Alterations to Titanium Surface Depending on the Fluorides and Abrasives in Toothpaste

Fluoride and abrasives in toothpastes may cause corrosion and deterioration of the titanium used for implants and other prostheses. The purpose of this study was to investigate how the presence or absence and types of fluoride and abrasives affected the titanium surface texture. Brushing with toothpastes was performed on pure-titanium discs using an abrasive testing machine. Unprocessed titanium discs without brushing were used as control samples. Surface roughness, color, and gloss of titanium were measured and the differences compared with the control were analyzed. Additionally, titanium surfaces and abrasives in toothpastes were observed using a scanning electron microscope to compare the surface texture of each sample. Some toothpastes (abrasive+) significantly increased the difference in surface roughness, color, and gloss, compared with ultrapure water. Toothpaste (fluoride+/abrasive+) that had many polygonal abrasive particles led to the largest color differences and exhibited notable scratches and a larger number of contaminant- or corrosion-like black spots. In contrast, brushing with toothpaste without fluoride or abrasives (fluoride−/abrasive−) caused little change to the titanium surface. These results suggest that both fluoride and abrasives in toothpaste used for brushing may be factors that affect surface texture and corrosion resistance of titanium.     

Prolonged total extracorporeal lung assistance without systemic heparinization

A 16-year-old female developed severe ARDS in her single remaining lung following pneumonectomy for blunt trauma. Total extracorporeal lung assist (ECLA) for 40 days using a covalently heparin-coated circuit proved lifesaving. Systemic heparinization was not applied, as the heparinized surface by itself prevented clotting of the extracorporeal circuit. Systemic primary fibrinolysis developed but was not associated with major bleeding. A veno-right ventricular cannulation technique was used and maximum venous drainage for the extracorporeal circulation was achieved by elevating the bed 50 cm from the floor. This allowed extracorporeal blood flow (ECBF) approaching cardiac output (CO) and complete extracorporeal replacement of lung function. After 40 days, lung recovery allowed discontinuation of ECLA. Five days later the patient suffered serious lung collapse and was operated for a bronchopleural fistula. The patient was extubated 4 weeks after terminating ECLA and discharged in good condition 5 weeks later.     

Direct measurement of the viscoelectric effect in water

The viscoelectric effect concerns the increase in viscosity of a polar liquid in an electric field due to its interaction with the dipolar molecules and was first determined for polar organic liquids more than 80 y ago. For the case of water, however, the most common polar liquid, direct measurement of the viscoelectric effect is challenging and has not to date been carried out, despite its importance in a wide range of electrokinetic and flow effects. In consequence, estimates of its magnitude for water vary by more than three orders of magnitude. Here, we measure the viscoelectric effect in water directly using a surface force balance by measuring the dynamic approach of two molecularly smooth surfaces with a controlled, uniform electric field between them across highly purified water. As the water is squeezed out of the gap between the approaching surfaces, viscous damping dominates the approach dynamics; this is modulated by the viscoelectric effect under the uniform transverse electric field across the water, enabling its magnitude to be directly determined as a function of the field. We measured a value for this magnitude, which differs by one and by two orders of magnitude, respectively, from its highest and lowest previously estimated values.

