Equilibrium

The load that is never all there at once

A column at the bottom of twenty storeys is designed for the imposed load of twenty floors added up, and twenty floors do not reach their own worst day together. The reduction that follows is not a discount on the safety margin. It is the central limit theorem, and it has a floor it never goes below.

Assumes The load a beam is given is a decision, The strength no specimen had and The envelope is not a structure.

A beam on the eighteenth floor of an office building is designed for an imposed load of five kilonewtons per square metre. So is the beam on the seventeenth, and the sixteenth, and every one below them. The column that carries all twenty of them is designed for the sum, and the sum is a number nobody expects to see.

Not because the five is wrong. It is a characteristic value — a load with a small probability of being exceeded on a floor over the building’s life — and it is roughly right for each floor taken alone. The trouble is what happens when twenty of those are added. Each was drawn at, say, the ninety-fifth percentile of its own distribution; the total of twenty is not the ninety-fifth percentile of the total, because twenty floors would all have to be having their worst afternoon at once.

Independence, and the floor it never goes below. The reduction factor a column is allowed, two ways. The code's storey rule falls to 0.70 and stops. The independence argument — n bays each with a mean and a standard deviation, summed — gives (1 + zv/√n)/(1 + zv), which falls faster and stops at 0.503: a floor with no n in it at all, decided only by how variable the load is and how far out the fractile is drawn. The mean is never reduced away, because every bay really does carry its mean. At ten storeys the two differ by 10.0 points.
Fig. 1 The reduction factor a column is allowed, two ways. The code’s storey rule is a straight line to a floor at ψ₀; the independence argument falls as one over the square root of the number of bays and stops at 1/(1 + zv). Neither reaches zero, and the reason is the same for both.

The arithmetic, which is one line

Let each bay carry a load with mean mm and standard deviation ss, and let the bays be independent. The characteristic value for one bay is the fractile

qk=m+zs,q_k = m + z s,

with z=1.645z = 1.645 for the ninety-fifth percentile. Now put nn of them on one column. A sum of independent variables has mean nmnm and standard deviation sns\sqrt{n} — the variances add, not the deviations — so the total’s own fractile is

Qk=nm+zsn.Q_k = nm + z s \sqrt{n}.

Divide the second by nn times the first and the reduction factor falls out:

α(n)=nm+zsnn(m+zs)=1+zv/n1+zv,\alpha(n) = \frac{nm + zs\sqrt n}{n\,(m + zs)} = \frac{1 + zv/\sqrt n}{1 + zv},

with v=s/mv = s/m the coefficient of variation. That is the whole derivation. There is nothing in it about buildings, floors or occupancy; it is the central limit theorem written for a column.

Two features of it are worth pausing on. The first is that the factor depends on the product zvzv and not on zz and vv separately, so a rarer fractile and a more variable load are interchangeable as far as the reduction is concerned. The second is that the numerator and denominator differ only in that n\sqrt n: at n=1n = 1 the two are identical and the factor is exactly one, which is not a boundary condition imposed on the formula but the formula agreeing that one bay is one bay.

The floor it never goes below

The interesting part of that expression is not how fast it falls but where it stops. As nn grows the 1/n1/\sqrt n term vanishes and

α()=11+zv,\alpha(\infty) = \frac{1}{1 + zv},

a floor with no number of storeys in it at all. For an imposed load with a coefficient of variation of 0.6 read at the ninety-fifth percentile it is 0.503. A hundred floors and a thousand floors get the same answer.

The reason is worth stating plainly, because the mistake it prevents is common. Averaging does not remove the load; it removes the variability. Every bay really does carry its mean, and no amount of independence makes the mean go away — what disappears is the pretence that all of them are simultaneously at the top of their own distributions. The reduction is bounded below by the ratio of the mean to the characteristic value, and that ratio is a property of how variable the loading is and of how far out the fractile was drawn.

That makes the floor a useful diagnostic. A load with a small coefficient of variation has almost nothing to reduce: at v=0.3v = 0.3 the limit is 0.670. A wildly variable one has a great deal: at v=1.0v = 1.0 it is 0.378. How much reduction a load class deserves is a statement about its scatter and about nothing else, which is why the rules distinguish offices from storage and not steel from concrete.

The characteristic strength, which nothing was measured at. A lognormal population of strengths with a mean of 5 N/mm² and a coefficient of variation of 0.60. The characteristic value is the 5% fractile — 1.7 N/mm², which is 34% of the mean, and which need not be the strength of any specimen that was tested. Dividing it by 1.50 gives 1.1, and the shaded sliver below that is the fraction of the population that would fail to reach it: 8.7e-3, or one in 114. A factor applied to a fractile is not covering the scatter, because the scatter has already been spent getting to the fractile.
Fig. 2 The same construction that produces a characteristic strength produces a characteristic load, from the other tail. A fractile is a distance from the mean measured in standard deviations, so the gap between the mean and the characteristic value is what a reduction has to work with — and it is the whole of what a reduction has to work with.

