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31 protocols using pyris diamond

1

Characterization of Polymeric Films and Nanofibers

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The infrared (IR) spectra were collected from the carriers and the raw materials with a universal attenuated total reflectance Fourier transform IR spectroscope (ATR-FTIR, UATR Two, Perkin Elmer, Llantrisant, UK). The measurements were conducted in a spectral range from 450 to 4000 cm−1 with 4 scans per spectrum (n = 3). The data collection and the baseline correction of the IR spectra were performed with Spectrum 10.03 software (PerkinElmer, Llantrisant, UK).
The thermal properties of the SC films and electrospun NFs were measured by differential scanning calorimetry (DSC, Pyris Diamond, PerkinElmer, Waltham, MA, USA). Samples of 1–3 mg were analyzed in 30 µL aluminum pans with pierced lids. A heating rate of 10 °C/min was used in a measuring range of 25–250 °C. An N2 purge gas was used with a flow rate of 40 mL/min. The DSC system was calibrated using indium (156.6 °C). Thermograms were baseline corrected prior to analysis.
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2

Mechanical Characterization of Polymer Scaffolds

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Mechanical characterization of scaffolds was determined using a Pyris Diamond dynamic mechanical analyzer (DMA) (PerkinElmer, Waltham, MA, USA). Uniaxial tensile analysis was performed on scaffolds while stretched at 50 μm/min to the point of failure. The elastic modulus and tensile strength were extrapolated from the stress versus strain data of each scaffold. Tensile strength was identified as the highest stress measured from the polymer construct during strain. All samples were strained to the point of failure. The elastic modulus was calculated according to eq 7, where F is the force exerted on the polymer sample, A is the sample cross-sectional area, L0 is the initial sample length, and ΔL is the change in sample length after straining
E= stress / strain =(F/A)/(ΔL/L0)
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3

Morphological Characterization of Nanocapsules

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The morphology of the PDA-EGaIn nanocapsules, graphene sheets, and DGP were investigated via scanning electronic microscopy (FE-SEM, Quanta FEG250, FEI, Waltham, USA). The core–shell structure of the PDA-EGaIn nanocapsules was further characterized by Fourier infrared spectroscopy (MB3000, ABB, Zurich, Switzerland) and transmission electron microscopy (F200×, The Thermo Scientific, Waltham, MA USA). High-angle annular dark-field and energy-dispersive X-Ray spectroscopy (EDS) were carried out using the scanning transmission electron microscopy (STEM) mode of the TEM. The thermal conductivity of the graphene paper can be calculated by the equation λ = α × Cp × ρ, in which thermal diffusivity (α) was measured using LFA 467 HyperFlash® system (NETZSCH, Selbu, Germany) and specific heat capacity (Cp) was evaluated using a differential scanning calorimeter (DSC) (PYRIS Diamond™, Perkin Elmer, Waltham, USA). An infrared camera (Fluke, Ti400, Everett, WA, USA) was used to capture IR images.
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4

Differential Scanning Calorimetry of Starch and Flour

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Determination of gelatinization properties of starch and flour samples were carried out using a differential scanning calorimeter (DSC) (Pyris Diamond, PerkinElmer, Waltham, MA, USA) equipped with an Intracooler 2P cooling system. Calibration was performed with indium and n-decan for a temperature range from +20 to +95 °C. Each sample was mixed with deionized water (flour: water ratio = 1:3), filled in DSC pans (20–35 mg) and hermetically sealed. After 2 min of equilibration at 25 °C, samples were heated to 95 °C at 10 K/min in a nitrogen atmosphere. The gelatinization onset (To), peak (Tp), and conclusion temperatures (Tc), and the enthalpy of gelatinization (ΔH) were determined using the Pyris software.
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5

Comprehensive Structural Analysis of VG

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The morphology and detailed structure of VG was investigated by SEM (FEI Quattro S, acceleration voltage 5–10 kV, TEM (FEI Tecnai F20; acceleration voltage 200 kV); Raman spectroscopy (Horiba, LabRAM HR 800, 532 nm laser wavelength), XPS (Kratos Analytical Axis‐Ultra spectrometer with Al Kα X‐ray source). The thermal diffusivities (α) of the sample were measured using LFA 467 MicroFlash system (NETZSCH, Germany). The specific heat capacity of the sample evaluated by using a DSC (PYRIS Diamond, PerkinElmer, USA). The infrared (IR) photos were captured by using an infrared camera (Fluke, Ti400, USA).
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6

