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Search for "stress" in Full Text gives 473 result(s) in Beilstein Journal of Nanotechnology. Showing first 200.

Effects of drug concentration and PLGA addition on the properties of electrospun ampicillin trihydrate-loaded PLA nanofibers

  • Tuğba Eren Böncü and
  • Nurten Ozdemir

Beilstein J. Nanotechnol. 2022, 13, 245–254, doi:10.3762/bjnano.13.19

Graphical Abstract
  • of the nanofibers were calculated from the strain–stress curves. Statistical analyses All data were expressed as mean ± SD. Statistical analyses were performed using SPSS 20.0 for Windows (SPSS, Chicago, IL). The significance was evaluated with one-way ANOVA followed by Tukey’s post hoc test (SPSS
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Published 21 Feb 2022

Relationship between corrosion and nanoscale friction on a metallic glass

  • Haoran Ma and
  • Roland Bennewitz

Beilstein J. Nanotechnol. 2022, 13, 236–244, doi:10.3762/bjnano.13.18

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  • copper surfaces, where it was suggested that more electrons escape in the vicinity of a peak than in a valley [27]. A surface undulation with parallel valleys on our ZrNiTi MG ribbons may be the reason for the distribution of pits along lines. Another possible reason is residual stress, indicated by the
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Published 18 Feb 2022

Piezoelectric nanogenerator for bio-mechanical strain measurement

  • Zafar Javed,
  • Lybah Rafiq,
  • Muhammad Anwaar Nazeer,
  • Saqib Siddiqui,
  • Muhammad Babar Ramzan,
  • Muhammad Qamar Khan and
  • Muhammad Salman Naeem

Beilstein J. Nanotechnol. 2022, 13, 192–200, doi:10.3762/bjnano.13.14

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  • diameter variation of nanofibers against different solution concentrations (D). X-ray diffraction pattern of nanofibers at various concentrations. Digital oscilloscope graph of the sensor under low dynamic strain (A), the output voltage under low dynamic stress (B), digital oscilloscope graph of the sensor
  • under high dynamic strain (C), the output voltage under high dynamic stress (D), digital oscilloscope graph of the sensor under low dynamic strain but with high frequency (E), and a piezoelectric sensor developed from 16 wt % solution (F). Integration of nanofibrous mesh into a knitted fabric for human
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Published 07 Feb 2022

Effect of lubricants on the rotational transmission between solid-state gears

  • Huang-Hsiang Lin,
  • Jonathan Heinze,
  • Alexander Croy,
  • Rafael Gutiérrez and
  • Gianaurelio Cuniberti

Beilstein J. Nanotechnol. 2022, 13, 54–62, doi:10.3762/bjnano.13.3

Graphical Abstract
  • fluid. One obtains several fluid properties such as pressure, velocity, shear stress, density and strain rate. In the case of the gear–oil–gear system, several studies based on the CFD simulation have been reported [11][12][13][14][15][16][17][18]. However, most of the simulations for this type of
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Published 05 Jan 2022

Sputtering onto liquids: a critical review

  • Anastasiya Sergievskaya,
  • Adrien Chauvin and
  • Stephanos Konstantinidis

Beilstein J. Nanotechnol. 2022, 13, 10–53, doi:10.3762/bjnano.13.2

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  • detailed information about the Finke–Watzky mechanism, the mathematical analysis of data, and links to useful references in [77][107][108][109]. It is important to stress that the autocatalytic model does not deny the possibility of the further growth of the metal NPs by secondary processes such as
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Published 04 Jan 2022

Alteration of nanomechanical properties of pancreatic cancer cells through anticancer drug treatment revealed by atomic force microscopy

  • Xiaoteng Liang,
  • Shuai Liu,
  • Xiuchao Wang,
  • Dan Xia and
  • Qiang Li

Beilstein J. Nanotechnol. 2021, 12, 1372–1379, doi:10.3762/bjnano.12.101

Graphical Abstract
  • /or the cytoskeleton, which cause cancer cell death [8][9]. Fang et al. found that N-methyl-ᴅ-aspartate (NMDA) binding to NMDA receptors on cell membranes will increase the overall contractile forces in the cytoskeleton, thus increasing the pre-existing mechanical stress [10]. Yun et al. reported that
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Published 14 Dec 2021

