Sebastian Marussi’s research while affiliated with University College London and other places

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Publications (61)


Physical twin of an industrial quad-laser powder bed fusion machine for high-speed multi-modal sensing measurements
  • Article

April 2025

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30 Reads

Materials & Design

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Sebastian Marussi

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Andrew Farndell

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[...]

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To faithfully capture the laser-material interaction and subsequent process dynamics during the industrial laser powder bed fusion process, we developed a Quad-laser in situ and operando process replicator (or the Quad-ISOPR) – a physical twin that mimics the Renishaw plc.’s RenAM 500Q multi-laser additive manufacturing system that can be used in laboratories and synchrotron radiation facilities. The Quad-ISOPR allows users to take synchrotron X-ray measurements while collecting correlative high-speed optical and photodiode imaging within a 10 ns delay, mounted in-line with the scanning lasers. We have selected case studies to demonstrate: (i) multi-modal data acquisition; (ii) signal processing using continuous wavelet transform; (iii) the study of laser drilling with ultra high-speed X-ray imaging; (iv) process mapping of melting and defect modes in Ti-6Al-4V; and lastly, (v) we showcase the interaction between multi-lasers on a Ti-6Al-4V alloy. Our experimental approach allows end-users to explore the process-structure–property relationship in multi-laser material processing and to use such the physical twin to design new materials and processes.


Magnetic modulation of keyhole instability during laser welding and additive manufacturing

February 2025

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231 Reads

Science

Keyhole instability during laser welding and laser powder bed fusion (LPBF) can cause keyhole collapse and pore formation. Using high-speed x-ray imaging, we demonstrate that the flow vortex–induced protrusion on the rear keyhole wall is crucial in initiating keyhole instability. Applying a transverse magnetic field suppresses the keyhole instability by driving a secondary thermoelectric magnetohydrodynamics (TEMHD) flow that alters the net flow vortex. This minimizes protrusions and large-amplitude keyhole oscillations. The suppression effectiveness depends on the laser scanning direction relative to the magnetic field orientation because this controls the Seebeck effect–induced Lorentz force’s direction. We show that at LPBF length scales, electromagnetic damping is weak, and for alloys with a large Seebeck coefficient, TEMHD becomes the dominant mechanism controlling flow behind the keyhole.


Novel insights into dynamics and timescales of vesiculation in basaltic magmas by in situ HP-HT X-ray synchrotron radiography experiments
  • Conference Paper
  • Full-text available

September 2024

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45 Reads

Transitions between effusive and explosive styles at basaltic volcanoes are strongly dependent on how easily gas can decouple from magma during ascent. Stronger gas-melt coupling favours highly explosive eruptions, whereas a weaker coupling promotes lava fountaining and lava flows. However, the mechanism fostering the transition from closed- to open-system degassing is still poorly understood, due to a lack of direct observations of bubble dynamics under natural magma ascent conditions. A series of in-situ experiments were performed at Diamond Light Source (United Kingdom) combining X-ray synchrotron radiography with a novel high-pressure/high-temperature X-ray transparent Internally Heated Pressure Vessel apparatus to directly observe and quantify in 2D bubble growth and coalescence in a basaltic magma from 100 MPa to the surface, in real-time. This new study provides unique quantitative information on bubble growth, expansion and coalescence through time. We found that for low-viscosity basaltic magmas, bubbles coalesce and recover a spherical shape within 3 s, implying that, for lava fountaining activity, both gas and melt remain coupled during the ascent up to the last hundred metres of the conduit. For higher viscosity magmas, instead, the recovery time becomes longer, promoting connected bubble pathways leading to some degree of decoupling that we directly observed as bubbles expand until they connect to an open pathway and then contract as gas escapes. This new apparatus combined with X-ray synchrotron radiography is an invaluable tool to capture and quantify bubble kinetics in basaltic magmas at natural pre- and syn-eruptive conditions, which are fundamental to improve our understanding of magma behaviour and mitigating the volcanic risk associated with basaltic systems.

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Synchrotron Tomography-Based Finite Element Analysis of Vertebral Endplate Loading Reveals Functional Roles for Architectural Features

September 2024

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66 Reads

Lower back pain is linked to vertebral biomechanics, with vertebral endplates (VEPs) playing a key role in vertebral load transfer and distribution. Synchrotron computed tomography (sCT) allows for detailed visualisation of the microstructure of intact VEPs under near-physiological loads and, when coupled with digital volume correlation (DVC), can be used to quantify three-dimensional (3D) strain fields with nanoscale resolution. Herein, we spatially couple DVC data and an image-based finite element model (FEM) to determine the material properties of murine VEPs. This model was then extended to investigate VEP biomechanics under different motions and disease conditions to reveal that VEP protrusions are important for load absorption and redistribution under different motions and predicted that abnormal intervertebral disc (IVD) stress may underpin osteoporosis- and pycnodysostosis-related IVD degeneration. Our study validates the efficacy of using DVC to increase the accuracy of FEM predictions and highlights that these methodologies may be scalable to large animals and humans.