What the codes say, and where they came from

Two rules are in general use and they are the same argument in different clothes.

The storey rule reduces on the number of floors: αn=(2+(n2)ψ0)/n\alpha_n = \big(2 + (n-2)\psi_0\big)/n, capped at one, with ψ0\psi_0 the combination factor — 0.7 for an office. It gives no reduction at all for one or two storeys, 0.90 at three, 0.80 at six and 0.76 at ten, and its own floor is ψ0=0.70\psi_0 = 0.70.

The area rule reduces on the area collected: αA=57ψ0+A0/A\alpha_A = \tfrac57 \psi_0 + A_0/A, capped at one, with A0=10A_0 = 10 m². Its floor is 57ψ0\tfrac57\psi_0, which for ψ0=0.7\psi_0 = 0.7 is exactly a half.

Set the two against the independence result and something worth noticing appears. At ten storeys the storey rule gives 0.760 and the independence argument gives 0.660: the code is the more conservative of the two, and it stays that way at every count. So the rule is not the statistical argument transcribed — it is the statistical argument with something held back, which is the right way to write a rule whose central assumption is one nobody can check.

A column is a running total. A column carrying 36 m² of floor at each of ten levels, at 5 kN/m². Each floor adds 180 kN, so the load at the base is 1800 kN — the same tributary area counted ten times. Nothing in the drawing changes down the height; only the number does.
Fig. 3 The column as a running total, before any reduction. Ten levels of 36 m² at 5 kN/m² is 1,800 kN into the foundation. The storey rule takes it to 1,368 and the independence argument to 1,188 — a difference of 180 kN, which is one and a half floors of the building, decided entirely by which of two defensible arguments is being made.

The square metre worth half a square metre

The area rule has a property that is not obvious from its form and is the most practically useful thing about it.

The load the column is designed for is A×q×αAA \times q \times \alpha_A, and substituting the rule gives

Aq(57ψ0+A0A)=q(57ψ0A+A0).A\,q\left(\tfrac57\psi_0 + \frac{A_0}{A}\right) = q\left(\tfrac57\psi_0 A + A_0\right).

The area cancels out of the second term. The design load is linear in the area collected, with a slope of 57ψ0\tfrac57\psi_0 — a half, for an office. Past the point where the reduction bites, every additional square metre of floor handed to a column contributes half of its own load and no more, for ever.

The square metre that is worth half a square metre. The load a column is designed for against the area it collects, with the area rule applied. Because α_A = (5/7)ψ₀ + A₀/A, the product A·α is (5/7)ψ₀·A + A₀ — linear, with a slope of 0.50. So past the point where the reduction bites, every extra square metre of floor adds 50 per cent of its own load to the column and no more. For the ψ₀ = 0.7 of an office that slope is exactly a half, which is the whole of the rule in one number.
Fig. 4 Design load against tributary area, with the area rule applied, against the unreduced line. The two diverge and then run parallel at half the slope. A column at the bottom of a large building is being charged half rate on everything past the first few bays, which is why the reduction matters far more to a transfer column than to a floor beam.

That is a strong statement about where the rule pays. A floor beam collecting 30 m² gets 0.78 — barely worth the arithmetic. A column collecting 360 m² gets 0.528. A transfer structure collecting the load of an entire tower gets the floor and nothing better. The rule is not a small correction applied uniformly; it is a correction that grows with exactly the members whose design is hardest.

Which free body produced the number

Every quantity in this collection comes from cutting something and insisting the sums cancel, and it is worth being explicit about what has been cut here, because the free body is not the usual one.

Take a horizontal cut through the column immediately below the topmost floor it carries, and draw the free body above the cut: nn floors, each carrying whatever it happens to be carrying at that instant. Vertical equilibrium says the axial force in the column is the sum of those nn floor loads. That is exactly the running total the tributary rule builds, and nothing about it is in question.

What is in question is which value of each floor load goes into the sum. The free body is drawn at an instant; the characteristic value is a statement about a distribution over decades. Putting twenty characteristic values into one instantaneous equilibrium equation is a category error, and the reduction factor is the correction for it. The equilibrium is exact and the loading is a hypothesis, which is the shape of most of the honest difficulty in this subject.

The dead load is not reduced, and the reason is the whole argument

Nobody reduces the self-weight, and it is worth asking why not, because the answer confirms the mechanism rather than merely stating an exception.

