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This study experimentally investigates passive drag reduction on a sphere using azimuthally spaced surface protrusions under subcritical Reynolds numbers, focusing on the effects of the protrusion number at fixed surface coverage. The proposed surface modification strategy, termed partial protrusions, maintains a constant total protruded area while varying the number of protrusions $N$, thereby adjusting their azimuthal spacing. The objective is to determine whether such configurations can outperform the conventional full protrusion, in which protrusions continuously surround the azimuthal direction, and to elucidate the flow mechanisms behind any observed enhancement. Drag and flow field measurements reveal that increasing $N$ significantly improves aerodynamic performance. When $N$ exceeds a certain threshold, the partial-protrusion configuration achieves a greater drag reduction than the full-protrusion case, despite using only half the surface coverage. For low $N$, asymmetric pressure distributions across the protruded and smoothed sides induce unsteady separation delay, leading to shear-layer oscillations and elevated turbulent kinetic energy. As $N$ increases, the azimuthal spacing between protrusions decreases, promoting stable interaction between the two sides and leading to separation delay farther downstream than in the full-protrusion case, along with suppression of flow unsteadiness. These results demonstrate that a well-designed partial-protrusion configuration can outperform the full-protrusion configuration in drag reduction and unsteadiness control, offering new insights into effective passive flow control strategies for bluff body flows.
A 10 m-thick and laterally extensive, mixed siliciclastic–carbonate heterolithic unit occurs between coastal quartz arenites (Banaganapalle Formation) and open marine outer-shelf carbonate platform (Narji Limestone) in the Mesoproterozoic Kurnool sea, India. While the dynamics of mixed siliciclastic–carbonate systems are well studied in the Phanerozoic, comparable Proterozoic examples remain poorly documented and are notably absent from the Indian subcontinent. High-resolution stratigraphic, facies, and petrographic analyses of this heterolithic unit reveal a progressive transition from outer-shelf to storm-dominated middle-to inner-shelf settings, periodically disrupted by episodic high-energy depositional events. Two distinct mixing modes are identified: (i) lithofacies to microscopic-scale strata mixing (Punctuated Mixing), linked to high-frequency sea-level oscillations, and (ii) bed-scale compositional mixing (In-Situ Mixing) of nearshore siliciclastics and subtidal carbonate mud. These findings demonstrate that repeated siliciclastic influx did not inhibit contemporaneous carbonate precipitation, documenting previously unrecognized mixed sedimentation between the Banaganapalle siliciclastics and the Narji carbonates, and advancing understanding of mixed-system dynamics in Proterozoic sedimentary rocks. The widespread occurrence of mixed heteroliths in the Kurnool sub-basin is interpreted to have formed during a phase of rapid subsidence that drove marine transgression, plausibly associated with a rise in sea-level, linked to post-Columbia breakup. Lithostratigraphically correlative heterolithic intervals in the intracratonic Bhima, Pranhita–Godavari and Kurnool basins suggest a regionally extensive, basin-wide Mesoproterozoic transgressive event across the Southern Indian Block. This heterolithic deposit may provide a key stratigraphic marker for regional correlation and yield new insights about the resilience of a Proterozoic non-skeletal carbonate factory and its interaction with episodic siliciclastic input.
Accurate identification of potentially toxic element (PTE) sources is crucial for effective risk mitigation; however, the complex solubility of trace elements hinders such identification. Here, levels of PTEs in the dust of 105 leaf samples from 21 sites in urban Guiyang (China) were measured and positive matrix factorization was applied to help identify PTE sources. These results were validated through correlating PTE concentrations with the land-use areas surrounding the sample sites. Ni and As in the leaf dust were linked to the cleanest conditions, followed by Cr. Conversely, Zn, Cu, Cd and Pb were associated with higher pollution levels. Three primary sources of PTEs were identified, with traffic-agriculture emissions being the largest contributor at 40.42%. Natural sources followed closely at 39.41%, while industrial processes accounted for the remaining 20.17%. High-pollution areas were clustered around traffic hubs, where frequent vehicle idling and acceleration increased emissions. As traffic emission was a major source of atmospheric pollution, targeted flow optimization is needed to reduce risks of human exposure.
