Deflection

The gap nobody computed

A movement joint is sized by adding up everything the structure will do to it, and the deflection calculation — the only term anybody computes carefully — is usually the smallest one in the list. The largest is a construction tolerance, which is not a structural quantity at all, and the sum of the extremes is nearly twice what treating them as independent would ask for.

Assumes The movement nobody applied, Stiffness is not strength, and usually it is the one that governs and The curvature nobody applied.

A partition runs up to the underside of a floor slab and stops. The gap between the two is filled with a compressible seal and covered with a bead, and the drawing says 25 mm.

Where did 25 come from?

The gap is a sum of five things and only one of them is computed. What a 30 mm movement joint is asked to accommodate, by three combination rules. The top bar is every term at its extreme, added: 33.2 mm, which assumes the hottest day, the fullest floor, the whole of the shrinkage and the worst-placed wall arrive together. The chance of that is about 1.5%. The bottom bar treats them as independent and asks for 16.0 mm. The middle bar is the rule used for actions and almost never for movements — one term at its full value and the rest at their coincidence factors — and gives 25.5 mm. The segments across the top bar are the terms themselves, and the ordering is the finding: the largest is tolerance at 10.0 mm, which is not a structural quantity at all, and the smallest is deflection at 3.2 mm — the only one anybody computes carefully, and 10% of the total.
Fig. 1 What a movement joint is asked to accommodate, under three ways of combining the five terms. Adding every term at its extreme asks for 33.2 mm; treating them as independent and taking the root-sum-square asks for 16.0; the rule used for actions and almost never for movements — one term at its full value and the rest at coincidence factors — gives 25.5. The segments across the top bar are the terms themselves, and their ordering is the finding: tolerance is the largest at 10.0 mm and deflection the smallest at 3.2, which is a tenth of the total and the only one anybody computes carefully.

The honest answer, on most projects, is that it came from a standard detail. And the reason that is not indefensible is that computing it properly is a job nobody’s discipline owns: the structural engineer computes one of the five terms, the concrete specialist knows two more, the contractor owns the fourth, and the fifth is a statistical question about all of them together.

Which free body produced the number

There is no free body here, and saying so is worth doing because it explains why the calculation is orphaned.

Every other quantity in this collection is a force or a stress, arrived at by cutting something and insisting the sums cancel. A movement budget is none of those. It is an accumulation of displacements, each computed by a different method, most of them not forces at all, and the answer is a length rather than a stress.

That is why the calculation has no natural home in a set of calculations organised by member. It belongs to the joint, and a joint is a place where two members are not, which is precisely the region every member-based method leaves out.

The five terms, and their ordering

For a concrete frame with a 6 m storey and a 30 m plan dimension, the movements at a wall head are roughly these.

Thermal — the slab above expands and contracts relative to the wall below, at αΔTL\alpha\Delta T L over whatever length is restrained. Nine or ten millimetres, and it reverses, which is what makes it different from the others.

Shrinkage — a concrete slab shrinks by 300 to 500 microstrain over its life, most of it in the first year. Six millimetres over the same length, one way only, and it never comes back. Where it is restrained it becomes a curvature rather than a movement, which is the curvature nobody applied and adds to the deflection term as well.

Creep — the slab shortens under sustained compression by two or three times its elastic shortening. Four or five millimetres, again one way.

Deflection — the slab above sags under its own weight and its live load, and the sag at the wall’s position is what closes the gap. Three millimetres, and the only one anybody calculates properly. It is also the only one with a code limit attached to it, which is part of why it receives the attention: span over 360 is a number a check can be written against, and there is no equivalent clause for any of the other four.

Tolerance — the slab is cast within a construction tolerance of its intended level, and the wall is built to within another. Ten millimetres, comfortably the largest term, and it is not a structural quantity at all.

The smallest term is the computed one and the largest is a builder’s tolerance. Every hour of analysis spent refining the deflection prediction is being spent on a tenth of the answer, and the term that dominates it is decided by a spirit level.