The viscoelectric effect concerns the change in the viscosity of polar liquids in the presence of an electric field (1–3). It arises from the interaction of the field with the dipolar molecules, and while its molecular origins are still not well understood (4–6), it has considerable relevance in areas ranging from surface potential measurements (7–9) and boundary lubrication (10) to nanofluidics and its applications (11–13). Knowing the magnitude of the viscoelectric effect is thus of clear importance. It was first measured by Andrade and Dodd (1–3) for a range of polar organic liquids, by monitoring their flow in a narrow channel between metal electrodes across which a known electric field E was applied, and quantified via a viscoelectric coefficient f using an empirical relation based on their results:η(E)= η0(1 + f∣E∣2),[1]a simplified analysis leading to such a relation is given in Ref. (8). Here, η₀ is the unperturbed bulk liquid viscosity (i.e., in the absence of any field). For the case of water, however, the most ubiquitous and important polar liquid, measurement of its viscosity in the presence of a strong, uniform field presents a strong challenge (as discussed later in this section), and to our knowledge no such direct measurements have been reported. Over the past six decades, therefore, the magnitude of the viscoelectric effect in water has been only indirectly estimated by extrapolation from its values for organic liquids (8), from estimates of its effect on electrokinetic phenomena (11, 14–19), or by other approaches (7, 12, 20, 21). These estimated values, as expressed in the viscoelectric coefficient f, vary over more than three orders of magnitude, ranging from f ∼10⁻¹⁷–2.5 × 10⁻¹⁴ (V/m)² (SI Appendix, Section 7). For completeness, we note that results contradictory to the viscoelectric model have also been reported (22) (i.e., suggesting a decreased water viscosity in an electric field). The reasons for the large span of these estimated f values were attributed to various factors such as solid/liquid coupling, varying ionic sizes, and varying water permittivity (12, 19); however, while these factors may play some role, there is no evidence that they could lead to such large discrepancies.We believe, rather, that the origin of the large variance in the estimated magnitude of the viscoelectric effect arises because none of the experimental studies on water to date in which the f values were estimated was direct, in the sense of probing how the water viscosity varied with field in a uniform electric field. In all cases, viscosity changes were assumed to occur only in the nonuniform, rapidly decaying electrostatic potential near charged surfaces immersed in water. Changes in electrophoretic mobility, electro-osmosis, or hydrodynamic dissipation or water mobility between similarly charged solid surfaces were then attributed to some mean viscosity increase in these thin surface-adjacent layers (7, 11, 12, 14–21). In practice, however, the effect on these electrokinetic phenomena of viscosity or water mobility changes in the thin layers where such nonuniform, rapidly decaying fields are present is not easy to quantify reliably, especially in the presence of salt ions (12). At the same time, measuring the viscosity of water in a uniform electric field between two surfaces at different potentials, as was done for the polar organic solvents (2, 3) and which would provide a direct determination of its viscoelectric effect, presents a considerable difficulty. This is due to two main factors and arises because, in contrast to organic solvents, water may self-dissociate. Firstly, the potential difference that may be applied between the surfaces across water is limited, if electrolysis is to be avoided (23, 24), and secondly, electrostatic screening implies that the field decays strongly (within a Debye screening length) away from the surfaces (25–27). Even in purified water with no added salt (as in the present study), the potential decays rapidly away from a charged surface (see, e.g., Fig. 1C), so that to measure viscosity in a uniform field between two surfaces, one would require flow channels of width of order some tens of nanometers or less, presenting a major challenge.Open in a separate windowFig. 1.Numerical solution to the nonlinearized PB equation with σ_mica = −8.1 mC/m², ψ_gold = 0.07 V, and ion concentration c_b = 8 × 10⁻⁵ M, corresponding to the conditions of Fig. 4A. (A) Surface potential on the mica surface and surface charge on the gold surface as a function of separation D. (B) Average electric field approximated as (|ψ_gold − ψ_mica|/D). (C) Local potential ψ as a function of distance d from the mica surface for different separations D. Dashed line in larger-scale inset is an eye guide of a linear approximation.In the present study, we overcome this by directly probing the viscosity of purified water across which a uniform electric field acts while it is confined between two surfaces in a surface force balance (SFB). In our experiments, a molecularly smooth gold surface at a controlled (positive) surface potential approaches an atomically smooth mica surface at constant surface (negative) charge density, so that a known electric field acts across the water-filled gap of width D between them; moreover, this field is very close to uniform at the most relevant surface separations (D ≲ 30 nm, Fig. 1C). The dynamics of approach is strongly modulated by the viscous damping due to squeeze-out of the water as D decreases, and hence by its viscosity in the uniform electric field; by monitoring the approach rate of the surfaces at high temporal (millisecond) and spatial (approximately angstrom) resolutions, we are able therefore to directly evaluate the magnitude of the viscoelectric effect (the value of f).     

指按法动力学参数的量化测定与比较分析

目的:通过对不同组别人群指按法动力学参数的量化测定与比较分析,观察其操作是否具有一致性,为指按法的量化与规范化、临床教学提供一定的依据.方法:应用MFF多点薄膜压力测试系统,检测并记录3组不同推拿年限的操作者进行手法操作过程中的动态图形,并保存分析相应的参数数据.结果:3组指按法的平均作用力为本科生组轻度(5.99±2...     