Self-weight is not independent between floors. If the screed on floor three came out twenty millimetres thick instead of fifteen, the screed on floors four to twenty very probably did too — same contractor, same specification, same misunderstanding. The variables are strongly correlated, the variances do not simply add, and n\sqrt n is replaced by something much closer to nn. In the limit of perfect correlation the reduction factor is exactly one.

So the rule’s real content is not live loads are reduced and dead loads are not. It is loads that vary independently between the bays being summed may be reduced, and loads that do not may not, and the familiar version is a shorthand that happens to be right for the usual case. It also says immediately where the shorthand fails.

Two beams tied together, and the deeper one takes 89% of the load. Two simply supported beams of 6 m, one twice as deep as the other, tied together at midspan so that they have to move as one. A load of 100 kN stands on the tie. Point stiffness is 48EI/L³, so the deeper beam is 8 times as stiff — depth cubed, nothing else — and the load divides in that ratio: 11.1 kN into the shallow beam and 88.9 kN into the deep one, 11% against 89%. Both midspan points move 5.00 mm, which is the whole of the argument: the geometry of the load never entered it. The deflection is drawn 78 times full size — the real sag is 5.00 mm on a 6 m span, about 1 in 1200.
Fig. 5 Independence is a property of the loading, not of the structure. Two paths sharing a displacement are perfectly correlated in what they carry, whatever their stiffnesses. Two floors sharing nothing but a column are as independent as their occupants are, which is an assumption about people rather than about statics.

The same argument, pointing the other way

There is a second place in this collection where a structural quantity is decided by many independent draws rather than by one, and it is worth setting beside this one because the two point in opposite directions for the same reason.

A larger specimen is weaker than a small one. Strength is set by the worst flaw the volume happens to contain, so a big volume is a large sample and a large sample has a worse worst member. The governing operation is a minimum over many draws, and a minimum gets worse as the number of draws grows.

Load works the other way. A column’s demand is set by the sum of many draws, and a sum concentrates: its coefficient of variation falls as 1/n1/\sqrt n while its mean grows as nn, so the sum becomes more predictable in relative terms and its characteristic value falls below the sum of the characteristic values.

A strength that is a property of the specimen. Nominal strength against size for geometrically similar specimens of one material. On the left the specimen is too small for a crack to run and the strength is a plateau — a plastic limit, and the regime laboratory specimens sit in. On the right a crack releases more energy than it consumes as soon as it starts and the strength falls as the inverse square root of size, which is the regime real structures sit in. The turn happens at D₀ = 120 mm. A 100 mm specimen reads 3.10 N/mm² and a 1500 mm member of the same material carries 1.14: the test overestimates the structure by a factor of 2.71.
Fig. 6 The mirror image, drawn. A strength decided by the weakest of many independent volumes falls with size; a load decided by the sum of many independent bays rises less than proportionally. Both are statements about a large number of independent draws and they pull in opposite directions — which means that scaling a structure up moves the demand and the capacity toward each other from both ends, and neither movement is in any code’s partial factors.

That is not a coincidence of arithmetic. It is the two ways a large structure differs from a small one, and a designer who knows only the first has half of it.

What it does to a foundation

The place the reduction is largest is the place where the consequence of getting it wrong is hardest to inspect.

A pad or a pile group under a tall building’s column collects the whole of that column’s reduced load, and its size follows almost linearly from it: at the area rule’s floor the foundation is being asked for a little over half of what the unreduced sum would demand. On a large raft or a heavily loaded pile group that is the difference between one arrangement and another.

But settlement is not decided by the characteristic load; it is decided by something much closer to the mean, sustained for years, and the two questions want different numbers out of the same distribution. A foundation checked for bearing capacity at the reduced characteristic load and for settlement at the quasi-permanent one is using two different points on one curve, which is correct and is often not what happens.

Where a beam's load comes from. A 8 × 6 m panel carrying 5 kN/m², divided at 45° from the corners. The long beams take a trapezoid of 15.0 m² each and the short beams a triangle of 9.0 m²; the four areas sum to 48.0 m², which is the panel, so no load has been invented or lost. The line loads quoted are the uniform equivalents; the real distributions peak at 15.00 kN/m at midspan.
Fig. 7 Where the load came from in the first place, which is the decision the reduction modifies rather than replaces. The tributary rule says which floor belongs to which column; the reduction says what fraction of its characteristic value that floor contributes once several of them are added. Neither is a measurement, and the second is much less often examined than the first.

Where it must not be applied

The exceptions are not a list to be memorised; each of them is a place where the independence assumption is visibly false.

Storage. A warehouse is loaded to its rated capacity on every floor by the same operation, on purpose, and the loads are close to perfectly correlated. No reduction.