Four camber rules, and what each leaves on the finished beam. The same 18 m composite beam, cambered against four different things, followed through its own load history. Positive is a sag and negative a hog, and the point at the left of each line is the shape it was fabricated to. Cambering against the wet concrete leaves 76.8 mm of sag at the end and a flat beam on the day the slab is poured; cambering against the total load leaves the beam dead flat when fully loaded and hogged 204.7 mm — one part in 88 of the span — before anything is on it at all.
Fig. 2 The one term that is computed, and its own decomposition. A deflection is itself a sum of stages arriving at different times, so even the small term is a budget rather than a number.

Two combination rules, and the answer between them

Add the extremes and the answer is 33 mm. That assumes the hottest day, the fullest floor, the whole of the shrinkage, the whole of the creep, and the worst-placed wall all arrive at once.

Treat them as independent and take the root-sum-square, and the answer is 16 mm — less than half.

Neither is right and the reason is structural rather than statistical. Some of the terms are not random at all: shrinkage and creep are one-way, they arrive with certainty, and there is no sense in which they might not happen. Some are random and reversible: thermal and live-load deflection are both at their extremes for a small fraction of the time. And one — the tolerance — is a fixed offset once the building exists, unknown before it is built and constant afterwards.

The rule that fits that mixture is the one already used for actions: one term at its full value and the rest at their coincidence factors, taken as the maximum over which term leads. On the budget drawn that gives 25 mm — which happens to be the number on the standard detail, arrived at by a route nobody took.

The envelope is not a structure is the same argument for load arrangements: the envelope of a set of cases is a curve no single case produces, and designing to it produces a member that no state of the structure ever asks for. A sum of movement extremes is that envelope, applied to displacements.

Why the conservative answer is not free

The instinct is to add the extremes and be safe, and it is worth being explicit about why that is not obviously right.

A joint that is too large is not a joint with a margin. It is a detail that has to work at every opening between zero and its full size, and the wider it is the harder that is: the seal has to compress and recover through a bigger range, the cover bead has to hide a bigger gap, the fire and acoustic performance of the joint has to hold at its widest, and the aesthetic of a 40 mm dark line at every wall head is a thing an architect will notice.

More practically, an over-sized joint on a partition is an under-sized joint somewhere else. The movement is a fixed quantity: it goes into the joints provided or into the elements that were not supposed to move. A design that provides generously at one joint and forgets another has moved the problem rather than solved it.

It moves, or it pushes. Never both, and never neither. A 30 m steel member 40 °C warmer than it was built, in three conditions. Free, it grows 12.0 mm and carries nothing. Held, it moves nothing and carries 84.0 MPa in compression — which is E·α·ΔT and contains neither the length nor the area of the member, so the identical stress arises in a two-metre strut. Held by a spring it does some of each: 4.6 mm of movement and 51.5 MPa, and the split is decided by the spring rather than by the member.
Fig. 3 What happens where the movement is not provided for: the same 30 m element through a 40 °C change, in three conditions. Free, it grows 12.0 mm and carries nothing. Held, it moves nothing and carries 84.0 MPa — which is EαΔTE\alpha\Delta T, and contains neither the length nor the area, so the identical stress arises in a two-metre one. Held by a spring it does some of each, 4.6 mm and 51.5 MPa, and the split is decided by the spring rather than by the element.

That last point is the movement nobody applied in its most useful form: the stress from restraining a thermal movement is EαΔTE\alpha\Delta T and contains no length whatever, so a small unprovided-for movement produces the same stress as a large one. There is no such thing as a movement small enough to ignore; there are only movements small enough to be absorbed by cracking something that does not matter.

That last clause is the one to be careful with, because “something that does not matter” is a choice somebody has to make rather than a property of the structure. A concrete wall cast against a base that has already hardened is the standard case, and the base does not have to hold it very firmly to break it.

Restraint is a fraction, and the length decides how far up it reaches. A 30 m wall 3.0 m high cast against a base that has already hardened — a length-to-height ratio of 10.00. The base holds the bottom of the wall at R = 0.50 and the top of it at 0.364, decaying as 0.727 to the power of the height in wall heights. The free contraction is 380 microstrain, of which 84 per cent is the wall cooling from its own hydration peak and the rest is drying; the concrete's own strain capacity is 50. Everything to the right of the dashed line cracks, which here is the bottom 3.00 m of it. Nothing has been loaded.
Fig. 4 A 30 m wall 3.0 m high on a base that has already set, at a length-to-height ratio of 10.00. The base holds the bottom of the wall at R=0.50R = 0.50 and the top of it at 0.364, decaying as 0.727 to the power of the height in wall heights. The free contraction is 380 microstrain, 84 per cent of it the wall cooling from its own hydration peak; the concrete’s own strain capacity is 50. Even the least-restrained line, at the top, is above that — so the whole 3.00 m of it cracks, with nothing loaded and nothing applied.