We investigate the unsteady lift response of compliant membrane wings in hovering kinematics by combining analytical inviscid theory with experimental results. An unsteady aerodynamic model is derived for a compliant thin aerofoil immersed in incompressible inviscid flow of variable free-stream velocity at high angles of attack. The model, representing a spanwise section of a hovering membrane wing, assumes small membrane deformation and attached flow. These assumptions are supported by experiments showing that passive membrane deformation suppresses flow separation when hovering at angles of attack up to $55^\circ$. An analytically derived expression is obtained for the unsteady lift response, incorporating the classical Wagner and Theodorsen functions and the membrane dynamic response. This theoretical expression is validated against experimental water-tank measurements that are performed on hovering membrane wings at angles of attack of $35^\circ$ and $55^\circ$. Data from membrane deformation measurements is applied to the theoretical lift expression, providing the theoretical lift response prediction for each of the available experimental scenarios. Results of the comparison show that the proposed theory accurately predicts unsteady lift contributions from membrane deformation at high angles of attack, provided the deformation remains small and the flow is attached. This agreement between inviscid theory and experimental measurements suggests that when flow separation is suppressed, the unsteady aerodynamic theory is valid well beyond the typical low-angle-of-attack regime.
The present study investigates the novel occurrence of rare garnet-aluminosilicate-bearing metapelitic enclaves from the Western Lohit Plutonic Complex in the Dibang Valley, Arunachal Pradesh, Northeastern India. Textural, mineralogical, thermobarometric and phase equilibrium modelling analyses reveal a complex polymetamorphic evolution characterized by two distinct stages. The first stage corresponds to a pre-Himalayan low-pressure, high-temperature event likely linked to Cretaceous magmatism, evidenced by relict andalusite porphyroblasts. The second stage reflects Barrovian-type Himalayan metamorphism associated with India-Asia collision, marked by peak assemblages of garnet, kyanite and melt formed near the solidus. Thermobarometric studies estimate near-peak metamorphic conditions at approximately 650 ± 25 °C and 7–9 kbar. Consistently, Pressure-temperature phase equilibrium modelling indicates that garnet core compositions record an initial metamorphic event at lower pressure (∼5.5 kbar) and temperature (∼550 °C), reflecting prograde burial prior to peak conditions. Peak metamorphic conditions, constrained by pressure-temperature phase equilibrium modelling, are estimated at approximately 670 °C and 8.5 kbar. Microstructural observations indicate muscovite-dehydration melting is the primary mechanism for incipient melt generation in the studied metapelite, with the melt largely retained within the rock. Ti-in-biotite thermometry reveals cooling temperatures of 560–590 °C during final exhumation. The rocks experienced a clockwise P–T path involving prograde burial, near-isothermal decompression and retrograde cooling, consistent with thrust duplexing and exhumation along the Lohit thrust shear zone. These findings provide new constraints on the metamorphic evolution and partial melting processes during Himalayan orogenesis in the northern Indo-Burma region.
Specimens of shrimp Heptacarpus maxillipes (Thoridae) infected by parasitic barnacle Sylon hippolytes (Rhizocephala) were found for the first time along the Kuril Islands at a depth of 241–670 m. It is the second host from the genus Heptacarpus. Total number of hosts of S. hippolytes is currently 24. Carapace length of the infected shrimps ranged from 3 to 10 mm. Hosts had one or two parasitic externae of S. hippolytes. The size of the externa ranged from 1.5 to 9.0 mm in length and from 1.0 to 4.0 mm in height. Retinacula were not found. A single colleteric gland was present. Receptacles were absent. Regeneration of the ovary in the ovigerous externa was not observed. Sylon hippolytes produces only one larval generation. Larvae are hatched as small cyprids. Phylogenetic reconstruction confirmed the belonging of our specimens to the monophyletic clade of S. hippolytes with genetic distances between subclades from 6.96 to 8.4%. High values of intraspecific distances in S. hippolytes from different areas may point to cryptic speciation within this rhizocephalan.
The family Yoldiidae encompasses protobranch bivalves with notable diversity in deep-sea habitats, with Yoldiella Verrill and Bush (1897) as the most speciose genus. In Brazilian waters, 11 species of Yoldiella have been recorded, including Yoldiella lapernoi Benaim and Absalão (2011) and Yoldiella paranapuensis Benaim and Absalão (2011), two species with similar shell morphology and overlapping geographical distributions. This study re-evaluated the taxonomic distinction between these two Yoldiella species using a combination of morphometric approaches. Size and growth rate comparisons were conducted using analysis of covariance and Bayesian model selection. The shell outline was compared using elliptical Fourier descriptors. The results did not support the current separation of these taxa. Instead, they reveal that the observed morphological differences are attributable to ontogenetic variation, indicating Y. paranapuensis as a juvenile stage of Y. lapernoi. This finding supports the synonymy of these two nominal species and highlights the importance of ontogenetic context in taxonomy.
