Rheology of Printable Concrete

Rheology is the study of how fresh cementitious material flows and resists flow, described for printable mortars by a yield stress that must be overcome before motion starts, a plastic viscosity that governs how hard it is to keep moving, and a time-dependent structural build-up that stiffens the material at rest.

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Rheology describes how a fresh cementitious material deforms and flows under stress. For 3D concrete printing it is the single most decisive material property, because a printable mortar has to be two contradictory things within a few seconds: fluid enough to be pushed through a hose and a nozzle, then stiff enough to hold a filament's shape and carry the weight of everything printed on top of it. Fresh concrete is not a simple liquid — it is a yield-stress fluid, a suspension of cement, fines and aggregate in water that behaves as a soft solid until the applied stress exceeds a threshold, and only then starts to flow. Printing is essentially the business of controlling that threshold in time and place.

What it is / Why it matters

The standard first approximation is the Bingham model, which characterises the material with two parameters. The yield stress τ₀ (in pascals) is the shear stress that must be exceeded before any flow occurs. The plastic viscosity μ (in pascal-seconds) is the slope relating shear stress to shear rate once flow has started. Below τ₀ the mortar holds its geometry; above it, the stress needed to keep it moving grows with how fast you move it.

Many printable mortars are not truly linear above the yield point. The Herschel–Bulkley extension adds a consistency coefficient and a flow index, capturing the shear-thinning common in mixes rich in fines, superplasticiser or viscosity-modifying admixture. It matters mostly when one mix must be described across a wide range of shear rates — high shear in the hose, almost none at the nozzle exit — which is exactly the situation in printing.

The physical meaning of the two parameters is easy to separate in practice. Yield stress governs shape: whether a deposited filament keeps its cross-section, whether a wall slumps under its own weight, and how many layers can be stacked before the bottom one deforms. Plastic viscosity governs motion: pumping pressure, pressure loss per metre of hose, the torque the pump must deliver, and how smoothly the material fills the nozzle. A mix can have an acceptable yield stress and still be unpumpable because its viscosity is too high, and the reverse failure — easy to pump, unable to stand — is just as common.

Two time-dependent effects sit on top of this. Thixotropy is a reversible, shear-induced breakdown of the flocculated particle network: shearing lowers the apparent yield stress, and rest lets the network rebuild. Structural build-up at rest is the broader phenomenon, combining reversible flocculation of cement particles, driven by colloidal and contact forces, with the irreversible contribution of early hydration as calcium silicate hydrate begins to bridge particles. Over the first seconds to minutes flocculation dominates and recovery is essentially complete after re-shearing; over longer intervals hydration takes over, the stiffening no longer reverses, and build-up shades into setting.

The build-up is usually described by a linear structuration rate, written Athix and expressed in pascals per second: the rate at which the resting yield stress rises in the early period. Roussel's rheological requirements framework, which underpins most of the current literature, ties printability to this quantity directly — the mortar must build up fast enough to support the deposition rate above it, without building up so fast that the previous layer can no longer bond. That trade-off is why a mix that performs well on a flow table can still fail on the machine.

How it is measured

Measurements split into two families, and confusing them is a frequent source of error.

Fundamental measurements use a rheometer to obtain values in physical units. A rotational rheometer with a vane or coaxial geometry shears the material at controlled rates and records torque, giving a flow curve fitted with the Bingham or Herschel–Bulkley model; vane geometry is preferred for mortars because it minimises wall slip. Structural build-up is measured by a rest-and-shear protocol: pre-shear to a reference state, rest for a defined interval, then shear again at a very low rate to capture the static yield stress that has developed, repeating over several intervals to obtain the Athix slope. These are research and laboratory protocols, not harmonised European standards — RILEM TC 276-DFC (Digital Fabrication with Cement-based materials) has worked on aligning them and ACI 238 covers workability measurement more broadly, but no EN standard prescribes a rheometer procedure for printable mortars.

Empirical measurements give a single number that correlates with yield stress without measuring it. The flow table to EN 1015-3 is the usual choice for mortars: the spread diameter after a defined number of drops is inversely related to yield stress. Slump and slump-flow to EN 12350-2 and EN 12350-8 serve the same function for concretes, though printable mixes are usually too stiff for slump to discriminate. Setting, which bounds the far end of structural build-up, is measured with the Vicat needle to EN 196-3. Penetrometer and fall-cone tests are widely used in 3DCP research to track yield stress on a bench, and unconfined uniaxial compression of a fresh cylinder — a green-strength test — connects rheology to buildability.

Empirical tests are for consistency control; fundamental tests are for understanding. A flow table result that drifts between batches tells you something changed, not what.

Typical ranges

The values below are indicative figures reported in the 3DCP literature for extrusion-based printing of cementitious mortars. They vary widely with binder, fines content and admixture system, and they are not measurements of any particular mix.