What we learn about bipolar disorder from large‐scale neuroimaging: Findings and future directions from the ENIGMA Bipolar Disorder Working Group

MRI‐derived brain measures offer a link between genes, the environment and behavior and have been widely studied in bipolar disorder (BD). However, many neuroimaging studies of BD have been underpowered, leading to varied results and uncertainty regarding effects. The Enhancing Neuro Imaging Genetics through Meta‐Analysis (ENIGMA) Bipolar Disorder Working Group was formed in 2012 to empower discoveries, generate consensus findings and inform future hypothesis‐driven studies of BD. Through this effort, over 150 researchers from 20 countries and 55 institutions pool data and resources to produce the largest neuroimaging studies of BD ever conducted. The ENIGMA Bipolar Disorder Working Group applies standardized processing and analysis techniques to empower large‐scale meta‐ and mega‐analyses of multimodal brain MRI and improve the replicability of studies relating brain variation to clinical and genetic data. Initial BD Working Group studies reveal widespread patterns of lower cortical thickness, subcortical volume and disrupted white matter integrity associated with BD. Findings also include mapping brain alterations of common medications like lithium, symptom patterns and clinical risk profiles and have provided further insights into the pathophysiological mechanisms of BD. Here we discuss key findings from the BD working group, its ongoing projects and future directions for large‐scale, collaborative studies of mental illness.     

口腔诊疗操作中高频接触表面的量性研究

目的 明确口腔诊疗操作中高频接触表面,为清洁消毒工作提供依据与指导。方法 采用直接观察法对北京市某三级甲等口腔医院7个门诊科室环境表面的接触时间与频次进行调查,计算平均接触频次、95%置信区间及累积接触频率。结果 口腔诊疗操作中环境表面平均接触26.75次/操作,平均接触频次最高为牙体牙髓病专业(46.25次/操作),最低为口腔黏膜病专业(10.19次/操作)。高频接触表面为无影灯手柄、综合治疗台操作面板及手柄(医生侧)、电脑键盘及鼠标、三用枪手柄及线前端、高速牙科手机及线前端,接触频次分别为3.99、3.85、2.65、1.86、1.40次/操作。所有口腔专业的高频接触表面均包含综合治疗台操作面板及手柄(医生侧),75%的专业包含电脑键盘及鼠标,50%的专业接触频次最高为无影灯手柄;环境表面平均接触频次最高为牙冠预备操作(113.50次/操作),最低为正畸咨询(8.50次/操作)。结论 不同口腔专业及不同口腔诊疗操作的高频接触表面不同,医疗机构应根据口腔科室高频接触表面的实际情况采取相应的清洁消毒及管理措施,切实提升环境清洁消毒质量。     

柴胡不同复种模式的比较研究

柴胡是山西省的道地药材,种植柴胡是当地农民增收的主要来源之一.在柴胡种植中,小麦-柴胡、玉米-柴胡和大豆-柴胡复种是常用的复种模式.本文研究了3种不同复种方式对土壤氮磷钾含量、柴胡光合参数、柴胡地上部和地下部农艺性状、柴胡皂甙A、C、D含量、柴胡产量和经济效益的影响.结果表明,在大豆-柴胡复种模式下,有利于土壤中氮素的...     

Surface NMR using quantum sensors in diamond

NMR is a noninvasive, molecular-level spectroscopic technique widely used for chemical characterization. However, it lacks the sensitivity to probe the small number of spins at surfaces and interfaces. Here, we use nitrogen vacancy (NV) centers in diamond as quantum sensors to optically detect NMR signals from chemically modified thin films. To demonstrate the method’s capabilities, aluminum oxide layers, common supports in catalysis and materials science, are prepared by atomic layer deposition and are subsequently functionalized by phosphonate chemistry to form self-assembled monolayers. The surface NV-NMR technique detects spatially resolved NMR signals from the monolayer, indicates chemical binding, and quantifies molecular coverage. In addition, it can monitor in real time the formation kinetics at the solid–liquid interface. With our approach, we show that NV quantum sensors are a surface-sensitive NMR tool with femtomole sensitivity for in situ analysis in catalysis, materials, and biological research.

