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At high surface Péclet numbers, it is common to associate the presence of surfactants with surface immobilization, where a free surface becomes indistinguishable from a no-slip surface. A different mechanism has recently been proposed for longitudinal shear flow along a unidirectional trench (Baier & Hardt, J. Fluid Mech., vol. 949, 2022, A34) wherein, at high Marangoni numbers, the meniscus spanning the finite-length trench becomes a constant-shear-stress surface due to contamination by incompressible surfactant. That model predicts recirculating interfacial flows on the meniscus, a phenomenon that has been observed experimentally (Song et al., Phys. Rev. Fluids, vol. 3, issue 3, 2018, 033303). By finding an explicit solution to the constant-shear-stress model at all protrusion angles and calculating the effective slip length for a dilute mattress of such surfactant-laden trenches, we show that those effective slip lengths are almost indistinguishable from those for a surface whose menisci have the same deflection but have been completely immobilized (i.e. they are no-slip surfaces). This means that, despite the presence of non-trivial recirculating vortical flows on the menisci, the aggregate slip characteristics of such surfaces are that they have been effectively immobilized. This surprising result underscores the need for caution in comparing theory with experiments based on effective slip properties alone.
The present study investigates the profiles of statistically axisymmetric turbulent jets with arbitrary buoyancy. Analytical expressions for the shape of the radial velocity, Reynolds stress and radial scalar flux profiles are derived from the governing equations by assuming self-similar Gaussian mean velocity and scalar profiles. Previously these have only been derived for the special cases of pure jets and plumes, whereas the present study generalises them to arbitrary buoyancies. These are then used to derive analytical expressions for the turbulent Schmidt/Prandtl numbers, which, along with the mean profiles, are shown to give predictions in agreement with existing literature.
Drop impact onto a thin liquid film of another liquid is observed and characterized using a high-speed video system. A new mode of splash – a complete, simultaneous corona detachment – has been observed, which is the result of the lamella breakup near the wall film. The abrupt outward and upward displacement of the lamella leads to an extreme stretching of the corona wall, resulting in its rapid thinning and a rupture. This rupture triggers propagating Taylor–Culick rims, which rapidly spread, meet and, thus, undercut simultaneously the entire corona, resulting in its detachment. Special experiments with the spreading corona impingement onto a fixed needle, supplement the physical evidence of the above-mentioned mechanism. A self-consistent theory of the observed phenomena is proposed and compared with experiments, exhibiting good agreement.
We present the analytical solution for the two-dimensional velocity and density fields within an approximation for laminar stratified inclined duct (SID) flows where diffusion dominates over inertia in the along-channel momentum equation but is negligible in the density transport equation. We refer to this approximation as the hydrostatic/gravitational/viscous in momentum and advective in density (HGV-A) approximation due to the leading balances in the governing equations. The analytical solution is valid for laminar flows in a two-layer configuration in the limit of long ducts. The non-dimensional volume flux within the HGV-A approximation is given by $Fr^* ={{Re}}_g/(AK)$, which is a control parameter with ${{Re}}_g$ the gravitational Reynolds number, $A$ the aspect ratio of the duct and $K$ a geometrical parameter that depends on the tilt of the duct and is obtained from the analytical solution. This analytical solution was validated against results from laboratory experiments, and allows us to gain new insight into the dynamics and properties of SID flows. Most importantly, constant values of $Fr^*$ describe, in both horizontal and inclined ducts, the transitions between increasingly turbulent flow regimes: from laminar flow, to interfacial waves, to intermittent turbulence and sustained turbulence.
Functional magnetic resonance imaging (fMRI) was conceived in the early 1990s due to the coincidence of two advances: (1) MRI scanner technology able to support fast echo-planar imaging imaging techniques with the required temporal stability and (2) the scientific knowledge that differences in the magnetic susceptibility of blood may be associated with MRI signal changes based on alterations in blood oxygenation levels. These elements, together with the assumption that changes in blood oxygenation and volume would accompany changes in neural activity in the brain, motivated research groups around the world to develop fMRI.
In the mid-1980s a number of scientists and research bodies conceived the idea of determining the DNA sequence of the entire human genome. Initiated in 1990 and known as the Human Genome Project (HGP), this ambitious, publicly funded project relied on contributions from numerous international laboratories and remains the world’s largest collaborative biological-based project to date. The completion of the HGP thirteen years later in 2003 allowed scientists to view the human genome in its entirety for the first time [1]. It was thought that this would usher in a new age for biological research, allowing for a more comprehensive understanding of complex human diseases and phenotypes. While this was true to an extent, completion of this project led to a series of new, more complicated questions, as is often the case in research.