QuantityIndicative range reported in the literatureNote
Yield stress at the pump (sheared state)roughly 0.1–1.5 kPaValues reported for pumpable printable mortars; higher makes pumping impractical
Yield stress just after depositionroughly 1–10 kPaTypical for a printable mortar in published studies; must carry the first layers
Plastic viscosityroughly 5–100 Pa·sStrongly dependent on fines and admixture; wide scatter across studies
Structuration rate Athixroughly 0.1–2 Pa/s without acceleratorReported values; accelerated systems are reported an order of magnitude higher
Flow table spread (EN 1015-3)roughly 140–190 mm for printable mortarsIndicative window reported in published studies, mix-specific
Static yield stress recovery after shearmost of the reversible gain within the first minutesFlocculation-dominated period described in the literature

Each is a window, not a target: a mix inside all of them can still be unprintable if the timing does not match the machine.

What changes it

Water content is the strongest single lever: a small increase lowers both yield stress and viscosity sharply, which is why water dosing tolerance matters more in printing than in casting. Superplasticisers disperse cement flocs and reduce yield stress with comparatively little effect on viscosity, while viscosity-modifying admixtures do the opposite and also suppress bleeding. Accelerators raise the structuration rate and shorten the open window; retarders do the reverse. Fine content — limestone filler, fly ash, slag, silica fume or calcined clay — changes particle packing and specific surface, and therefore both water demand and the rate of build-up; silica fume and calcined clays in particular tend to raise yield stress and thixotropy. Aggregate grading and maximum particle size shift viscosity and the risk of blockage, and clay-based additives are used specifically to raise the recovery rate. Temperature accelerates hydration and therefore build-up. Mixing energy and history matter too: the same mix measured straight after mixing and after ten minutes in a hose is, rheologically, two different materials.

Failure modes

The characteristic failures map cleanly onto the parameters. Yield stress too low at the nozzle gives spreading filaments, loss of dimensional accuracy, and progressive slumping of the lower layers. Yield stress too high in the hose gives excessive pumping pressure, blockages, and in severe cases filter-pressing, where water is squeezed out of the mix and the solid skeleton jams; viscosity too high produces the same pumping symptoms without any shape problem. Structuration too fast leaves a stiff, poorly bonded surface by the time the next layer arrives, and cold joints between layers. Structuration too slow limits how many layers per hour the geometry can take and eventually leads to plastic collapse or elastic buckling of the wall. Poor stability — insufficient cohesion rather than insufficient yield stress — shows as bleeding water and segregation of the coarse fraction. Because rheology drifts with time, a mix that behaves correctly at the start of a run can leave the window before its end.

Concreef context

Concreef is a Bulgarian 3D concrete printing company based in Sofia, running material trials in its own workshop on a Crane WASP printer. It currently prints with a commercial premix while developing its own dry mix, and it has no published test data.

In practice rheology is handled as workshop discipline rather than as a published specification. Water dosing, mixing time and the interval between mixing and printing are kept as consistent as the equipment allows, because these are the variables that move yield stress and build-up most for a fixed premix. Batch-to-batch consistency is checked by simple empirical means before a run, and filament behaviour during a print — spreading, tearing, deformation of the lower layers — is read back as a rheological signal. In the development of an in-house dry mix, the targets described above are the framework being worked against. Nothing on this page represents a measured property of a Concreef material, and no claim is made that any Concreef mix has been tested to a standard.

Frequently asked questions

What is the difference between yield stress and viscosity?
Yield stress is the shear stress that must be exceeded before the material flows at all; below it the mortar behaves as a soft solid and holds its shape. Plastic viscosity describes the resistance to flow once motion has started, so it governs pumping pressure and how fast the material moves for a given driving force. A printable mortar generally needs a moderate yield stress that recovers quickly and a viscosity low enough to pump without excessive pressure.
Why does a printable mix need to be thixotropic?
Thixotropy is a reversible, shear-induced breakdown of the internal structure that rebuilds when the material is left at rest. In printing this is exactly the behaviour required: under the shear of the pump and hose the mortar becomes fluid enough to move, and within seconds of leaving the nozzle it regains stiffness and carries the layers placed on top. Without that recovery the filament spreads and the object slumps.
What does the Athix value mean?
Athix is the linear rate, in pascals per second, at which the yield stress of a mortar at rest increases over the first minutes after mixing. It is measured by repeated low-shear tests on a rheometer after controlled rest intervals. A higher Athix means faster stiffening, which supports more layers per hour but shortens the window in which the next layer still bonds properly.
Is a slump or flow table test enough to control a printable mix?
They are empirical single-point tests: they give a number that correlates with yield stress but say nothing about viscosity or about how the material stiffens at rest. For day-to-day consistency checks in a workshop they are useful and fast. For understanding why a mix prints or fails they are not a substitute for rheometer measurements or a structured build-up test.
Does rheology change after the material leaves the nozzle?
Continuously. Flocculation of cement particles dominates in the first seconds to minutes and is largely reversible, while early hydration progressively forms bridges that are not. The practical consequence is that the properties measured at the mixer are not the properties at the nozzle, and dwell time in the hose shifts the result.

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