The characterization of surface processes at the molecular level is essential for understanding fundamental processes in industrial catalysis, energy conversion, electronic circuits, targeted drug delivery, and biosensing (1). However, many analytical techniques used in surface science are inaccessible under ambient or chemically relevant conditions. Therefore, it remains challenging to perform chemical analysis under the conditions in which these processes occur (2, 3). Commonly used surface sensitive methods, such as X-ray photoelectron spectroscopy (XPS), Auger electron spectroscopy, and secondary ion mass spectroscopy can perform chemical analysis but require ultra-high vacuum and expensive equipment (4). Great efforts have been devoted to extending XPS analysis to near ambient conditions (2). Indeed, both near-ambient pressure XPS and extended X-ray absorption fine structure have significantly expanded the applicability of these X-ray–based techniques for understanding reaction mechanisms at chemically active interfaces (2, 5). However, both methods require intense synchrotron radiation to achieve high sensitivity and resolution, which limits their practical accessibility and increases their cost. State-of-the-art surface-sensitive spectroscopy techniques, such as sum frequency generation and second harmonic generation, can perform analysis under ambient conditions but require technically complex equipment such as femtosecond lasers (6). Even with all these techniques available, molecular dynamics or chemical reaction kinetics at surfaces are still challenging to probe experimentally (7) (SI Appendix, Supplementary Note 1).NMR spectroscopy is one of the major tools for chemical and structural analysis in chemistry, biology, and materials science. Solid-state NMR in particular (8) has advanced understanding of a range of systems, including metal organic frameworks (9), batteries (10), and catalysts (11). However, sensitivity remains a challenge for traditional NMR spectroscopy, making studies at surfaces difficult because of the limited numbers of nuclear spins. Recently, surface-enhanced NMR spectroscopy (DNP-SENS) relying on hyperpolarization such as dynamic nuclear polarization (12, 13) or xenon-based techniques (14) gained research momentum and enabled probing spins located at surfaces. However, even in highly porous materials with greater than 1,000 m²/g surface area, the concentration of NMR-active nuclei of interest often remains low (e.g., 1 mmol of surface atoms/g), which requires long averaging times to obtain solid-state NMR spectra with reasonable signal-to-noise ratios (SNR) (12) (SI Appendix, Supplementary Note 2).Here, we demonstrate the use of quantum sensors in diamond as a surface-sensitive spectroscopy technique that works at ambient conditions and can probe planar interfaces on the microscopic length scale with far greater sensitivity (femtomoles, see Materials and Methods) than conventional NMR. The spectroscopic technique relies on the nitrogen vacancy (NV) point defect, consisting of a nitrogen impurity (N) and an adjacent vacancy (V) in the carbon lattice of diamond. These spin-1 defects allow for optical detection of magnetic resonance and have been established as highly sensitive nanoscale magnetic field sensors (15, 16). Near-surface NV centers are sensitive to magnetic fields from the Larmor precession of nuclei from samples positioned outside of the diamond. This enables nanoscale NMR detection—even down to a single molecule (17) or spin (18, 19). The measurement volume of such NV sensors (20, 21) corresponds to a hemisphere whose radius is roughly their depth below the surface in the diamond lattice (e.g., 5 to 10 nm). At this small length scale, the thermal polarization of the nuclear spins can be neglected since spin noise dominates for a small number of spins (22, 23). For that reason, the NMR signal strength is independent of the applied magnetic field B₀, reducing experimental complexity and costs, which makes the technique accessible to a broader community. Previously published nanoscale NV-NMR experiments detected NMR signals from either bulk samples [such as viscous oils (21, 22, 24)] or samples tethered to (17) or placed directly on the diamond surface (25). In this work, we propose the use of NV centers in diamond combined with state-of-the-art thin film deposition techniques as a general platform to detect NMR signals with high sensitivity and spatial resolution even from nondiamond surfaces. This approach is general and allows for the probing of a variety of surfaces and interfaces with NMR, thereby enabling their chemistry to be explored. Here, we use atomic layer deposition (ALD), a technology that can be applied to synthesize films of a wide variety of materials with high thickness precision to coat the diamond with amorphous aluminum oxide (Al₂O₃). Al₂O₃ provides an exemplary surface of high technical relevance in optoelectronic applications and acts as structural support in various catalytic processes (26). In a proof-of-concept study for this surface-sensitive spectroscopic technique, we probe the chemical modification of the Al₂O₃ surface with phosphonate anchoring during the formation of a self-assembling monolayer (SAM) (27).     

