1.48K_2 = 1.48 is fixed. Ask for reverse at −2.22 and K1=3.22K_1 = 3.22 is fixed. Second is now 1.461.46 and the overdrive is 0.6890.689, and it does not matter in the slightest what anybody thinks of them.

The three steps that come out are

2.481.46=1.699,1.461.00=1.460,1.000.689=1.451,\frac{2.48}{1.46} = 1.699, \qquad \frac{1.46}{1.00} = 1.460, \qquad \frac{1.00}{0.689} = 1.451,

against a spread of 3.598, which over three steps asks for 3.5981/3=1.53243.598^{1/3} = 1.5324 each. The bottom step is 10.8% too large and the top two are about 5% too small, and no amount of re-cutting the gears inside this arrangement moves the shape — only where the whole ladder sits.

A Simpson three-speed is worse off still, having one number for two steps. Its ladder is 2+1/K2+1/K, 1+1/K1+1/K, 11, and the steps are

2K+1K+1andK+1K.\frac{2K+1}{K+1} \quad\text{and}\quad \frac{K+1}{K} .

At K=74/34K = 74/34 that is 1.6852 and 1.4595, against an ideal of 1.5683 — 7.5% and 6.9% out, in opposite directions.

Asking for equal steps is a quadratic

Since the steps are functions of KK, “make them equal” is not a design goal but an equation. For the Simpson:

2K+1K+1=K+1K    K(2K+1)=(K+1)2    K2K1=0,\frac{2K+1}{K+1} = \frac{K+1}{K} \;\Longrightarrow\; K(2K+1) = (K+1)^2 \;\Longrightarrow\; K^2 - K - 1 = 0,

whose positive root is

K=1+52=φ=1.6180K = \frac{1+\sqrt5}{2} = \varphi = 1.6180\ldots

The golden ratio, arriving unbidden out of a gearbox. And it is not a coincidence of that arrangement: doing the same for the Ravigneaux’s three steps, with u=1+K2/K1u = 1 + K_2/K_1, gives u2u1=0u^2 - u - 1 = 0, the same quadratic, so u=φu = \varphi, K2=φK_2 = \varphi and K1=φ2K_1 = \varphi^2. The four ratios then come out as

φ2:φ:1:φ1  =  2.618:1.618:1.000:0.618,\varphi^2 : \varphi : 1 : \varphi^{-1} \;=\; 2.618 : 1.618 : 1.000 : 0.618,

with a spread of φ3=4.236\varphi^3 = 4.236 and every step exactly φ\varphi. Reverse, which was not asked to join in, is (K11)=φ-(K_1-1) = -\varphi.

The reason φ\varphi shows up is not mysterious once it is written down. The ladders are built from expressions of the form one plus a reciprocal, and the fixed point of “one plus a reciprocal” is the equation that defines the golden ratio. Any gearset whose members compose that way will produce it.

The tooth counts are Fibonacci numbers

φ\varphi is irrational and a ratio of tooth counts is not, so the question is how close the integers get. The best rational approximations to φ\varphi are ratios of consecutive Fibonacci numbers, and that is what the gearsets are:

  • a Simpson with a sun of 55 in a ring of 89. K=89/55=1.61818K = 89/55 = 1.61818, planets of 17, ladder 2.61798:1.61798:1.0002.61798 : 1.61798 : 1.000, and the two steps are 1.61806 and 1.61798 — different from each other by 0.0024%, or one part in forty thousand.
  • a Ravigneaux with suns of 34 and 55 in a ring of 89. K1=89/34K_1 = 89/34, K2=89/55K_2 = 89/55, long planets of 17, and the four ratios 2.61818:1.61818:1.00000:0.617982.61818 : 1.61818 : 1.00000 : 0.61798, whose three steps differ by 0.0084%.
The steps, against the ones the rule asks for. The design rule everybody quotes is that the steps between gears should be equal in ratio, so that the engine returns to the same speed after every shift. That makes the sequence geometric, and the ideal step for this spread over this many gears is 1.6181, marked. The steps a gearset actually gives are not free: the whole sequence is a function of the tooth counts, so once the top and bottom are chosen there is nothing left to spend on the middle. The worst step here is off the ideal by 0.0%.
Fig. 2 The same three steps for the Fibonacci gearset. Every bar is on the dashed ideal to within a hundredth of a per cent, and the ideal is φ. The ratios are exact fractions of Fibonacci numbers — 34/89, 55/89, 89/144 — because the ladder was never told about φ; it was told about 34, 55 and 89.