The first report of Ophiophragmus luetkeni occurred in the British Virgin Islands; however, it was also recorded in Brazil, the United States Virgin Islands, and Trinidad and Tobago, yet its occurrence in Colombia was previously lacking. Between 2023 and 2024, four specimens were collected from sandy and muddy substrates in Cispatá Bay, Colombian Caribbean. Taxonomic identification was conducted through morphological observations and microstructural analysis using Scanning Electron Microscopy. A comparative table for Ophiophragmus species recorded in Colombia are also provided. This new record increases the number of Ophiophragmus species in Colombia to three, contributing to the country’s marine biodiversity and expanding the knowledge of O. luetkeni distribution.
Smooth surface features were recently found to stabilise stationary cross-flow instability (CFI) of swept-wing boundary layers, thus holding potential for passive laminar flow control. Notably, the effect of surface features on the transition location exhibited a significant dependence on the CFI amplitude. In this work, numerical solutions of the harmonic Navier–Stokes (HNS) equations are used to explore the impact of a smooth surface hump on the linear and nonlinear development of stationary CFI under various perturbation amplitudes. Linear simulations identify regions of successive inhibited and enhanced perturbation growth. Despite the recovery of the base flow and perturbation kinetic energy to the reference (i.e. no-hump) state, significantly reduced perturbation growth is observed. The distorted perturbation profile due to the interaction with the hump is postulated to be responsible for this. Increasing the perturbation amplitude results in a response of the flow that is qualitatively similar to the linear case, albeit with increasing local destabilisation of new fundamental (i.e. primary wavelength) structures and higher-order harmonics near the wall. An energy budget analysis reveals that the growth of the fundamental incoming CFI is inhibited through the reduced effectiveness of the lift-up mechanism downstream of the hump. This is preceded by a spatial perturbation shape deformation, governed by (spanwise) transport terms. The results suggest that stabilisation of incoming stationary CFI via smooth surface humps is most effective at low incoming perturbation amplitudes. At higher perturbation amplitudes, newly formed near-wall structures, pre-conditioned by the incoming CFI, overtake the incoming CFI and could anticipate the transition process.
Plastic pollution represents far more than an environmental crisis—it serves as the gateway to a global meta-crisis encompassing climate change, hyper-consumption, biodiversity loss, and profound threats to human health. This letter examines plastic’s role as both catalyst and symptom of unsustainable global systems, arguing that addressing the plastic crisis provides a roadmap for broader systemic transformation.
Since mass production began in the 1950s, humanity has produced over 10 billion tonnes of plastic, with annual waste now reaching 400 million metric tonnes. Production is forecast to triple within 25 years, consuming one-fifth of the global carbon budget, with 90% of emissions occurring during production.
Plastics now permeate the human body. Over 16,000 chemicals are potentially present in plastics, with only 6% globally regulated. Recent research estimates 13% of cardiovascular deaths in individuals aged 55–64 are attributable to phthalates, while microplastics accelerate cancer development.
Solutions require comprehensive legislative frameworks creating financial risk and accountability. The Health Scientists’ Global Plastics Treaty, produced by the Plastic Health Council, proposes a roadmap to change, with measures such as a 70% reduction in virgin plastic production by 2040 and elimination of chemicals of concern. Ultimately, the plastic crisis offers humanity a tangible challenge that could catalyse essential systemic change toward regenerative systems working within planetary boundaries.
Preventing human-caused extinctions is a foundational aim of conservation. However, in addition to causing extinctions, humans have moved numerous species to new areas. A considerable percentage of these are threatened in their native ranges. Broadening our conservation ethos to include introduced species is contentious and requires critical thinking in empirical and normative dimensions to negotiate between conflicting conservation goals. Here, we present a series of questions to inspire critical thinking in the negotiation of these conflicts. Empirically, we suggest that conservationists should consider whether the effects of introduced species are due to their non-nativeness per se or are simply a consequence of the organism having a metabolism and taking up space. Importantly, this requires proper scientific comparison to the effects of similar native organisms – otherwise many claims of ‘harm’ are unfalsifiable and could be used to justify the eradication of any organism. We further propose questions to help conservationists sort facts from normative values, which often wear empirical clothes. Through empirical rigor, value transparency and critical justification of these values, we believe that twenty- first century conservation can become a future-facing and pluralistic discipline with a heightened ability to prevent extinctions in an increasingly unpredictable and novel biosphere.