Thermal Analysis of DOX-NCPE Interactions

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A differential scanning calorimeter (DSC, Perkin-Elmer Pyris Diamond) was used to observe the change in the crystal form of DOX with or without being encapsulated by NCPE. Differential scanning calorimetry runs were performed over a temperature range from 25°C to 400°C at a heating rate of 10°C per minute. Free DOX and blank NCPE were selected as the controls.
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7

Structural Characterization of Hydroxyapatite Scaffolds

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Fourier transform infrared (FT-IR) spectrum of the products was recorded on a Magna-IR, spectrometer 550 Nicolet in KBr pellets in the range of 400–4000 cm−1. Micrographs of HA powders were taken by using a field-emission scanning electron microscope (FE-SEM, TESCAN, Brno, Czech Republic). Powder X-ray diffraction (XRD) patterns were collected from a diffractometer of Philips Company (Amsterdam, The Netherlands) with X’Pert Pro monochromatized Cu Kα radiation (λ = 1.54 Å, operated on 35 mA and 40 kV current).
For microstructural studies, the porous scaffolds were frozen at −50 °C and cross-sectionally cut to small pieces by a sharp surgical blade. After gold sputtering, the cross-sections were observed by SEM. Pore size distribution of the porous scaffolds were supplied by Digimizer software. Thermogravimetric analysis (TGA) and derivative thermogravimetry (DTG) were carried out with Pyris Diamond Perkin Elmer, under air atmosphere, at a heating rate of 10 °C/min, from room temperature to 1200 °C.
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8

Thermal Analysis of Polymer Films

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Thermogravimetric analysis of MET-PGA-, R1- and R2-derived films was performed using a thermogravimetric analyzer TGA/DTG Perkin-Elmer PyrisDiamond, equipped with gas station. Samples (3–4 mg) were placed in an open ceramic crucible and heated from 25 °C to 600 °C at a speed rate of 10 °C·min−1, under nitrogen flow of 30 mL·min−1. Before testing, samples were conditioned for 24 h at 25 °C and 50% RH. Thermal properties of MET-PGA-, R1- and R2-derived films were investigated by using a Q2000 T zero differential scanning calorimeter (DSC), TA Instrument (New Castle, DE, USA), equipped with a liquid nitrogen accessory for fast cooling. The calorimeter was calibrated in temperature and energy using indium. Dry nitrogen was used as purge gas at a rate of 30 mL·min−1. Samples (3–4 mg) were weighed and placed individually in aluminum pans; an empty pan was then used as reference. DSC measurements were performed in double heating run; the first one, occurring from 50 to 200 °C, at 10 C·min−1, could reproduce the thermal history of the samples. After an isothermal step of one min, non-isothermal crystallization experiments were performed by cooling the specimens up to −50 °C, at a rate of 10 C·min−1. Finally, a second heating ramp from −50 °C to 250 °C at 10 °C·min−1 was recorded. Before testing, the samples were conditioned for 24 h at 25 °C and 50% RH.
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9

Thermal Analysis of Biocomposite Materials

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The thermal characteristics of GCLPL, GCLPH, GCHPL, and GCHPH, biocomposites with weight between 2–10 mg were recorded using a Perkin-Elmer Pyris Diamond differential scanning calorimeter. All the samples were lightly pressed into the bottom of the pan to ensure good thermal contact. Sealed DSC pans were used in the study. Triplicate samples were heated at a rate of 10 °C/min from 10 °C to 100 °C. Peak melting temperature (Tm) and heat of fusion data for the PCL component of the materials were determined using the built-in software of the DSC. The latter measurement was subsequently used to estimate the percentage crystallinity of PCL in the composites from the reported heat of fusion of 139.5 J/g for fully crystalline PCL (Burke, 1987 (link)). Indium was used as a standard.
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10

Comprehensive Structural Characterization of Nanocomposites

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SEM (Hitachi S4800) was carried out to study the morphologies of the composites and the electrodes. The internal structure and element distribution of the nanoarchitectures were studied by TEM (FEI Tecnai F20). The surface structural characteristics of the sample were analyzed by X-ray photoelectron spectroscopy (XPS) (Thermo Scientific K-Alpha, USA). Raman spectra were constructed through a Renishaw inVia Reflex Raman spectrometer with excitation by a 532 nm-wavelength laser. The XRD images were collected via an AXS D8 Advance diffractometer (Cu-Kα radiation, 40 mA, 40 kV) from Bruker, Inc. (Germany). Thermogravimetric analysis (TGA) was performed by using a Pyris Diamond, PerkinElmer, USA from 30 °C to 800 °C at a ramp rate of 10 °C min−1. The specific surface area and pore size distribution of the samples were measured based on the Brunauer–Emmett–Teller (BET) and Barrett–Joyner–Halenda (BJH) methods, respectively.
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