Biocompatibility and cytotoxicity in vitro of surface-functionalized drug-loaded spinel ferrite nanoparticles

  • Sadaf Mushtaq,
  • Khuram Shahzad,
  • Tariq Saeed,
  • Anwar Ul-Hamid,
  • Bilal Haider Abbasi,
  • Nafees Ahmad,
  • Waqas Khalid,
  • Muhammad Atif,
  • Zulqurnain Ali and
  • Rashda Abbasi

Beilstein J. Nanotechnol. 2021, 12, 1339–1364, doi:10.3762/bjnano.12.99

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  • . The nanoparticles caused cytotoxicity via oxidative stress, causing DNA damage and activation of p53-mediated cell cycle arrest (significantly elevated expression, p < 0.005, majorly G1 and G2/M arrest) and apoptosis. Cytotoxicity testing in 3D spheroids showed significant (p < 0.05) reduction in
  • or by leakage of the metal ions from the core surface, causing oxidative stress. This phenomenon can be controlled by coating the NPs with polymeric shells, which enhances their biocompatibility and stability [40]. All drug-loaded samples exhibited a dose-dependent response. Among DOX-loaded NPs, ZFO
  • biocompatibility of NPs-PMA at a given dose and treatment time. Cells undergo oxidative stress upon treatment with functionalized MFe2O4 NPs Generation of ROS has been associated with DNA damage, inflammation, apoptosis and senescence in cells [41]. The 2',7'-dichlorodihydrofluorescein diacetate (H2-DCFDA) assay
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Published 02 Dec 2021

Polarity in cuticular ridge development and insect attachment on leaf surfaces of Schismatoglottis calyptrata (Araceae)

  • Venkata A. Surapaneni,
  • Tobias Aust,
  • Thomas Speck and
  • Marc Thielen

Beilstein J. Nanotechnol. 2021, 12, 1326–1338, doi:10.3762/bjnano.12.98

Graphical Abstract
  • stress, temperature, and excess radiation and/or might represent a defense mechanism against, for example, insects or viruses [33][34][35]. When the leaves are rolled, the intensity of light reaching each underlying layer of the rolled-up leaf and the transpiration properties within each layer will be
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Published 01 Dec 2021

Enhancement of the piezoelectric coefficient in PVDF-TrFe/CoFe2O4 nanocomposites through DC magnetic poling

  • Marco Fortunato,
  • Alessio Tamburrano,
  • Maria Paola Bracciale,
  • Maria Laura Santarelli and
  • Maria Sabrina Sarto

Beilstein J. Nanotechnol. 2021, 12, 1262–1270, doi:10.3762/bjnano.12.93

Graphical Abstract
  • with zinc oxide nanostructures [1][3][5][6]. Recently, it was shown that the β phase content of PVDF can be improved introducing CoFe2O4 nanoparticles into the polymer and applying a DC magnetic field [25]. This effect has been ascribed to the strong tensile stress at the CoFe2O4/PVDF interfaces
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Published 19 Nov 2021

A review on slip boundary conditions at the nanoscale: recent development and applications

  • Ruifei Wang,
  • Jin Chai,
  • Bobo Luo,
  • Xiong Liu,
  • Jianting Zhang,
  • Min Wu,
  • Mingdan Wei and
  • Zhuanyue Ma

Beilstein J. Nanotechnol. 2021, 12, 1237–1251, doi:10.3762/bjnano.12.91

Graphical Abstract
  • zero (see Figure 1a). The relationship between slip length b and liquid slip velocity νs at the surface can be expressed as follows: where ν is liquid velocity and h is the channel height. When the liquid is at equilibrium, the viscous shear stress is exerted by the liquid on the wall, where η is the
  • shear viscosity of the liquid, equal to the friction stress suffered by the liquid from the wall, which is expressed as σ = λνs, where λ represents the interfacial friction coefficient [46]. Therefore, the slip length can be expressed as , which indicates that the slip length is reduced with the
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Published 17 Nov 2021

Impact of electron–phonon coupling on electron transport through T-shaped arrangements of quantum dots in the Kondo regime