The extent to which continental acidity during the Early Triassic varied with latitude remains insufficiently constrained, despite its relevance for understanding environmental stress and biotic recovery patterns across the Smithian–Spathian boundary (SSB). We examined the abundance, textures and compositions of strontium-rich hydrated aluminium phosphate–sulphate (APS) minerals in 179 continental samples spanning tropical to high paleolatitudes in both hemispheres. APS minerals display broadly comparable early-diagenetic features across sections, indicating formation shortly after deposition under acidic meteoric conditions. Their distribution suggests a latitudinal trend: APS contents commonly exceed 0.1 vol.% in equatorial western peri-Tethyan basins, where faunal and floral records are sparse during the SSB, whereas concentrations decrease towards higher latitudes and are rare beyond ∼40° in both hemispheres. This pattern does not appear to correlate with lithological or textural variability and may reflect spatial differences in the intensity or duration of acidification linked to Siberian Traps volcanism. Equatorial basins thus likely experienced more prolonged or recurrent acidic episodes, whereas higher-latitude areas may have been subject to comparatively attenuated effects, potentially contributing to earlier ecological recovery. These results provide a useful framework for evaluating continental acidification and its environmental implications during the interval following the end-Permian mass extinction (EPME).
We have been conducting mass-balance monitoring on Aldegondabreen since the early 21st century. Over the most recent five year period (2019/20–2023/24), the glacier has experienced its most negative mass balance, averaging −2.0 m w.e. a−1. This dramatic loss is linked to rising air temperatures, with several of the warmest years on record for the Arctic land occurring during this interval. In 2024, for the first time, the critical threshold of 1.5°C above pre-industrial levels was exceeded globally, and this resulted in the lowest annual balance observed since the beginning of our monitoring program (−2.48 m w.e. a−1). Archival evidence indicates that such intense melting is unprecedented since at least 1911, which marked the end of the Little Ice Age in the region. As of 2025, the glacier’s mean ice thickness has been estimated at 39 m (33 m w.e.) meaning that the loss of 10 m w.e. in just the last five years is an enormous change.
Fluids at supercritical pressure (SCP) exhibit significant real-fluid effects across the pseudo-critical point, which challenges the validity of the existing wall-scaling laws developed under atmospheric pressure condition. This study revisits prior efforts on the temperature-based transformation for the collapse of mean scalar profiles, emphasising the difficulties in accurately describing universal characteristics of thermal boundary layers at SCP. To address this, a novel thermal scaling law using enthalpy transformation is proposed by incorporating the chain rule and heat flux balance. This transformation effectively accounts for variations in the near-wall thermophysical properties associated with the scalar profile while excluding the gradient of isobaric specific heat capacity-related terms. The proposed scaling law demonstrates substantially improved alignment of transformed mean scalar profiles in SCP channel flows at different wall-temperature differences and Reynolds numbers. Additionally, the enthalpy transformation shows superior performance compared with the existing enthalpy–velocity relations, particularly near the heated-wall region where the fluid thermodynamic states undergo the pseudo-boiling process. The present work could facilitate the development of universal wall model in supercritical flows, enabling rapid and reliable heat transfer predictions in practical applications.
Englacial layers are a product of historic accumulation and are reshaped by ice deformation. Hence, radio-echo sounding (RES), which can resolve englacial layering, has been adopted as an observational tool to infer ice age and ice dynamics from ice stratigraphy. However, the commonly applied synthetic aperture radar focusing algorithms, used to improve image resolution, are either i) incoherent or ii) optimized for the ice-bed interface. Dipping specular reflectors, such as englacial layers, are then lost during focusing. Instead, we focus the RES measurements using subapertures, synthetically squinting the radar beam toward orthogonal incidence for every dipping layer. We then either recombine all subapertures or reject those with low signal to generate an image that resolves all englacial targets together. We apply these methods to both along- and across-flow RES images at Academy Glacier, East Antarctica, which has significant englacial layer relief, especially perpendicular to the ice-flow direction. Our method significantly elevates signal power for dipping englacial layers ($ \gt $15 dB), and quantifiably improves layer continuity compared to other processed data products. This squinted focusing approach enables novel studies of ice deformation (as recorded in englacial layering) in the presence of complex basal topography and heterogeneous substrate properties.