Plant rooms and equipment. The load is a machine that is either there or not there, and it is there on every floor of the plant level simultaneously. It is closer to a dead load than to an imposed one.

Car parks. The correlation is unfortunate rather than physical: everyone arrives at the same time.

Anything already reduced. The storey rule and the area rule are two estimates of the same effect and must not be multiplied together. A designer who applies both to one column has taken the reduction twice, and the second application has no argument behind it at all.

Loads whose arrangement is the point. Pattern loading asks what happens when some bays are loaded and others are not, which is a question about arrangement rather than about magnitude. The two are independent decisions and both apply — but a reduction taken on a pattern case has to be taken on the intensity, not on the number of bays chosen to be loaded, or the two arguments collide.

The rule is a fractile correction, not a saving

The most common misreading is that the reduction is margin being given away, and it is worth refuting directly because the correct reading changes what a designer should feel about it.

Take twenty floors at the ninety-fifth percentile each. If the loads really are independent, the sum of twenty characteristic values sits at roughly the 99.9th percentile of the total distribution — a return period of centuries rather than of decades. That is not the reliability the design was aiming at; it is a much higher one, arrived at accidentally, applied only to the columns, and different for every column depending on how many floors it happens to carry.

The reduction restores the intended fractile. A designer who declines it has not built in extra safety in any principled sense — they have built in an unknown and uneven amount of it, concentrated on the members where material is most expensive, and they have made the structure’s reliability a function of its height. The characteristic value exists precisely so that this does not happen; refusing to apply it consistently discards the thing it was for.

What it looks like when it is wrong

Two failure modes, and both are quiet.

Taking the reduction on a correlated load. The arithmetic still produces a number and the number is smaller, so nothing complains. The error is invisible in the calculation and shows up, if at all, as a column that is more heavily loaded than its neighbours expected. A structure whose imposed load is genuinely correlated between floors and which has been reduced as though it were not has had a real margin removed.

Taking it twice. A spreadsheet that applies the area rule at the beam and the storey rule at the column has multiplied 0.78 by 0.76 and arrived at 0.59 for a column the rules would each have given about 0.76. Nothing in either rule refuses this, because each is written as though it were the only one.

The second is worth a check that could fail: sum the reduced column loads over a floor plate and compare with the reduced total of that floor. If the reductions have been applied consistently, the two agree; if a column has been reduced twice, the sum of the parts falls below the whole by exactly the extra factor. A statement that can be tested against a total is worth more than one that can only be read, and this one costs a single line in a schedule.

Where the model stops

Independence is an assumption about occupancy, not a fact. It is a good one for offices and a poor one for buildings where one tenant fills several floors and moves in over a weekend. Nothing in the calculation knows the difference.

The fractile drifts with the number of bays being summed. The derivation above holds the fractile fixed and asks what the factor must be. Real rules were calibrated against reliability targets on a small number of representative buildings, which is not the same operation and does not give the same answer to more than two figures.

The coefficient of variation is not measured on the building being designed. It comes from surveys, most of them decades old, most of them of offices, and it is the single number the whole floor depends on. A change from 0.6 to 0.8 moves the limiting factor from 0.503 to 0.432 — a fifteen per cent change in the load a tall building’s columns carry, from a statistic nobody on the project will ever see.

The rule says nothing about arrangement. Reducing the intensity leaves the question of which bays are loaded entirely open, and on a continuous structure that question is often the one that governs.

And the whole apparatus is about the ultimate limit state. A deflection check, a vibration check and a crack-width check each want a different point on the same distribution, and none of them wants the reduced characteristic value. Carrying one reduced number through every check is the commonest way this rule is misused, and it is misused in the direction of optimism on exactly the checks — the serviceability ones — that most often decide the member.

Where the ladder goes

Later rungs on this anchor: the reliability calculation behind the combination factors, and what target it was calibrated to. Correlated imposed loads and how the factor changes when the correlation is not zero. Reduction rules for members other than columns — walls, transfer beams, foundations — and why they differ. The interaction between reduction and load arrangement, where the two are usually applied together and rarely reconciled. Imposed load surveys and what they actually measured. The treatment of loads that are partly permanent, such as partitions. Reduction in seismic mass, where the same argument is made about a completely different quantity. And the question underneath all of it: whether a rule calibrated on offices in the nineteen-seventies describes a building that is now half meeting rooms and half server racks.

Named alongside this one

Essays reaching for the same objects. Nobody chose these; they are what the concept index makes visible.

The objects this essay names

Each one links to every other essay that touches it.

Characteristic valueFractileImposed loadIndependenceLive load reductionLoad combinationLoad pathTributary area