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18 protocols using vk x250

1

Surface Roughness Analysis of Fabricated Specimens

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3D laser confocal microscope Keyence VK-X250 was used to measure the surface roughness of as-fabricated specimens. The imaging process takes surface height measurements using the point illumination method, where a laser beam is scanned across the sample in a raster pattern at incremental vertical displacements. The vertical resolution is dependent on the aperture of the objective lens. The measured height data was then analyzed using Keyence Multi-file Analyzer software. Image processing procedures were applied to account for the curved surface of the cylindrical samples, and surface roughness parameters are calculated. The surface roughness measurements were performed using an objective lens of 20 × magnification with a z-pitch of 0.20 µm. Approximately 4.7 mm × 1.4 mm of surface area was scanned within the central gage section of each specimen. The nominal scan step size was set to 1.4 µm which corresponds to 3345 × 1024 pixels within the surface map. Efforts were made to scan approximately similar regions across each specimen using print marks on specimens, as shown in Fig. 2. Each specimen was aligned under the confocal microscope using print marks as guidance prior to scanning the central gage section.
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2

Microscopic Characterization of 3D-MNSs

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An optical microscope (Olympus K-100, Olympus Co., Japan) was employed to observe the status of the template and the fabricated workpiece. A confocal laser microscopy setup (VK-X250, Keyence Co.) was employed to characterize the morphology and the profile of the imprinted 3D-MNSs in the semiconductors.
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3

Roughness Characterization of Ceramic Femoral Heads

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The roughness measurements were performed for all femoral heads shown in Figure 1 after five million cycles in the hip wear simulator. The maximum height (Rz) and arithmetic average roughness (Ra) were determined optically with a laser scanning microscope (LSM, VK-X250, Keyence Germany GmbH, Neu-Isenburg, Germany), according to DIN EN ISO 3274: 1998 [24 ] and DIN ES ISO 4288: 1998 [25 ]. For comparison, the roughness of each ceramic head was examined at three different locations on the unaltered surface without visible metallic deposition and at three areas with metallic depositions on the same retrieved head. Four roughness measurements were obtained for each location and the roughness values of the unaltered and altered surface were compared.
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4

Characterizing 3D-Printed Flow Channels

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Surface measurements on 3D-printed flow master molds were performed using a confocal laser scanning microscope (VK-X250; Keyence, Japan). Confocal images were then analyzed using MATLAB (R2019a; MathWorks, MA, USA) to obtain the flow channel profiles.
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5

Characterization of Liquid Crystalline Polymer Films

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Liquid crystalline phase transition temperature was measured with DSC curves using a differential scanning calorimeter (DSC 2500, TA Instruments) with a temperature ramp rate of 10 °C min−1. Cholesteric textures of LC samples were characterized with Zeiss AXIO polarized optical microscope. Reflection spectra were measured with PerkinElmer Lambda 1050+ photospectrometer and Thorlabs CCS200/M Compact Spectrometer. Keyence laser scanning microscope VK-X250 was used to measure the sample thickness in dry/humid states. The mechanical properties of samples were measured with a tensile machine Instron 5942 using a 10 N load cell with a displacement rate of 0.05 mm s−1. In the tensile test, CLCN films in the size of 10 mm × 20 mm were used. The thickness of films at different states was measured for the calculation of corresponding Young's moduli.
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6

PEG1000 Thermal and Structural Analysis

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The specific volume expansion ratio was obtained using a gravity density cup. The material temperature was saturated in an oven for 4 h at each step. The melting temperature was measured by differential scanning calorimetry (DSC, Discovery DSC, TA Instruments) under a nitrogen atmosphere. The average heights of the molded PEG1000 and cross-sectional images were obtained with a 3D laser microscope (VK-X250, Keyence).
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7