Note what the restraint fraction does and does not depend on. It is a ratio of two stiffnesses, so it carries the wall’s proportions and not its size: the same figure at twice the length and twice the height gives the same fractions. The movement a joint would have accommodated does not disappear when the joint is left out — it is redistributed into cracks whose spacing and width are the only remaining design variables.

There is a third failure mode of the conservative answer that is worth naming because it is the one that actually happens. A joint sized by adding extremes is a joint that spends its entire life partly open, because the coincidence it was sized for never occurs. A 40 mm gap that is at 12 mm on an ordinary day is a 28 mm void behind a bead, and voids behind beads collect dust, admit sound, defeat fire seals and get filled by somebody with a mastic gun who has not been told why the gap is there. Built to the wrong shape is the same idea for a beam: a member cambered for a movement that does not arrive is a member that is visibly wrong for the whole of its life, and being wrong in the safe direction is still being wrong.

A joint has two budgets, not one

The five terms have been added as magnitudes, and they do not all have the same sign. Sorting them by direction turns one number into two, and the two are not equal.

Some terms close the gap: the element above sagging under load and creep, a support beneath settling relative to the one above, the element below expanding as it warms. Others open it: the element below shrinking, contracting as it cools, or losing a camber it was built with.

So the joint has a required closure capacity and a required opening capacity, computed from two different subsets of the same five terms, and quoting a single dimension conflates them. On a typical wall head the closing sum is dominated by the slab’s long-term deflection and the opening sum by the wall’s own shrinkage, and the two are rarely within a factor of two of each other.

That distinction is what selects the component rather than the dimension. A gap that mostly closes needs a compressible filler with enough travel and enough recovery to be squeezed repeatedly. A gap that mostly opens needs a seal that stays sealed as it is stretched, which is a different material property and a different failure mode — a compressible filler pulled apart simply parts.

And the tolerance term sits in both, with an unknown sign. It is a fixed offset once the building exists, so it does not consume travel in either direction repeatedly — it just decides where in the joint’s range the building starts, which is the reason a joint sized correctly can still be at the end of its travel on the day it is built.

The differential is what does the damage

One further distinction turns the budget from an accounting exercise into a design problem.

Nothing is damaged by moving. Things are damaged by moving relative to something else, and the relative movement is a difference of two of the quantities above rather than either of them.

A wall head gap closes by the difference between the slab’s downward movement and the wall’s upward growth. A cladding panel is distressed by the difference between the frame’s shortening and its own. A column and a core standing side by side shorten by different amounts because one is more heavily stressed than the other, which is the columns are shorter than the core and is a differential of two large numbers.

Two differences up the same building, peaking in different places. Differential shortening between a perimeter column and the core of a 30-storey building, plotted up the height. The part driven by load peaks at level 15 — exactly half way up, because a floor near the top has almost nothing built above it to shorten what is beneath, and a floor near the bottom has almost nothing beneath it to shorten. The part driven by shrinkage does not care what is above it at all and accumulates all the way to the roof. Their sum is worst at level 30, at 32 mm, which across a 9 m bay is a floor out of level by one in 278.
Fig. 5 Two elements shortening at different rates, and the difference between them accumulating up a building. The absolute movements are large and harmless; the difference is small and is what the floors have to accommodate.

It follows that a joint is not the only remedy and often not the best one. Making the two elements move together removes the differential without removing either movement — which is why a partition fixed rigidly to the slab above and free at the bottom can be a better detail than one free at the top, and why a cladding system hung from one floor and restrained laterally at the next has no differential to accommodate in the vertical direction at all. The design variable is the connection, and the budget is what says which connection to make free. Stiffness is not strength has a corollary here: what matters at a joint is neither, it is whether the two things are allowed to move apart.