Epilepsy affects approximately 1% of the population [1]. Although generally treatable, up to 30% of patients do not achieve seizure freedom from anticonvulsive medication alone. Due to its relationship with cognitive abilities [2], quality of life [3], and the associated risk of premature death [4], drug-refractory epilepsy should be treated promptly. Temporal lobe epilepsy (TLE) associated with mesiotemporal sclerosis [5] and extra-temporal lobe epilepsy related to focal cortical dysplasia (FCD) [6] constitute the most common refractory epilepsy syndromes. Surgical resection of these lesions remains the treatment of choice [7], with success rates approaching 80% [8]. By allowing the detection of epileptogenic lesions and offering system-level mechanisms of the disease process, MRI has shifted the field from electro-clinical correlations toward a multidisciplinary approach.
Complex systems theory is a nebulous field whose overarching goal is to understand the dynamical behavior of systems consisting of many interconnected component parts. It has attracted widespread interest from many domains that study examples of such systems, including ecologists, sociologists, engineers, artificial intelligence researchers, condensed matter physicists, neuroscientists, and many others. The results of these collected, multi-disciplinary efforts have not been so much a comprehensive theory of Complex Systems (capital-C, capital-S), but rather a set of techniques, analogies, and attitudes toward problem solving that emphasize interactions and dynamics over individual components and their functions. The chapters are written in a complex adaptive systems frame and therefore it is useful to provide a provisional theoretical description of such systems. Following Holland [1], a generalizable description of complex adaptive systems is that they are collections of relatively simple agents that have the property that they can aggregate, so that collections of agents can form meta-agents (and meta-meta-agents etc.) with higher-order structure. These aggregates interact nonlinearly, so that the aggregate behavior of a collection of agents is qualitatively different from the behavior of the individual agents. The interactions among agents mediate flows of materials or information. Finally, the agents are typically diverse with distinct specialties that are optimized through adaptation to selective pressures in their environments.
The genetic underpinnings of epilepsy have come into much clearer focus over the past two decades. Advances in high-throughput molecular techniques have markedly improved our ability to identify potential therapeutic targets in epilepsy. Many of the monogenic effects identified through these methods have resulted in effective therapeutic targets for seizure amelioration [1,2,3]. Currently, around 200 definitively annotated epilepsy genes causing a range of seizure disorders and phenotypes have been identified [4]. Many more genes with putative associations with epilepsy pathways require further study [5]. The expansion of known genetic mechanisms and risk factors presents us with several benefits, including an increased pool of possible drug targets [6], genetic subtyping of seizure disorders [7], and the possibility for integrative analysis across different disorders [8,9]. However, the increasingly rich collection of genetic associations has also revealed the complexity of seizure disorders. Many mutations in different genes can converge on a similar clinical presentation [10], while different mutations in the same gene can have radically divergent outcomes [11,12]. Moreover, while robust data from twin and family studies demonstrate that common epilepsies are highly heritable [13,14], association studies have only detected risk factors that account for a small fraction of risk [15]. Thus, the data on epilepsy suggests a dichotomy. On one side, genetics is critical for describing etiology [16]. On the other side, using this information for prognosis or therapeutic development is limited by our current understanding of the complex genetic underpinnings of the disease and our analytic tools [10,17]. As a response to this complexity, researchers have started to shift toward complex systems approaches to genetics, which changes the focus from individual mutations to interactions among many mutations. The purpose of this chapter is to elaborate this ethos and present examples of this approach.