Fig. 1. Variation of incremental bubble growth rate and bubble radius with pressure. Plots showing (A) incremental bubble growth rate (ΔG R ) and (B) bubble radius versus pressure for the Superliq_dec experiments. in (A), the decompression rate (megapascal per second) for each run is reported in parentheses. insets show magnification of ΔG R (A) and bubble radius (B) at low pressure (P < 3 MPa). Both (A) and (B) show the comparison between the observed bubble growth rates and radius measured from the decompression experiments with those calculated (table S5) using the numerical bubble growth model of coumans et al. (44). numerical results are obtained assuming different decompression rates (0.05 and 0.08 MPa s −1 ) and different volatile contents (1 and 2 wt % of h 2 O). Plotted numerical simulations have been computed using the etna composition (table S1), a magma density of 2700 kg m −3 , and assuming N b = 10 12 m −3 .
Fig. 2. Variation of incremental expansion rate with pressure. Plot showing incremental expansion rate (ΔE R ) versus pressure for (A) Subliq_dec and (B) Superliq_dec experiments. in (A), the liquid viscosity (log Pa·s) for each run is reported in parentheses.
Fig. 3. Radiographic images of Superliq_Dec runs showing coalescence steps and timescales. (1) contact between two bubbles; (2) bubble interconnection during which bubble walls thin (bubbles assume an "eight" shape with cusps on their walls); (3) bubble coalescence after the rupture of the thinned films (replacement of the cusps in the "eight" shape by smooth bumps on the walls of the new coalesced bubble); (4) bubbles assume an oval shape and lastly recover to a spherical one.
Fig. 4. Sketch reporting bubble growth and coalescence within the conduit and mechanisms of coupling (up to the last ~100 m) and decoupling between volatiles and magma. Plots show bubble recovery time and magma time to surface versus pressure. in particular, the time required by magma to reach the surface for each pressure within the conduit using the lava fountaining simulations performed by la Spina et al. (69) for Kilauea is reported.
Direct observation of degassing during decompression of basaltic magma

August 2024

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254 Reads

Science Advances

Transitions in eruptive style during volcanic eruptions strongly depend on how easily gas and magma decouple during ascent. Stronger gas-melt coupling favors highly explosive eruptions, whereas weaker coupling promotes lava fountaining and lava flows. The mechanisms producing these transitions are still poorly understood because of a lack of direct observations of bubble dynamics under natural magmatic conditions. Here, we combine x-ray radiography with a novel high-pressure/high-temperature apparatus to observe and quantify in real-time bubble growth and coalescence in basaltic magmas from 100 megapascals to surface. For low-viscosity magmas, bubbles coalesce and recover a spherical shape within 3 seconds, implying that, for lava fountaining activity, gas and melt remain coupled during the ascent up to the last hundred meters of the conduit. For higher-viscosity magmas, recovery times become longer, promoting connected bubble pathways. This apparatus opens frontiers in unravel-ing magmatic/volcanic processes, leading to improved hazard assessment and risk mitigation.



In situ 4D crystallisation of magma via HP-HT X-ray transparent IHPV

February 2024

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179 Reads

Crystallisation processes affect the rheological properties of magma and, hence, its ability to move and rise in the crust and erupt. Here we propose in situ crystallisation experiments to study for the first time crystal nucleation and growth in a tephritic magma at high pressure and high temperature under water saturated conditions. We combined fast synchrotron x-ray microtomography with a unique X-ray transparent Internally Heated Pressure Vessel (IHPV) apparatus to simulate magma storage conditions within the crust at pressures ≤100 MPa and temperatures ≤1200 °C in presence of volatiles (H2O). Through the experiments we investigated crystal and bubble nucleation and growth during single step and continuous cooling. At first we pressurised the system with gas (He), and then we heated up to 1140 °C. At this point we continued the experiments via (1) single step cooling (ΔT = 20 °C) at temperatures between 1140 and 1080 °C with a cooling rate of 45 °C/min between each step, and (2) continuous cooling at cooling rates of 0.5 and 1 °C/min. We worked at fixed pressures typical of shallow to intermediate crustal storage (P = 20-50 MPa, corresponding to a depth of ~1-2 km), under H2O-saturated conditions. We were able to directly observe and record vesiculation and crystallization kinetics in both experimental settings. This new apparatus in combination with fast synchrotron x-ray microtomography allow us to capture, visualize and quantify in 4D (3D + time) crystallisation and vesiculation kinetics in magmas at pre- and syn-eruptive conditions, which are fundamental to improve our understanding of magma behaviour and mitigate the volcanic risk associated with these systems. This apparatus, indeed, opens a new frontier in unravelling the processes which control volcanic eruptions, leading to improve the current numerical models by integrating new experimental constraints, and, in turn, hazard assessment and risk mitigation.