Differences of large numbers are the hardest quantities to predict, because the errors do not cancel — a 20% error in each of two 15 mm movements is a 6 mm error in a 3 mm difference. So the term of the budget that matters most is the one computed least reliably, and the response has to be a detail that tolerates the answer being wrong rather than a calculation that gets it right.

The same budget everywhere else

The wall head is the smallest instance and the easiest to draw. The same accounting, with the same ordering and the same neglect, decides several much larger things.

A cladding support. A curtain wall bracket has to accommodate the frame’s floor-to-floor movement, the panel’s thermal movement, the frame’s shortening differential and the erection tolerance of two components made in different factories. The tolerance term dominates again, and the failure — a bracket at the end of its adjustment — is discovered on site with the panel in the air.

A settlement joint. Two parts of a building founded differently settle by different amounts, and the settlement that matters is the difference — which is another one-way term with a large uncertainty and no code limit.

A bridge bearing. Its movement rating is the sum of thermal, shrinkage, creep, live-load rotation effects and the setting error at installation, and where the structure is allowed to move shows that the articulation scheme decides how much of the total any one bearing sees.

A lift shaft. The guide rails are fixed to a shaft wall that shortens under creep while the rails do not, so the brackets have to slide — and the accumulated differential over forty storeys is tens of millimetres.

And a movement joint through a whole building. Here the budget decides a spacing rather than a dimension: how far apart the joints have to be for a joint of the available size to cope, which converts the whole argument into a plan decision made at scheme stage.

The bridge version of that last one is the clearest, because somebody has actually built the alternative. An integral bridge has no joint at all: the deck is cast into the abutments and the movement goes into the soil behind them.

Why a jointless bridge has a length. Long-term earth pressure force on an integral abutment against the length of the deck it is holding. The movement is proportional to the length, the pressure goes as roughly that movement to the power 0.6, and the force integrates over the wall height — so the load grows faster than the deck does and there is a length past which it is not worth having. At 60 m the abutment is carrying 2.49 times its at-rest force; the curve flattens only when the pressure reaches the passive limit of 4.2, which is a ceiling rather than a comfort. The expansion joint was not removed, it was moved into the soil — and the soil charges for it by the square of the length.
Fig. 6 Long-term earth pressure on an integral abutment against the length of deck it is holding. The movement is proportional to the length, the pressure goes as roughly that movement to the power 0.6, and the force integrates over the wall height — so the load grows faster than the deck does. At 60 m the abutment carries 2.33 times its at-rest force, and the curve flattens only when the pressure reaches the passive limit of 4.2, which is a ceiling rather than a comfort. The expansion joint was not removed, it was moved into the soil, and the soil charges for it by roughly the square of the length.

That is the budget argument with the joint deleted and the terms unchanged: the same thermal movement, the same shrinkage, the same creep, now accommodated by something that answers back. A jointless bridge therefore has a length, and the length is set by the budget rather than by the deck.

In every case the pattern is the same. The structural term is computed, the others are estimated or inherited, the combination rule is chosen by habit, and the result is a dimension that decides whether a component works.

Where the model stops

The terms were taken as independent when they are not. Creep and shrinkage share a moisture mechanism and both depend on the member’s thickness and the ambient humidity, so a dry environment increases both together. The root-sum-square is optimistic to the extent that they are correlated.

Nothing here is about time. Shrinkage and creep are mostly over within a year or two, and a wall built at six months has missed some of both — so the movement a joint has to accommodate depends on when the wall was built, which is a programme decision.

The tolerance was taken as a single number. It is a distribution, with its own mean and scatter, and it is the term with the least published data.

And a term can grow after the building is finished, which is the assumption most invisible in a budget written once. The integral abutment above is the case where it has been measured.

The summer that is worse than the one before it. The earth pressure behind an integral abutment, summer by summer, as a multiple of the at-rest value it started at. A 60 m deck expands by 10.8 mm at each end and pushes the abutment into the backfill. Granular soil under cyclic strain densifies, so the same movement next year needs a higher pressure to achieve, and K climbs from 0.38 toward 0.96 — a factor of 2.49 on the force, reached after about a century. The design load on an integral abutment describes the bridge's whole life rather than a load case, and it is the only load in this collection that gets larger because time has passed rather than because something was added.
Fig. 7 Earth pressure behind an integral abutment, summer by summer, as a multiple of the at-rest value it started at. A 60 m deck expands 9.0 mm at each end and pushes the abutment into the backfill; granular soil under cyclic strain densifies, so the same movement next year needs a higher pressure to achieve, and KK climbs from 0.38 toward 0.90 — a factor of 2.33 on the force, reached after roughly a century. The design value describes the structure’s whole life rather than a load case.