  • Patryk Florków and
  • Stanisław Lipiński

Beilstein J. Nanotechnol. 2021, 12, 1209–1225, doi:10.3762/bjnano.12.89

Graphical Abstract
  • for ω = 0 for the main peaks (see inset) and for ω = nω0 for the satellites, exhibit Fano shape corresponding to a given qeff. For λO = 0.22, where qeff = 0, the line is symmetric. It is worth to stress that the widths of the dips in the main peak are the same as in the satellites, which proves that
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Published 12 Nov 2021

A new method for obtaining model-free viscoelastic material properties from atomic force microscopy experiments using discrete integral transform techniques

  • Berkin Uluutku,
  • Enrique A. López-Guerra and
  • Santiago D. Solares

Beilstein J. Nanotechnol. 2021, 12, 1063–1077, doi:10.3762/bjnano.12.79

Graphical Abstract
  • excitation of stress. Our proposed model-free approach follows the spirit of related Fourier-based methods, where viscoelastic material extraction has been achieved under some limited circumstances [29][30][31]. However, in this work, we exploit the advantages of the Z-transform, which we believe is more
  •  2), for which we carry out the force analysis in the complex domain (force spectroscopy). Theoretical Background It is well known that the behavior of viscoelastic materials is history-dependent, as a result of which, the stress–strain relationships governing their deformation are functionals (not
  • functions). More specifically, the stress at a given instant depends on the total previous history of strain and vice versa [13]. This history dependence is often expressed in the form of convolution integrals: where Q(t) and U(t) are known as relaxance and retardance, respectively. As already stated
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Published 23 Sep 2021

An overview of microneedle applications, materials, and fabrication methods

  • Zahra Faraji Rad,
  • Philip D. Prewett and
  • Graham J. Davies

Beilstein J. Nanotechnol. 2021, 12, 1034–1046, doi:10.3762/bjnano.12.77

Graphical Abstract
  • penetration are obviously dependent on microneedle tip dimensions and skin puncture stress. Consequently, there is increased interest in ultrasharp microneedles with tips having minimum lateral dimensions below 1 µm. The penetration force linearly increases with array size and the use of controlled force
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Published 13 Sep 2021

Progress and innovation of nanostructured sulfur cathodes and metal-free anodes for room-temperature Na–S batteries

  • Marina Tabuyo-Martínez,
  • Bernd Wicklein and
  • Pilar Aranda

Beilstein J. Nanotechnol. 2021, 12, 995–1020, doi:10.3762/bjnano.12.75

Graphical Abstract
  • the nanometer scale in form of nanoparticles, nanorods, nanofibers, nanoarrays, and nanosheets, which are more tolerant to dilative stress [75][76]. In addition, these nanostructures can be incorporated into a flexible carbon matrix for further accommodation of mechanical strain (Figure 10A) [74][77
  • . Nanostructured and nanoparticulated sulfur is easily entrapped in electroconducting matrices, which reduces the shuttle effect, increases the cathode conductivity, accommodates mechanical stress from volume expansion. Also, the high surface area accelerates reaction kinetics. A similar strategy can be pursued at
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Published 09 Sep 2021

Is the Ne operation of the helium ion microscope suitable for electron backscatter diffraction sample preparation?

  • Annalena Wolff

Beilstein J. Nanotechnol. 2021, 12, 965–983, doi:10.3762/bjnano.12.73

Graphical Abstract
  • electropolishing protocol induced some artefacts in this sample which could lead to misinterpretation for stress/strain analysis of the sample. The forward scatter diffraction (FSD) image (Figure 4e) shows void formation on the sample surface and significant sample surface alterations close to the area that was
  • electropolishing protocol not feasible for stress and strain analysis of the Cu sample. Argon ion polishing of the Cu sample produced better results than electropolishing. The FSD image (Figure 4j) reveals grains and does not show obvious sample surface alterations in comparison to the electropolishing approaches
  • challenging stress/strain analysis. Irradiation of copper at 0° incidence angle To assess the effect of ion irradiation, the copper TEM lamella grids were irradiated with Ga ions using a Ga FIB/SEM or Ne ions using HIM. An ion dose of 3371 ions/nm2 was chosen to allow a comparison with a previously reported
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Published 31 Aug 2021

Self-assembly of Eucalyptus gunnii wax tubules and pure ß-diketone on HOPG and glass

