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23 protocols using oca40

1

Surface Characterization of Coated Membranes

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Unless specified otherwise, coated membranes were used before re-swelling as described in 2.2 and 2.3, uncoated membranes were treated with NaOH as described in 2.2 and 2.3, respectively, and used after drying under vacuum for 1 h at 60 °C.
Membranes were characterized using scanning electron microscopy (SEM), X-ray photoelectron spectroscopy (XPS), infrared spectroscopy (IR) and contact angle measurements. SEM pictures of dry membranes were collected on a Zeiss Leo 1530 VP (Jena, Germany) to analyze the surface morphology. IR spectra were collected on a Vertex 70 spectrometer (Bruker, Germany) (spectra see supporting information). Water-air contact angles of membranes re-swollen in ultrapure water were measured using the captive bubble method with an OCA40 (Dataphysics, Germany). XPS spectra were measured on an AXIS Supra surface analysis instrument (Kratos Analytical, England).
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2

Characterization of Acid-Etched Titanium Surfaces

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The grade IV titanium implants (Carpenter, US) had an identical cylindrical shape with a core diameter of 2.0 mm and three rings with an outer diameter of 3.5 mm and a length of 7.8 mm (Fig. 1a). The titanium sheets were reduced to 4.0 × 2.0 × 0.2 mm, polished, and acid-etched by 4.62 mol L−1 H3PO4 + 0.249 mol L−1 NaF or 5.00 mol L−1 H2SO4 + 5.05 mol L−1 HCl, respectively, at 60 °C for 30 min. After etching, the samples were cleaned with acetone and anhydrous alcohol for 30 min each. Ssk, Sa, surface concave depth (Sv), contact angle, and hydrogen content were examined using white-light interferometry (Taylor Hobson CII, Leicester, United Kingdom), a surface contact angle tester (Dataphysics OCA40, Germany), and inert gas fusion thermal conductivity analysis (ASTM E 1447-09), respectively (n = 25).
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3

Comprehensive Characterization of Carbon Fiber Samples

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The surface morphologies of CF samples were observed via field emission scanning electron microscope (FESEM, FEI Quanta 250 FEG) at an acceleration voltage of 15.0 kV equipped with an energy-dispersive X-ray (EDX) spectroscopy for elemental mapping analysis. X-ray diffraction (XRD) was carried out by XRD system (Bruker AXS, Model D8 Discover) using Cu Kα radiation (λ = 1.5418 Å) at a power of 40 kV × 40 mA. Raman spectra of original and modified electrodes were analyzed by Raman Microscope (Model XploRA PLUS) using a 532 nm exciting wavelength at room temperature. The wettability of the CFs was investigated by contact angle measurement applying a water droplet method using Dataphysics OCA 40.
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4

Contact Angle Measurement of Grafted Surfaces

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The captive bubble technique was used for contact angle measurement because the surfaces are constantly in contact with fluid media. The captive bubble contact angle measurements were taken at 22 °C using a video capture system (OCA 40, Data Physics Instruments GmbH, Filderstadt, Germany). One drop of water was dripped on the graft surfaces. After a few seconds, the static contact angle near the three-phase line was measured.
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5

Characterization of Hydrophobic Particle Coatings

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The morphologies of particles were characterized on a scanning electron microscope (SEM, Hitachi, Tokyo, Japan, S-4800, 20 kV) and the feature sizes of the particles were obtained by measuring at least 200 particles. The SEM samples were sputtered with Au to improve the conductivity. The hydrophobic property of particulate coatings was analyzed with an OCA (Optical Contact Angle) meter (Dataphysics, OCA40, Filderstadt, Germany) via the sessile drop method using the Laplace–Young fitting algorithm. The volume of the water drop was 3 μL and the dispensing speed was 0.5 μL/s. The contact angle values were determined from the average of three measurements at different positions. TGA curves were obtained with a Mettler TGA 1100 SF, and FTIR spectra were collected with ABB FTLA 2000-104 (ABB, Zurich, Switzerland).
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6

Characterization of TiO2@CB/CF Composites

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Scanning electron microscopy (SEM, SU8010, HITACHI, Hitachi, Japan) was performed to observe the chemical element of the TiO2@CB/CF. Fourier-transform infrared (FTIR, NEXUS-670, GNI, Woburn, MA, USA) spectra were used at room temperature from 400 to 4000 cm−1. An ultraviolet-visible-near-infrared spectrometer (UV-vis-NIR, UV 3600, Shimadzu Scientific Instruments, Kyoto, Japan) was used to test the total transmittance (T) and reflectance (R) of a sample. The water contact angles of different materials were obtained with a goniometer (OCA40, Dataphysics, Filderstadt, Germany) using 2 μL of water at ambient temperature.
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7