Surface Morphology Analysis of CA Film on Ti

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The surface morphology of the CA film deposited on the Ti substrate was observed under a scanning electron microscope (SEM; JSM-5600LV, JOEL Ltd., Tokyo, Japan) at an accelerating voltage of 15 kV after sputter coating with Au using an ion coater (QUICK COATER SC-701, Sanyu Electron, Tokyo, Japan). Three-dimensional observations of surface morphology were performed by a shape analyzer laser microscope (VK-X250, KEYENCE, Osaka, Japan). Images were acquired in three-dimensional ranges of decreasing size of 25 × 25 μm2. Two surface parameters, three-dimensional arithmetic height (Sa) and surface deployment area rate (Sdr), were obtained.
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8

Surface Topography Analysis of Coatings

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The surface
profile of different coatings developed in this study was studied
using a confocal laser scanning microscope-based profilometer (VK-X250,
KEYENCE, Japan) in combination with its MultiFileAnalyzer analysis
software (KEYENCE, Japan). To determine the surface roughness, three
regions of interest (ROI) and four lines of interest (LOI) were selected
per sample. ROI and LOI were used to calculate the arithmetic mean
heights over surface (Sa) and over line (Ra), respectively. In addition,
the surface of the coatings was imaged using a scanning electron microscope
(Teneo, FEI, USA) at a magnification of 2000X, an accelerating voltage
of 2 keV, and a working distance of approximately 10 mm. Prior to
SEM imaging, the samples were sputter-coated with a gold layer (SC7620,
Quorum, UK) for increasing the surface conductivity.
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9

Hybrid Materials Shear Testing

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The static and dynamic shear testing of the hybrid materials was performed according to the relevant standards [59 ,60 ,61 ]. The dimensions of the shear test specimens are shown in Figure 1.
Furthermore, the influence of artificial aging (0.5 MPa, 70 °C, 14 days [62 ]) on the static shear strength was evaluated. Accordingly, six different groups (Table 1) were characterized, and each group contained n = 5 specimens.
The static shear tests were conducted using a universal testing machine (Zwick 50kN RetroLine, Zwick Roell, Ulm, Germany). The specimens were loaded until fracture at a rate of 2.5 mm × min−1. The fatigue tests were performed using an electro-dynamic testing machine (ElectroForce 3510, TA Instruments—Waters LLC, Eden Prairie, MN, USA) with a sinusoidal load between 1 MPa and 10 MPa and a frequency of 10 Hz [63 ]. Furthermore, 107 cycles were defined as a successful test [59 ].
After mechanical testing, the fractured surfaces of all specimens were analyzed with a digital microscope (VHX-6000) and laser scanning microscope (VK-X250) (both obtained from Keyence Corporation, Osaka, Japan) to determine the causes of fracture.
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10

Characterization of Porous Titanium Alloy Specimens

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The biological characterization was performed with both densely and open porous lattice–structured specimens. Cylindrical dense specimens (d = 12 mm, h = 2 mm) were fabricated in 0° and 90° build orientation, leading to six different groups [Ti–20Nb–6Ta, Ti–27Nb–6Ta, Ti–35Nb–6Ta] × [0°, 90°] with n = 38 specimens each. Additionally, specimens made of Ti–6Al–4V serving as a reference were manufactured in 0° and 90° build orientations. The surfaces were not further processed and are referred to as “as-printed” in the following. Open porous lattice-structured specimens were manufactured consisting of one layer of the above-described face-centered cubic unit cells (Figure 1D). Accordingly, the specimens were 12 mm in diameter and 2 mm in height, i.e., 1 mm of dense structure and 1 mm of open porous lattice structure. Prior to their biological testing, all specimens were cleaned in an ultrasonic bath to remove residual powder and heat-sterilized at 180 °C for 135 min.
The surface roughness of the dense specimens was analyzed with a laser-scanning microscope (VK-X250, Keyence Germany GmbH, Neu-Isenburg, Germany) with 20 times magnification, λS = 8, and λC = 25. The roughness values are summarized in Table 3, and light microscopic images are shown in Figure 1E. The light microscopic images demonstrated melt tracks and partly melted particles on the surface.
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