Two things are worth checking before this becomes a party trick, and both check out.

It assembles. A sun of 55 and a ring of 89 add to 144, which is divisible by 3 and by 4, so the gearset takes three or four equally spaced planets; the planets are 17 teeth, comfortably above the undercut limit, and they clear each other with room to spare. The assembly conditions are the ones that kill most nice-looking tooth counts, and these survive them.

The ratios are usable. 2.62 : 1.62 : 1.00 : 0.62 with a spread of 4.24 is an entirely ordinary four-speed ladder — deeper than some, taller than others, nothing out of range.

The sequence of speeds, and the geometric one it is not. The reductions on a logarithmic axis, so equal steps would be a straight line. The dashed line is the geometric sequence with the same top, bottom and number of gears — the one the design rule asks for — and the marks are what the gearset gives. They are not the same, and they cannot be made the same by choosing the tooth counts differently: a gearset has far fewer numbers to spend than it has gears, so from the third one on the sequence is a consequence rather than a choice. The largest departure is 0.0%.
Fig. 3 The Fibonacci Simpson’s ladder on a logarithmic axis, where equal steps are a straight line. The marks and the dashed geometric ideal are indistinguishable, which is the point: at K = 89/55 the two coincide to four decimal places, and the departure from the rule is smaller than the difference between two adjacent tooth counts.

Two of the seven ratios coincide there

The golden gearset is a single point in the plane of the two proportions, and something happens to the Ravigneaux’s full ledger at that point which does not happen anywhere else in it.

The seven exact ratios are 1+K21+K_2, 1+K2/K11+K_2/K_1, 11, 11/K11-1/K_1, (K11)-(K_1-1), 1+K1/K21+K_1/K_2 and 1+1/K21+1/K_2. Equal steps forced K2=φK_2 = \varphi and K1=φ2K_1 = \varphi^2, and φ2=φ+1\varphi^2 = \varphi + 1, so every one of those expressions collapses onto a power of the golden ratio. The first becomes 1+φ=φ21+\varphi = \varphi^2. The sixth becomes 1+φ2/φ=1+φ=φ21 + \varphi^2/\varphi = 1 + \varphi = \varphi^2 as well. The second becomes 1+φ/φ2=1+1/φ=φ1 + \varphi/\varphi^2 = 1 + 1/\varphi = \varphi, and so does the seventh, 1+1/φ1 + 1/\varphi.

So two pairs of the seven coincide. The gearset has seven ways of being driven and, at this one setting of its proportions, only five distinct ratios among them: φ2\varphi^2, φ\varphi, 11, 1/φ1/\varphi and a reverse of φ-\varphi. Two of the seven arrangements deliver a ratio another arrangement already delivers, which is a degeneracy that exists at no other point in the parameter plane.

The reverse is the neatest of them. (K11)=(φ21)=φ-(K_1 - 1) = -(\varphi^2 - 1) = -\varphi, so the geometric Ravigneaux reverses at exactly the magnitude of its own second gear. That is a real and slightly startling property of a real gearbox layout — reverse and second identical in ratio, differing only in sign — and it is not a coincidence so much as the same identity φ2=φ+1\varphi^2 = \varphi + 1 turning up in a third place.

Nothing about that is a design argument, and it is worth saying so plainly rather than letting the tidiness carry it. Coincident ratios are not useful; a transmission with two ways to produce φ\varphi has a redundancy rather than a feature, and a designer would not pay anything for it. What the coincidence is worth is as a check, and it is a strong one. The seven closed forms were derived independently of the quadratic that produced φ\varphi, so a computation that puts K2=φK_2 = \varphi and K1=φ2K_1 = \varphi^2 into all seven and does not get two coincident pairs has an error in one of the two derivations. That is a test with a sharp verdict and no tolerance in it, arriving free from a fact about the golden ratio.