Contact Angle Analysis of Bioactive Complexes

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The contact angles of the OSAS, SP-EGCG, and OSAS-SP-EGCG complexes were determined using an OCA 40 (Dataphysics Instruments GmbH, Stuttgart, Germany) following the method described by Dai et al. (25 (link)). First, the dried sample powders were pressed to obtain particle-based tablets (13 mm diameter and 2 mm thickness). A drop of pure water (5 μL) was then lightly dripped onto the surface of the tablets. After equilibrium was reached, the droplet was photographed, and the profile of the droplet was automatically fitted to the Laplace-Young equation using software to acquire the contact angle. Measurements were performed at least three times.
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8

Measurement of Static and Roll-off Angles

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Static contact angles (SCA) were attained with a CAM200 contact angle meter (KSV instruments Ltd, Finland). A 10 μL drop was deposited on the capsule-coated glass-slide using a micropipette and images were recorded and analysed by the software (OneAttension, Biolin Scientific, Sweden). The SCA was measured at five different positions on the surface, and in each position more than 20 images were processed.
The surface tensions of the liquids used in the present study were measured with the same instrument and were 72.1 mN m−1 MilliQ-water, 48.4 mN m−1 ethylene glycol, 33.4 mN m−1 olive oil and 27.3 mN m−1 hexadecane.
Methylene Blue and Oil Red O was used to color the water blue and hexadecane red in MOVIE_2, MOVIE_3, MOVIE_4 and Fig. 3E.
Roll-off angles (RAs) were measured with a Dataphysics OCA 40 instrument equipped with a tilting stage. A 10 µL droplet was dispensed on the horizontal surface with a syringe needle after which the sample was tilted at a speed of 0.3° s−1. The roll-off angle was recorded as the tilt angle when the droplet was set in motion (see MOVIE_1.avi). The roll-off angle was measured at 8 different positions on the surface.
All measurements were performed at 23 °C and 50% RH.
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9

Wettability of Ibrutinib Compounds via Contact Angle

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Example 2

The wettability of the below compounds was determined by contact angle measurement. For this purpose, the substances were pressed (2 t*cm−2) to a pellet. On each pellet were placed three water drops (2 μL) on three individual measurement points and the contact angle was measured with the apparatus OCA40 (DataPhysics Instruments) on two sides of the drop. The determined values are given in table below.

API Formcontact angle θ
Ibrutinib free base form A67.9° ± 2.1
Ibrutinib fumaric acid56.8° ± 2.4
Irbutinib succinic acidincapable of measurement*
*The contact angle of the co-crystal of ibrutinib and succinic acid was incapable of measurement because the wettability of this co-crystal is so high that the water drops immediately spread over the surface and the water sunk into the pellet.

A lower contact angle corresponds to an increase in wettability of the substance. An increased wettability facilitates granulation, in particular wet granulation of the substance. Therefore, as the co-crystals of the present invention have a lower contact angle and, thus, an increased wettability compared to ibrutinib free base, the co-crystals have advantageous properties with respect to further processing of the compound into pharmaceutical preparations.

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10

Characterization of Col/BG Nanofibers

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The morphology of the Col/BG nanofibers was observed by scanning electron microscopy (SEM; JSM-5600; JEOL, Tokyo, Japan). Image analysis software (ImageJ, National Institutes of Health) was used to determine the mean fiber diameter by selecting 100 fibers randomly. The weight loss temperature was determined using a thermogravimetric analyzer (209F1; Netzsch, Selb, Germany). The contact angle was measured by a contact angle measuring instrument (OCA40; Dataphysics, Filderstadt, Germany). The elementary composition was measured with an energy dispersive spectrometer (IE 300X; Oxfordshire, UK). The chemical structure and the phase composition were determined with Fourier transform infrared spectroscopy (Avatar 380, Nicolet, Waltham, MA, USA) and X-ray diffraction (D/Max-2550 PC; Rigaku, Tokyo, Japan), respectively. The tensile strength was analyzed with a universal materials testing machine (Hounsfield, H5K-S UTM, Redhill, UK).
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