Bioconjugation Strategy for Ceramic Membranes Decorated with Candida Antarctica Lipase B—Impact of Immobilization Process on Material Features

A strategy for the bioconjugation of the enzyme Candida antarctica lipase B onto titania ceramic membranes with varied pore sizes (15, 50, 150, and 300 kDa) was successfully performed. The relationship between the membrane morphology, i.e.,the pore size of the ceramic support, and bioconjugation performance was considered. Owing to the dimension of the enzyme (~33 kDa), the morphology of the ceramics allowed (50, 150, and 300 kDa) or did not allow (15 kDa) the entrance of the enzyme molecules into the porous structure. Such a strategy made it possible to better understand the changes in the material (morphology) and physicochemical features (wettability, adhesiveness, and surface charge) of the samples, which were systematically examined. The silane functionalization and enzyme immobilization were accomplished via the covalent route. The samples were characterized after each stage of the modification, which was very informative from the material point of view. As a consequence of the modification, significant changes in the contact angle, roughness, adhesion, and zeta potential were observed. For instance, for the 50 kDa membrane, the contact angle increased from 29.1 ± 1.5° for the pristine sample to 72.3 ± 1.5° after silane attachment; subsequently, it was reduced to 57.2 ± 1.5° after the enzyme immobilization. Finally, the contact angle of the bioconjugated membrane used in the enzymatic process rose to 92.9 ± 1.5°. By roughness (S_q) controlling, the following amendments were noticed: for the pristine 50 kDa membrane, S_q = 1.87 ± 0.21 µm; after silanization, S_q = 2.33 ± 0.30 µm; after enzyme immobilization, S_q = 2.74 ± 0.26 µm; and eventually, after the enzymatic process, S_q = 2.37 ± 0.27 µm. The adhesion work of the 50 kDa samples was equal to 136.41 ± 2.20 mN m⁻¹ (pristine membrane), 94.93 ± 2.00 mN m⁻¹ (with silane), 112.24 ± 1.90 mN m⁻¹ (with silane and enzyme), and finally, 69.12 ± 1.40 mN m⁻¹ (after the enzymatic process). The materials and physicochemical features changed substantially, particularly after the application of the membrane in the enzymatic process. Moreover, the impact of ceramic material morphology on the zeta potential value is here presented for the first time. With an increase in the ceramic support cut-off, the amount of immobilized lipase rose, but the specific productivity was higher for membranes possessing smaller pores, owing to the higher grafting density. For the enzymatic process, two modes of accomplishment were selected, i.e., stirred-tank and cross-flow. The latter method was characterized by a much higher effectiveness, with a resulting productivity equal to 99.7 and 60.3 µmol h⁻¹ for the 300 and 15 kD membranes, respectively.     

淋球菌外膜蛋白NspA基因重组子的构建与表达

目的构建淋球菌标准株外膜蛋白NspA基因重组子,在大肠杆菌BL21（DE3）中诱导表达外膜蛋白NspA。方法提取淋球菌标准株基因组DNA,PCR扩增其NspA基因,插入表达质粒载体pET-30c（＋）中,构建pET-NspA重组子,转化表达宿主大肠杆菌BL21（DE3）,异丙基-β-D-硫代半乳糖苷（IPTG）诱导重组蛋白表达,SDS-PAGE和Western Blot检测表达蛋白。结果成功构建了淋球菌标准株的pET-NspA大肠杆菌表达重组子,经IPTG诱导表达后,该蛋白在大肠杆菌中高效表达。结论淋球菌外膜蛋白NspA在大肠杆菌中的成功表达,为研究该蛋白的免疫学性能、制备抗体和研制预防淋病的疫苗奠定了基础。