Many will trace the earliest articulation of what we may today call the science of complexity to Weaver’s [1] classic essay. In this work, Weaver distinguished between (i) the science of “simplicity” with phenomena that could be understood when reduced to a few variables, such as classical mechanics in two dimensions, (ii) the science of “disorganized complexity” concerning systems with large numbers of variables analyzed by a process of averaging, such as statistical thermodynamics, and (iii) an emerging field of “organized complex” systems, also with large numbers of variables, that was not amenable to either approach. This third middle region, Weaver wrote, would form the next significant challenge for science, needing both the power of machines (computers) and large interdisciplinary scientific teams for progress. Today, the field of complex systems, though lacking a universally accepted definition, studies entities – physical, biological, or social – united by the presence of large numbers of nonlinearly interacting agents that yield collective behavior not directly predictable from the laws governing interactions of the individual agents [2]. The thesis of complexity is therefore in direct opposition to the philosophy of reductionism and the source of an important debate regarding the foundations of science itself [3]. Examples of collective behavior in complex systems include, for instance, the “emergent” phenomena of macroscopic patterns [4] and phase transitions [5]. These coherent structures occur at scales far removed from those governing the interaction of the individual entities of the system and are due to bifurcation and symmetry breaking [6] involving macroscopic “collective” variables. On the other hand, the large size and nonlinearity of complex systems endow them with a measure of unpredictability – arising from deterministic chaos as well as inherent “fluctuations” – that naturally invokes a probabilistic description. Complex systems are thus said to have an “open” future that generates information and “surprise” as they evolve [7].
Epilepsy is the most common of the chronic and severe neurological diseases. It affects 65 million people worldwide and is characterized by an augmented susceptibility to seizures. Seizures are “transient occurrence of signs and/or symptoms due to abnormal excessive or synchronous neuronal activity in the brain” [1]. Current therapeutic strategies have the goal of suppressing or reducing the occurrence of seizures, thus being symptomatic rather than curative. There are no known therapies able to modify the evolution of acquired epilepsy, or to prevent its development. Furthermore, 25–40% of patients do not respond to pharmacological treatment, and this number stays unchanged when using new generation antiepileptic drugs as compared to established ones. For drug-resistant patients with focal epilepsy (an epilepsy in which seizures start in one hemisphere) there exists an alternative to medication: surgical resection of the brain regions involved in the generation of seizures, the epileptogenic zone, under the constraints of limiting post-surgical neurological impairments. Rates of success of brain surgery for epilepsy treatment vary between 34% and 74% as a function of the type of epilepsy. Outcomes are very variable, depend on the patient condition, and can change in time.
In this paper, the acoustic resonance mechanism for different axisymmetric screech modes of the underexpanded jets that impinge on an inclined plate is investigated experimentally. The ideally expanded Mach number of jets ($M_j$) ranges from 1.05 to 1.56. The nozzle-to-plate distance at the jet axis and the impingement angle are respectively set as 5.0$D$ and $30^{\circ }$, where $D$ is the nozzle exit diameter. The acoustic results show that the $M_j$ range for the A2 screech mode of impinging jets is broader than that of underexpanded free jets, and a new axisymmetric screech mode A3 appears. With the increase of $M_j$, the effect of the impinging plate on the shock cell structures of jets becomes obvious gradually, and the second suboptimal peaks are evident in the axial wavenumber spectra of mean shock structures. The coherent flow structures at screech frequencies are extracted from time-resolved schlieren images via the spectral proper orthogonal decomposition (SPOD). The axial wavenumber spectra of the selected SPOD modes suggest that the A1, A2 and A3 screech modes are respectively closed by the guided jet modes that are energized by the interactions between the Kelvin–Helmholtz wavepacket and the first three shock wavenumber peaks. The upstream- and downstream-propagating waves that constitute the screech feedback loop are analysed by applying wavenumber filters to the wavenumber spectra of SPOD modes. The frequencies of these three screech modes can be predicted by the phase constraints between the nozzle exit and the rear edge of the third shock cell. For the A3 mode, the inclined plate invades the third shock cell with the increase of $M_j$, and the phase constraint cannot be satisfied at the lower side of the jets, which leads the A3 mode to fade away. The present results suggest that external boundaries can modulate the frequency and mode of jet screech by changing the axial spacings of shock cells.
The previous chapters have dealt with the complex adaptive nature of the genome. Similar concepts in terms of interacting elements, self-organization and adaptation can be applied at other hierarchical scales. In this chapter we will show how complex adaptive systems (CAS) concepts can be usefully applied at the level of action potential firing patterns of single neurons in terms of seizure generation and of associated morbidities.
Epilepsy is a family of neurological disorders in which patients experience unprovoked spontaneous seizures. Unfortunately, there is currently no cure for epilepsy, and seizure management is the target of most therapies. The first-line treatment of epilepsy is usually antiepileptic drugs. However, depending on the subtype of epilepsy and the individual, drug treatments fail to control the seizures in around one-third of patients. One challenge in the treatment of epilepsy is its heterogeneity. In each patient, seizures are thought to be generated by different mechanisms, processes, and parameters, and treatment outcomes will also depend on these.