Direct numerical simulation is performed to study the effects of spanwise curvature on transitioning and turbulent boundary layers. Turbulent transition is induced with an array of resolved cuboids. Spanwise curvature is prescribed using a novel approach with a body force that is applied orthogonally to the bulk flow to curve the mean free-stream streamlines at a set radius. The flows are analysed in a streamline-aligned coordinate system. Although the radius of curvature is large compared with the size of the boundary layer, its effects on the development of the boundary layer are appreciable. The results indicate that spanwise curvature induces a non-uniform mean secondary flow and alters the structure of turbulence within the boundary layer. Analytical expressions for the crossflow are derived in the viscous sublayer and log layer. These alterations are visible as changes in the distribution of the turbulent stresses and alignment of the vortical structures with the mean flow. These modifications are responsible for a misalignment between the Reynolds stress tensor and the velocity gradient tensor, which has important consequences for the validity of the widely used Boussinesq turbulent viscosity hypothesis in Reynolds-averaged Navier–Stokes models. Spanwise curvature was observed to decrease turbulent kinetic energy. These results have important implications on the development of turbulence in general applications, such as the flow over a prolate spheroid.
Previous studies show that at the small scales of stably stratified turbulence, the scale-dependent buoyancy flux reverses sign, corresponding to a conversion of turbulent potential energy (TPE) back into turbulent kinetic energy (TKE). Moreover, the magnitude of the reverse flux becomes stronger with increasing Prandtl number $\textit{Pr}$. Using a filtering analysis we demonstrate analytically how this flux reversal is connected to the mechanism identified in Bragg & de Bruyn Kops (2024 J. Fluid Mech. vol. 991, A10) that is responsible for the surprising observation that the TKE dissipation rate increases while the TPE dissipation rate decreases with increasing $\textit{Pr}$ in stratified turbulence. The mechanism identified by Bragg & de Bruyn Kops, which is connected to the formation of ramp–cliff structures in the density field, is shown to give the scale-local contribution to the buoyancy flux. At the smallest scales this local contribution dominates and explains the flux reversal, while at larger scales a non-local contribution is important. Direct numerical simulations of three-dimensional statistically stationary, strongly stably stratified turbulence confirm the theoretical analysis, and indicate that, while on average the local contribution only dominates the buoyancy flux at the smallest scales, it remains strongly correlated with the buoyancy flux at all scales. The results show that ramp cliffs are not only connected to the reversal of the local buoyancy flux but also the non-local part. At the small scales (approximately below the Ozmidov scale), ramp structures contribute exclusively to reverse buoyancy flux events, whereas cliff structures contribute to both forward and reverse buoyancy flux events.
A stakeholder structured engagement process at the Sustainable Water Infrastructure Management (SWIM) conference and workshop was held in December 2024. The participants identified critical current and future issues facing the water sector that are synthesized in this paper. In particular, they highlighted issues of water systems’ vulnerability and lack of resilience to hazards and stressors; inequities associated with water scarcity; and water quality problems – all affected by natural or man-made influences. The Smart One Water (S1W) vision was the baseline for the SWIM 2024 conference. This paper expands the S1W vision with a synthesis of the conference discussions about S1W-related fundamental concepts, practices and implementation barriers. It includes initial recommendations – based on a digital, data-focused, stakeholder-driven approach – with expert representatives of the public and private water supply sectors, academia, government and policymakers tasked to generate real-world adaptable ideas and practical solutions. Specifically, S1W envisions a future where water management and governance silos are eliminated to provide the necessary collaboration to enable efficient, resilient, affordable and equitable water access capable of adapting to a changing environment. This would be a future where communities govern collaboratively through integrated decision-making on policy, management and funding of natural and engineered water systems at the river basin scale.
This work uses large-eddy simulations to study the transition of a tulip flame stabilised by bubble vortex breakdown (BVB) mode towards a V flame stabilised by a conical vortex breakdown (CVB). The transition is triggered when the equivalence ratio is increased, resulting in a rise in temperature within the central recirculation zone (CRZ). Simultaneously, the pressure inside the CRZ bubble increases, while the average pressure inside the combustion chamber remains constant. This increase in pressure causes the CRZ bubble to open radially and expand, changing the vortex breakdown mode from BVB to CVB, and the flame shape from a tulip shape to a V shape. A criterion for a limit pressure inside the CRZ was then devised based on the radial momentum equation and the balance between centrifugal force and radial pressure gradient, found to control the radial motion of the CRZ. This criterion helped us to understand the main events of the transition, showing that, once the pressure inside the CRZ exceeds the limit given by the criterion, the flow topology changes from a BVB mode to a CVB mode. This transition highlights the differences between a BVB mode and a CVB mode, showing for the first time that there are characteristic pressure and velocity profiles for each mode in their swirling jets and CRZ. Finally, a significant achievement of this work is the identification of a novel mechanism for the controlled transition of vortex breakdown mode, a combustion-driven transition of vortex breakdown mode.