It also says something about why φ\varphi turns up at all, which the essay above declined to call mysterious and is worth finishing off. The equal-step condition asks for a ladder in which each rung is the same multiple of the last, and the gearset’s forms are built from 1+x1 + x and 1/x1/x shapes. A number that is its own reciprocal plus one is the fixed point of exactly that pair of operations, and there is only one positive such number. The gearbox is not producing the golden ratio because of anything about gears; it is producing it because the ladder’s own recurrence and the gearset’s algebra are the same recurrence.

What a step is for

Before deciding whether the geometric rule is worth obeying, it is worth being precise about what a step does, since the usual justification is stated in a hurry.

An engine has a useful band of speeds. Driving along at a given road speed, the transmission’s ratio decides where in that band the engine sits. Shifting up multiplies the road-speed-to-engine-speed relation by the step, so the engine drops by exactly the step and the driver — or the controller — is handed the engine at a new operating point.

If every step is the same size, then every shift drops the engine by the same proportion, so a single strategy works at every gear: run up to the top of the band, shift, land at the same place, repeat. That is the whole of the argument, and it is exactly the argument for a geometric progression: equal ratios between neighbours means the ladder is r0,r0/s,r0/s2,r_0, r_0/s, r_0/s^2, \ldots

Its assumption is that the engine’s band is the same in every gear and that the object is to stay inside it. Both are true for a truck climbing a hill and for a machine tool cutting at a fixed surface speed; neither is quite true for a car, where the bottom gear is used from rest and the top ones at part throttle.

The sequence of speeds, and the geometric one it is not. The reductions on a logarithmic axis, so equal steps would be a straight line. The dashed line is the geometric sequence with the same top, bottom and number of gears — the one the design rule asks for — and the marks are what the gearset gives. They are not the same, and they cannot be made the same by choosing the tooth counts differently: a gearset has far fewer numbers to spend than it has gears, so from the third one on the sequence is a consequence rather than a choice. The largest departure is 9.8%.
Fig. 4 The four-speed’s ladder on a logarithmic axis, where a geometric progression is a straight line. The marks bow away from the dashed ideal at the bottom, which is where the departure lives — and it is entirely in the first step, the other two being within half a per cent of each other.

So why does nobody build it

This is where the finding has to be handled honestly, because “the mathematically perfect gearbox exists and industry ignores it” is the kind of sentence that is nearly always wrong.

The equal-step rule is not what a transmission engineer is actually trying to achieve, and the departures in real gearboxes are in a consistent direction that says so. Look again at the four-speed measured above: bottom step 1.699, then 1.460 and 1.451. The bottom step is deliberately the biggest and the top steps are deliberately close together. That shape has a name — a progressive ladder — and the reasons for it are about what the gears are for:

  • The bottom gear exists to get a heavy vehicle moving from rest, and how far the engine falls on the shift out of it matters much less than how much torque multiplication it provides. Making first deeper costs almost nothing in driveability.
  • The top gears are used at cruise, where the engine is near its efficient band and where a large step means either revving needlessly or labouring. Close spacing at the top is worth paying for.
  • A torque converter blurs the bottom of the ladder anyway, multiplying torque continuously below its coupling point, which further reduces the value of a precise first-to-second step.

So the geometric ladder is a rule of thumb aimed at a use — hold the engine in a band, all the way up — that fits a truck, a racing car or a machine tool much better than a passenger car. The real result of this essay is not that manufacturers are wrong. It is the structural one: whether a gearbox’s ladder is geometric or progressive, it has at most two numbers in it, so its shape is chosen once for all the gears at once and cannot be tuned gear by gear. What a designer picks is a family, not a list.