  • Miriam Anna Huth,
  • Axel Huth and
  • Kerstin Koch

Beilstein J. Nanotechnol. 2021, 12, 939–949, doi:10.3762/bjnano.12.70

Graphical Abstract
  • protect plants from environmental stress [4]. Waxes are, thereby, essential for a variety of functions, especially in the wettability and self-cleaning ability of plant surfaces [5][6]. Plant waxes consist of a complex mixture of aliphatic and aromatic compounds. The exact chemical composition of the wax
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Published 20 Aug 2021

Effects of temperature and repeat layer spacing on mechanical properties of graphene/polycrystalline copper nanolaminated composites under shear loading

  • Chia-Wei Huang,
  • Man-Ping Chang and
  • Te-Hua Fang

Beilstein J. Nanotechnol. 2021, 12, 863–877, doi:10.3762/bjnano.12.65

Graphical Abstract
  • as the temperature increases, the content of Shockley dislocations will increase and the maximum shear stress of the zigzag and armchair directions also decreases. The mechanical strength of the zigzag direction is more dependent on the temperature than that of the armchair direction. Moreover, self
  • -healing occurs in the armchair direction, which causes the shear stress to increase after failure. Furthermore, the maximum shear stress and the shear strength of the composites decrease with an increase of the repeat layer spacing. Also, the shear modulus increases by increasing the grain size of copper
  • the mechanical properties of carbon materials [31]. In this study, graphene with zigzag and armchair chirality is considered while simulating different properties of graphene monolayers and copper layers, including stress–strain curve variations, the distribution of von Mises stress, the evolution of
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Published 12 Aug 2021

Comprehensive review on ultrasound-responsive theranostic nanomaterials: mechanisms, structures and medical applications

  • Sepand Tehrani Fateh,
  • Lida Moradi,
  • Elmira Kohan,
  • Michael R. Hamblin and
  • Amin Shiralizadeh Dezfuli

Beilstein J. Nanotechnol. 2021, 12, 808–862, doi:10.3762/bjnano.12.64

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  • proximity to the cell membrane. It has been shown that during inertial cavitation, in addition to direct oscillating MB–cell membrane interactions, a fluid microjet formed around the MBs can be responsible for providing secondary mechanical stress on the cell membrane and create transient disruption. In
  • . reported that when the distance between the cell and the MB was increased to 5.5 µm, the exerted shear stress on the cell membrane suddenly decreased [78]. Schlicher et al. exposed prostate cancer cells (DU145) to 24 kHz US irradiation to investigate the cavitation events and the changes in the cell
  • further suggested that the same results would be obtained if a higher frequency US was employed [79]. Both mechanical stress and chemical effects induced by US could be responsible for the formation of repairable cell membrane pores [74]. Van Wamel et al. reported that the mechanism leading to enhanced
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Published 11 Aug 2021

Silver nanoparticles nucleated in NaOH-treated halloysite: a potential antimicrobial material

  • Yuri B. Matos,
  • Rodrigo S. Romanus,
  • Mattheus Torquato,
  • Edgar H. de Souza,
  • Rodrigo L. Villanova,
  • Marlene Soares and
  • Emilson R. Viana

Beilstein J. Nanotechnol. 2021, 12, 798–807, doi:10.3762/bjnano.12.63

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  • aluminosilicate sheet that folds over itself in virtue of the internal stress inherent to the crystalline structure of the material, forming nanotubes [25]. As shown in Figure 1, it folds with a silicate phase facing outwards (Si-O), and an aluminol phase facing inwards (Al-OH). Since the internal and external
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Published 05 Aug 2021

Electromigration-induced formation of percolating adsorbate islands during condensation from the gaseous phase: a computational study

  • Alina V. Dvornichenko,
  • Vasyl O. Kharchenko and
  • Dmitrii O. Kharchenko

Beilstein J. Nanotechnol. 2021, 12, 694–703, doi:10.3762/bjnano.12.55

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  • include the formation of surface steps [28][29][30][31], faceting of the surface [32][33][34][35][36][37], elimination of instability of surface morphology caused by stress and wetting of the substrate [38][39][40][41], the evolution of contact irregularities in switches of microelectromechanical systems
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Published 13 Jul 2021

A review of defect engineering, ion implantation, and nanofabrication using the helium ion microscope

  • Frances I. Allen

Beilstein J. Nanotechnol. 2021, 12, 633–664, doi:10.3762/bjnano.12.52

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  • Irradiation-induced restructuring The following applications have used localized helium ion irradiation in the HIM to change the morphology and/or internal structure of a material by ion-induced mass transport along surfaces, ion-induced collisional atomic mixing, and through stress gradients induced in
  • stress gradients across the membrane that lead to deformation by buckling [101]. Various intricate 3D structures have been created following this approach. Interestingly, right at the beginning of HIM-based research, membrane folding using localized helium ion irradiation was also demonstrated [99
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Published 02 Jul 2021

Stability and activity of platinum nanoparticles in the oxygen electroreduction reaction: is size or uniformity of primary importance?