Pore evolution mechanisms during directed energy deposition additive manufacturing

February 2024

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725 Reads

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38 Citations

Porosity in directed energy deposition (DED) deteriorates mechanical performances of components, limiting safety-critical applications. However, how pores arise and evolve in DED remains unclear. Here, we reveal pore evolution mechanisms during DED using in situ X-ray imaging and multi-physics modelling. We quantify five mechanisms contributing to pore formation, migration, pushing, growth, removal and entrapment: (i) bubbles from gas atomised powder enter the melt pool, and then migrate circularly or laterally; (ii) small bubbles can escape from the pool surface, or coalesce into larger bubbles, or be entrapped by solidification fronts; (iii) larger coalesced bubbles can remain in the pool for long periods, pushed by the solid/liquid interface; (iv) Marangoni surface shear flow overcomes buoyancy, keeping larger bubbles from popping out; and (v) once large bubbles reach critical sizes they escape from the pool surface or are trapped in DED tracks. These mechanisms can guide the development of pore minimisation strategies.


Direct observation of degassing and crystallisation of magma via HP-HT X-ray transparent Internally Heated Pressure Vessel

Transitions in eruptive style during volcanic eruptions are strongly dependent on how easily gas can decouple from magma during ascent. Stronger gas-melt coupling favours highly explosive eruptions, whereas a weaker coupling promotes lava fountaining and lava flows. However, the mechanism fostering the transition from closed- to open-system degassing is still poorly understood, due to a lack of direct observations of bubble dynamics under natural magma ascent conditions. We combined X-ray synchrotron radiography with a novel high-pressure/high-temperature X-ray transparent Internally Heated Pressure Vessel apparatus to directly observe and quantify in 2D bubble growth and coalescence from 100 MPa to the surface, in real-time. We found that for low-viscosity basaltic magmas, bubbles coalesce and recover a spherical shape within 3 s, implying that, for lava fountaining activity, both gas and melt remain coupled during the ascent up to the last hundred metres of the conduit. For higher viscosity magmas, instead, the recovery time becomes longer, promoting connected bubble pathways leading to some degree of decoupling that we directly observed as bubbles expand until they connect to an open pathway and then contract as gas escapes. Together with degassing, also crystallisation processes play a key role in determining transitions in eruptive style by affecting the rheological properties of magma and, hence, its ability to move and rise in the crust and erupt. For this reason, we combined fast synchrotron x-ray microtomography with our X-ray transparent Internally Heated Pressure Vessel to simulate magma storage conditions within the crust at pressures ≤100 MPa and temperatures of ≤1200 °C in presence of volatiles (H2O). These experiments allowed us to capture, visualise and quantify in 4D (3D + time) crystallisation and vesiculation kinetics in a tephritic magma at pre and syn-eruptive conditions, which are fundamental to improve our understanding of magma behaviour and mitigating the volcanic risk associated with tephritic systems like the one that fed the 2021 Tajogaite eruption (Canary Islands). This apparatus opens a new frontier in unravelling the processes which control volcanic eruptions, leading to improve the current numerical models by integrating new constraints, hazard assessment and risk mitigation.



Citations (31)


... These thermal fluctuations cause gases trapped within the porous substrate to expand and escape, forming voids at the interface between the substrate and the deposited material. The magnitude of these thermal gradients plays a crucial role in determining the extent of outgassing and subsequent defect formation [43,44]. ...

Reference:

Laser-Based Directed Energy Deposition with Mullite: A Necessary Step For Lunar Regolith Printing
Pore evolution mechanisms during directed energy deposition additive manufacturing

... This result suggests that the increase in molten pool magnitude could be accelerated under Case-3 rather than Case-1 owing to reinforced heat accumulation, resulting from the short return time of the electron beam. Bhatt et al. demonstrated that liquid metal can be pushed towards the back of the melt pool via Marangoni convection, and it causes surface undulation due to the Plateau-Rayleigh instability [44]. As noted previously in the single-track simulation, rapid fluid flow stabilizes the molten pool surface by improving fluid feeding during solidification (Fig. 12f). ...