And the family that is geometric is a specific point in the parameter plane with a closed form, and the tooth counts nearest to it are Fibonacci numbers. That is worth knowing even if nobody wants to be there, because it says exactly how far from geometric an arrangement is and in which direction.

What it would take to fix

Suppose the geometric ladder were wanted after all. What is the cheapest change to a Ravigneaux four-speed that gets it?

Not re-cutting the gears within the arrangement, because the arrangement’s two numbers are already spent — and this is where the closed forms earn their keep. The equal-step condition fixes K1=φ2K_1 = \varphi^2 and K2=φK_2 = \varphi, and those two numbers then fix first gear at 2.618 and reverse at −1.618, whether anybody wanted them or not. If a designer needs a first gear of 2.9 and a reverse of −2.6, the equal-step ladder is unavailable at any tooth count; there is nothing left to spend.

So the fix is a third number, which means a third proportion, which means another gearset. A simple planetary in front of a Ravigneaux — the arrangement used in most six-speed automatics — brings its own ring-over-sun and takes the design space from two dimensions to three. With three numbers and six gears the ladder is still not free, but there is now enough room to hit a spread, a first gear and a step profile at the same time.

That is a useful way to read the history of automatic transmissions. Three speeds from one number, four from two, six from three: each generation adds a gearset, and what the gearset buys is not gears — those come from clutches — but a degree of freedom in the ladder’s shape.

The lever of a Ravigneaux gearset at the golden ratio. Each member sits at a position on the lever fixed by the tooth counts alone, and its speed is the height of one straight line over that position. The line here is drawn through sun2 and sun1; every other member is plotted where the train's null space puts it, and lands on the line exactly — the residual is zero in rationals, and 2.2e-16 once the coordinates have been rounded to doubles for the drawing. Where the line crosses the axis is the member that is standing still, and that is what a brake does: it pins the line to the axis at one position and leaves it free to pivot there. The planets are on the lever too, off the end of it, which is where they belong — they are members of the train and are not shafts anybody can reach.
Fig. 5 The equal-step gearset’s lever, at Fibonacci coordinates. Its two interior stations are where φ puts them, and moving either of them by one tooth is the whole of the design freedom this arrangement has.
A Simpson gearset at the golden ratio, turning. ring1 in, hold carrier2, with every member's speed taken from the train's null space and every angular position that speed integrated. The teeth are marked at the pitch points rather than cut as involutes — the flank is the teeth field's subject — but the count is the tooth count and the positions are the solved ones, so what turns and how fast is real. Drag it and watch which way each member goes: sun -0.618 · ring1 1.000 · output 0.382 · carrier2 0.000.
Fig. 6 The Fibonacci Simpson turning: a 55-tooth sun in an 89-tooth ring with 17-tooth planets, whose three-speed ladder is geometric to a hundredth of a per cent and which assembles with three planets or four.

What “spread” hides

One more consequence, since spread is the number gearboxes are advertised with.

Spread is top over bottom and says nothing about what is between. Two four-speeds with a spread of 4.24 can have completely different ladders: the geometric one with three steps of 1.618, or one with a first step of 2.0 and two of 1.46. The advertised number is the same and the cars drive differently.

For a given arrangement, though, spread is more informative than it looks, because it is a function of the same one or two parameters as everything else. A Simpson’s spread is exactly its first gear, 2+1/K2 + 1/K, since third is 1 and there is no overdrive; so a Simpson advertised with a spread of 2.46 has declared KK, and therefore its second gear, and therefore both its steps. One number quoted, and the whole gearbox is determined. That is not true of a countershaft manual gearbox, where every pair is independent, and it is one of the ways in which planetary automatics are a different sort of object.

The steps, against the ones the rule asks for. The design rule everybody quotes is that the steps between gears should be equal in ratio, so that the engine returns to the same speed after every shift. That makes the sequence geometric, and the ideal step for this spread over this many gears is 1.5683, marked. The steps a gearset actually gives are not free: the whole sequence is a function of the tooth counts, so once the top and bottom are chosen there is nothing left to spend on the middle. The worst step here is off the ideal by 7.5%.
Fig. 7 The three-speed’s two steps against its ideal — 7.5% and 6.9% out, in opposite directions, and the departure is again bottom-heavy. With one parameter and two steps there is nothing to trade: the whole shape moved when K was chosen for first gear.