  • Kirill O. Paperzh,
  • Anastasia A. Alekseenko,
  • Vadim A. Volochaev,
  • Ilya V. Pankov,
  • Olga A. Safronenko and
  • Vladimir E. Guterman

Beilstein J. Nanotechnol. 2021, 12, 593–606, doi:10.3762/bjnano.12.49

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  • obtained during accelerated stress tests and the use of fuel cells in real practice is far from being perfect. Therefore, along with the study of how certain factors influence on the catalyst stability, the search for optimal methods and conditions for stress tests in an electrochemical cell is still
  • increasing NP size [14][22][32][33][34][35][36]. The probability of agglomeration and coalescence of NPs during a stress test also decreases with an increase in the average distance between platinum NPs in catalysts, which results in an increase of their stability [14]. Apparently, a relatively high
  • series G40 < G35 < G30 < G25 < G20, the mass activity of the synthesized catalysts also increases (Table 2). Note that the mass activity of the sample G20 is almost 1.5 times higher than that of JM20, a commercial analog with a similar platinum content (Table 2). During the stress test of the catalysts
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Published 29 Jun 2021

The preparation temperature influences the physicochemical nature and activity of nanoceria

  • Robert A. Yokel,
  • Wendel Wohlleben,
  • Johannes Georg Keller,
  • Matthew L. Hancock,
  • Jason M. Unrine,
  • D. Allan Butterfield and
  • Eric A. Grulke

Beilstein J. Nanotechnol. 2021, 12, 525–540, doi:10.3762/bjnano.12.43

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  • have adverse consequences and raised the question whether its method of preparation and solubility are contributing factors. In contrast to the results with NM-212, other nanoceria have been demonstrated to have therapeutic potential for multiple conditions with an oxidative stress/inflammation
  • ). The initial experiment was repeated with as-prepared and 75, 102, and 152 day partially dissolved nanoceria. Nanoceria reactivity Oxidative stress, as mass-based biological oxidative damage (mBOD), and surface-based biological oxidative damage (sBOD), of NM-211, NM-212, and the solvothermally
  • more available oxygen on the surface of nanoceria not exposed to high temperature. Biological identity of as-prepared and partially dissolved nanoceria Nanoceria has the potential to act as a pro- or antioxidant, depending on its valence, and the oxidative stress level of the system under study
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Published 04 Jun 2021

A review on nanostructured silver as a basic ingredient in medicine: physicochemical parameters and characterization

  • Gabriel M. Misirli,
  • Kishore Sridharan and
  • Shirley M. P. Abrantes

Beilstein J. Nanotechnol. 2021, 12, 440–461, doi:10.3762/bjnano.12.36

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  • considered the ion content (Ag+) of those nanoparticles. Toxicity assays could be performed by using oxidative stress and other reliable markers, such as 8-oxoguanine DNA glycosylase 1 (OGG1) and nuclear factor erythroid 2-related factor 2 (Nrf2) [132] or 3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyltetrazolium
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Published 14 May 2021

Spontaneous shape transition of MnxGe1−x islands to long nanowires

  • S. Javad Rezvani,
  • Luc Favre,
  • Gabriele Giuli,
  • Yiming Wubulikasimu,
  • Isabelle Berbezier,
  • Augusto Marcelli,
  • Luca Boarino and
  • Nicola Pinto

Beilstein J. Nanotechnol. 2021, 12, 366–374, doi:10.3762/bjnano.12.30

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  • = α0, with: where e is the Neper number, ϕ = e−3/2cot(θ), with θ the contact angle of the island facet with the substrate. Γ = γecsc(θ) − γscot(θ) with γe and γs are the surface energy per unit area of the edge facet and the substrate, respectively. , where σb, ν and μ are the stress tensor in the
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Published 28 Apr 2021
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