In situ characterisation of surface roughness and its amplification during multilayer single-track laser powder bed fusion additive manufacturing
  • Citing Article
  • October 2023

Additive Manufacturing

... They confirmed that the solidification process is a key factor in controlling this phenomenon. Additionally, they found that adding TiB2 powder to the process could significantly reduce cracking [338]. Tristan G. Fleming et al., 2023, observed crack formation using novel equipment integrated with coherent imaging (ICI) in an X-ray facility. ...

In situ X-ray imaging of hot cracking and porosity during LPBF of Al-2139 with TiB2 additions and varied process parameters
  • Citing Article
  • June 2023

Materials & Design

... The maximum velocity exceeds 0.2 m/s in the absence of the electromagnetic field, which can be explained by the effect of Marangoni flow (seeFig. 39)[293]. In another study, Kai Zhang et al. (2024) estimated bubble velocities in the circulation zone of the laser DED process and developed simulation models to predict these velocities, which were validated through experiments. ...

Thermoelectric magnetohydrodynamic control of melt pool flow during laser directed energy deposition additive manufacturing

Additive Manufacturing

... Tristan G. Fleming et al., 2023, observed crack formation using novel equipment integrated with coherent imaging (ICI) in an X-ray facility. However, this publication did not provide more detailed information or discussion on the mechanism of this phenomenon [339]. Yunhui Chen et al., 2023, utilized an X-ray facility with 200,000 pfs to observe hot cracking formation during the LBP process for aluminum alloy. ...

In situ Correlative Observation of Humping-Induced Cracking in Directed Energy Deposition of Nickel-Based Superalloys
  • Citing Article
  • April 2023

Additive Manufacturing

... Importantly, XPCT provides a scalable and isotropic resolution without destructive slicing of the specimen and quantitative density-based contrast (9)(10)(11)(12)(13)(14)(15)(16)(17). At the same time, XPCT is extremely flexible concerning the sample environment (18)(19)(20). Recently, complementing histological investigation, XPCT was used to study murine (21) and human placenta vasculature and tissue architecture (22)(23)(24). ...

Preparation of large biological samples for high-resolution, hierarchical, synchrotron phase-contrast tomography with multimodal imaging compatibility
  • Citing Article
  • March 2023

Nature Protocols

... The ISOPR chamber [36] (Fig. 1 -(6)) is mounted on a breadboard inside the laser enclosure. The chamber is equipped with multiple gas flow mechanisms: (i) a knife-edge gas flow on the top window; and (ii) a flowing gas atmosphere above the powder bed in which the gas flow velocity above the bed has been simulated in [37]. The laser beam ( Fig. 1 -(7)) and the X-ray beam ( Fig. 1 - (8)) enter from the top and the side of the ISOPR chamber, respectively, during in situ and operando Xray imaging experiments. ...

Quantification of Interdependent Dynamics during Laser Additive Manufacturing Using X‐Ray Imaging Informed Multi‐Physics and Multiphase Simulation

... In 2007, A. Olivo and colleagues from the University of London introduced a phasecontrast imaging method based on wavefront coding [53], referred to as the coded aperture method or edge illumination method [54]. This non-coherent imaging technique [55,56] utilizes standard X-ray tubes to achieve image quality comparable to that obtained under synchrotron radiation source conditions. The schematic diagram of the experimental setup is illustrated in Figure 10. ...

Time resolved in-situ multi-contrast X-ray imaging of melting in metals

... Test data DSC CLD NSD (t = 1) NSD (t = 0) ASSD kidney tissues from the same organ, reflecting its capability to learn kidney anatomy and thereby enhancing the efficiency of the labeling process. It also shows the expected improvement by comparison to the other three experiments, indicating the challenges with accounting for anatomical variation across human samples, or variations in the data aquisition and data reconstruction parameters see 16,134,142 for details on protocol variations. ...

A multiscale X-ray phase-contrast tomography dataset of a whole human left lung

Scientific Data

... Most high-speed X-ray imaging studies have focussed on the laser powder bed fusion (LPBF) AM process studying the laser melting modality [14], melt pool flow [15,16], or the development of laser keyholes and subsequent porosity formation [17,18]. A few in situ DED X-ray studies have been carried out to observe the influence of processing parameters on melt pool geometries and build quality [19,20] as well as powder capture and melting [21,22]. Various porosity formation mechanisms have also been observed in DED, including porosity inside powder particles, entrapped gas on the powder surface, or keyhole induces pores for this specific system [23,24]. ...

Sinter formation during directed energy deposition of titanium alloy powders

International Journal of Machine Tools and Manufacture