The other ladders in this field

Two of the field’s mechanisms have no ladder at all, and putting them beside the argument sharpens what a ladder is.

A continuously variable transmission has no steps, so the whole geometric-progression question evaporates: at every road speed the controller picks the ratio it wants rather than the nearest of four. That is the mechanism’s whole selling point, and what it costs is that the ratio stops being a count and starts being a quotient of two solved lengths.

A reverted train has one ratio and no ladder, and its difficulty is of a completely different kind: getting a single exact ratio out of it while keeping its shafts coaxial turns out to be a Diophantine problem with no solutions at all below a certain size.

Between the three, the field has a nice spread of what “a ratio is hard to get” can mean. For a gearset the ratios are easy individually and constrained collectively — any one of them can be had, and not all four at once. For a reverted train one ratio is hard because two integer conditions have to hold together. For a variator every ratio is available and none of them is exact.

The steps, against the ones the rule asks for. The design rule everybody quotes is that the steps between gears should be equal in ratio, so that the engine returns to the same speed after every shift. That makes the sequence geometric, and the ideal step for this spread over this many gears is 1.6180, marked. The steps a gearset actually gives are not free: the whole sequence is a function of the tooth counts, so once the top and bottom are chosen there is nothing left to spend on the middle. The worst step here is off the ideal by 0.0%.
Fig. 8 The Fibonacci three-speed’s two steps, which are the same number to four decimal places. Set against the catalogue gearbox’s 7.5% departure, this is what the equal-step rule looks like when the arrangement is allowed to satisfy it rather than being asked to after its ends are fixed.
A Ravigneaux gearset at the golden ratio, turning. sun2 in, hold ring, with every member's speed taken from the train's null space and every angular position that speed integrated. The teeth are marked at the pitch points rather than cut as involutes — the flank is the teeth field's subject — but the count is the tooth count and the positions are the solved ones, so what turns and how fast is real. Drag it and watch which way each member goes: sun1 -0.618 · sun2 1.000 · ring 0.000 · carrier 0.382.
Fig. 9 The Fibonacci Ravigneaux turning: suns of 34 and 55 in a ring of 89, with long planets of 17. Its four ratios are φ², φ, 1 and 1/φ, and the tooth counts are three consecutive Fibonacci numbers because those are the best rational approximations to the root of the quadratic.

The check

The gate asserts four things separately, and the third is the one that keeps the others honest.

That φ\varphi solves the quadratic the ladders produce. That the Fibonacci gearsets’ steps are equal to within a hundredth of a per cent. That a catalogue four-speed’s steps are not — the check fails if the ordinary gearset ever comes out closer than five per cent — so the first two are a discovery rather than a property of the measurement. And that the Fibonacci gearsets pass the assembly conditions, without which the whole result would be a piece of arithmetic about numbers rather than a statement about a gearbox that could be cut.

One last consequence of reading the ladder as a recurrence rather than as four numbers. A geometric ladder is the only one whose shape is unchanged by adding a gear at either end: append a rung above the top and the ratios are still in geometric progression, with the same step, and every strategy built on the ladder still applies. Any other ladder has to be redesigned when a gear is added, because the steps that were tuned around a particular top gear are now interior steps with a different job. That is a property nobody asks a gearbox for and it is quietly the reason the rule survives — a designer who follows it has a family of transmissions rather than a design, and the eight- and nine-speed automatics that came later were extending a ladder rather than replacing one.

What this makes readable

Essays that name this one as a prerequisite.

About the same objects

Not linked from either essay — found by the objects both name.

What links here

Essays that link to this one from their own argument.

The objects this essay names

Each one links to every other essay that touches it.

Catalogue numberDesign ruleDimensionless ratioEpicyclicGeometric progressionRatio stepsRavigneauxSimpson gearsetTransmission relationVelocity ratio