Modelling the 3D printing of nanocellulose hydrogels of the future/3D... · Modelling the 3D...

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Modelling the 3D printing of nanocellulose hydrogels Tatu Pinomaa VTT Technical Research Centre of Finland Ltd

Transcript of Modelling the 3D printing of nanocellulose hydrogels of the future/3D... · Modelling the 3D...

Modelling the 3D printing of

nanocellulose hydrogels

Tatu Pinomaa VTT Technical Research Centre of Finland Ltd

www.nafems.org

Contents

• Motivation

• Nanocellulose-based hydrogels

• Material characterisation

• CFD models

– Printer head

– Deposition process

• Validation experiments

• Conclusions

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Motivation

• Bio-based dispersions for direct-write-printable structures with embedded sensing for health care applications (BioDisp3D)

– Academy of Finland, VTT and the University of Tampere; years 2014–2017

– Goal: to study the potential of nanocellulose-based pastes for the fabrication of sheets or 3D structures with special functionality for medical applications

• For example: Custom wound pads with the possibility to monitor healing without removing the pad. For large, hard-to-treat wounds.

• Modelling goals

– Predict the 3D printability of the material candidates

– Predict the sensitivity of the outcome to the process parameters

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Direct write paste -technology

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• Direct write technique for printing pastes

• Micro-dispensing environment based on nScrypt technology

• Prints 3D structures on 2D and 3D surfaces

• Post-treatments are usually needed (drying, sintering, UV-curing, laser, etc.)

• Compatible with all kinds of Nordson EFD tips and needles

• Line widths from 20 to 3000 μm, thicknesses from 5 μm upwards

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Nanocellulose hydrogels

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• Three-dimensional networks that consist of nanostructured forms of cellulose in a water matrix

• Reference material (TCNF)

– TEMPO-oxidised cellulose nanofibrils in water

– Produced from never-dried bleached hardwood kraft pulp

– Dry matter content of 1.06 wt-%

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Rheometry

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• Material models based on rheological characterisation

– Dynamic viscosity as a function of shearing conditions (incl. transient)

– Yield stress behaviour

• Anton Paar MCR-301 rheometer

– vane spindle and concentric cylinder geometries

• Measuring procedure

– Pre-shear at 100 s-1 for 60 seconds

– Rest period at 0.01% strain and 1 Hz for 300 seconds

– Gel strength: shear strain sweep from 0.01% to 100% at 1 Hz frequency

– Viscosity: shear rate sweep from 0.0001 s-1 to 3160 s-1

• Dispersing with an impeller, Ultra-Turrax and a sonifier

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Viscosity: steady-state behaviour

η = 𝑘𝛾 𝑛−1 How far does the power-law hold?

How does it level?

How does the paste settle?

𝑘cc, 𝑛cc

𝑘va, 𝑛va

Apparent power-law fluid in the measured range

Dependence on measurement geometry

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Goniometry

Contact angle in a sessile drop experiment

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CFD models for the printer heads

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• One-phase system of hydrogel

• Driven by a constant velocity boundary condition

• Volume of fluid (VOF) method used for compatibility with the deposition model

• No turbulence modelling applied

• Used to predict the dependence of hydrogel mass flux on the operating pressure

• Employs the open-source software OpenFOAM 2.3.x

Cylindrical steel tip Conical plastic tip

Axisymmetric mesh

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Analytical solution for power-law fluids

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ds dt

ls lt

P2 P1

𝑄s =𝜋𝑟s

3

1𝑛 + 3

Δ𝑃2→1𝑟s2𝑙s𝑘

1𝑛

P0

vs, Qs

vt, Qt

𝑄t =𝜋𝑟t

3

1𝑛 + 3

Δ𝑃1→0𝑟t2𝑙t𝑘

1𝑛

𝑄s = 𝑄t

Δ𝑃2→1 =

1𝑛 + 3

𝜋𝑟s3

𝑛

2𝑙s𝑘

𝑟s𝑄𝑠𝑛

Δ𝑃1→0 =

1𝑛 + 3

𝜋𝑟t3

𝑛

2𝑙t𝑘

𝑟t𝑄𝑡𝑛

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CFD model for the deposition process

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• Two-phase system of hydrogel and air

• Volume of fluid (VOF) method & Reynolds- averaged stress (RAS) model for turbulence

• Mobile substrate and air flow boundary conditions used to simulate printer head movement

• Wettability of the plastic substrate determined by an experimental contact angle

• Used to establish a connection between the paste rheology, printing parameters and the line profile

Printer head boundary condition

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Validation experiments

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• Step 1: pressure-massflux dependency

Hydrogel printed on the substrate for a fixed time at various operating pressures, then weighed

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Validation results

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• Step 1: pressure-massflux dependency (analytical predictions based on rheometry)

200 μm steel tip

510 μm steel tip

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Validation results

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• Step 1: pressure-massflux dependency (analytical predictions based on rheometry)

200 μm steel tip

510 μm steel tip

Pressure loss is dictated by the asymptotic behaviour of viscosity at high shear rates

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Validation results

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• Step 1: pressure-massflux dependency (numerical predictions based on rheometry & the massflux data)

200 μm steel tip

510 μm steel tip

Behaviour explained by an effective power-law model with viscosity cut-offs and slightly slower shear-thinning

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Validation results

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• Step 1: pressure-massflux dependency

Viscosity curves of CNF suspensions: rheometry with the parallel plate geometry

Kumar et al. (2016) Ind Eng Chem Res 55:3603

Effective power-law fluid model with viscosity cut-offs at both low and high shear rates

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Validation results

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• Step 2: printing parameters-line profile dependency

Option A: 2D image analysis (for the TCNF gel)

Option B: 3D profilometry (for more rigid gels)

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Validation results

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• Step 2: printing parameters-line profile dependency

Sensitive to the contact angle value Roughly 100 μm resolution feasible with successful massflux prediction

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Conclusions & further work

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• Modelling the 3D printing of nanocellulose hydrogels is feasible with currently available CFD tools

• Conventional rheometry is not necessarily a sufficient basis for the needed rheology models

– High shear rate behaviour dominates the flow within the printer head

– Low shear rate behaviour dominates the deposition process

• To be considered

– Rheometry (or capillary viscosimetry) at higher shear rates

– Thixotropic effects

– Boundary conditions at solid surfaces (slip etc.)

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Goniometry

Predicts hydrogel mass flow for a given operating pressure

Predicts deposition profile for given printing conditions

Summary

Rheometry

Rheology model

CFD simulations

Something

Experiments

Deposition model

Printer head model