Nothing in the five terms of the wall-head budget ratchets like that, and the reason is worth stating: none of them is accommodated by a material that changes when it is worked. A soil is, a sealant is, and a compressible filler that has been squeezed ten thousand times is not the filler that was specified. The budget is written against the joint’s first year and the joint has to survive its fiftieth.

The reversible and irreversible terms were added as though they were the same kind of thing. They are not, and the distinction decides the detail rather than the dimension: a joint accommodating a reversible movement has to work at both ends of its range for a hundred years, while one accommodating a one-way movement passes through its range once and stays there. The first needs a seal that recovers; the second needs a seal that can be pointed once the movement has happened, which is a much easier component and a much harder programme.

And the joint has to be built. A 25 mm gap detailed and a 25 mm gap constructed are different things: the seal has a compression range, the bead has a coverage, and the two together define a working window narrower than the nominal dimension.

The generalisation

The habit worth taking away is to write out every term of a quantity before refining any of them.

The instinct in an engineering calculation is to compute the term that has a method behind it, carefully, and to allow for the rest. That is the right instinct when the computed term dominates and it inverts the effort exactly when it does not — and a movement budget is the clearest case in this collection of a quantity whose largest term is outside the calculating discipline altogether.

The second habit is about combination. Any quantity that is a sum of several uncertain things needs a rule for how they combine, and there are only three candidates: add the extremes, add them in quadrature, or take one at its extreme and the rest at a factor. The profession has a well-developed version of the third for loads, has thought about it for decades, and applies it to actions and to nothing else. Movements, tolerances, temperature effects and construction stages are combined by whichever of the first two the author reached for, and the difference between them is a factor of two.

There is a diagnostic that follows from the ordering and takes no calculation at all. On any budget of this kind, write the terms in order of size and then mark which discipline owns each. If the largest terms belong to disciplines that are not in the room, the number on the drawing was not designed — it was inherited, and it is right or wrong by whatever margin the standard detail happened to have. That is a defensible position on a repeat building and an indefensible one on a long-span, a tall building, or anything with an unusual grid, which is exactly where the standard detail’s assumptions have been left behind.

Scale changes everything has a version here that is easy to miss. Every term in the budget except the tolerance is proportional to a length, and the tolerance is not. So on a short element the tolerance dominates completely and on a long one it hardly matters — and a standard detail that works on a 6 m grid is the wrong detail on a 20 m one, for a reason that has nothing to do with the structure.

The stress has no length in it and the movement is nothing but length. Stress and movement against member length, for a 40 °C change. Held rigidly, the stress is 84.0 MPa at every length there is — E·α·ΔT, with no L, no A and no I anywhere in it. Held by a spring of 100 kN/mm the answer climbs with length rather than falling, because a longer member hands the same spring more movement to absorb: 36% of full restraint at 10 m and 76% at 60 m. The free movement, plotted to its own scale, reaches 24 mm.
Fig. 8 The two halves of that statement drawn against each other, for the same 40 °C change: the movement, which is nothing but length, and the stress, which has no length in it at all. Held rigidly the stress is 84.0 MPa at every length there is. Held by a real spring of 100 kN/mm it climbs with length rather than falling — 36 per cent of full restraint at 10 m and 76 per cent at 60 — because a longer element hands the same spring more movement to absorb. The free movement, on its own scale, reaches 24 mm.

Read that against the budget at the top of the page and the two ends of the argument meet. On a short element the movement terms shrink toward nothing while the tolerance stays at ten millimetres, so the joint is sized by the builder; on a long one the movement terms dominate the budget and, if the joint is not provided, the restraint is more nearly complete rather than less. Both ends of the length scale are worse than the middle, for opposite reasons, and the standard detail was drawn for the middle.

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ArticulationCamberCoincidenceCreepDeflectionDetailingDifferential movementImposed deformationLoad combinationMovement jointReliabilityServiceabilityShrinkageThermal movementTolerance