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Q20 dsc system

Manufactured by TA Instruments
Sourced in United States

The Q20 DSC system is a differential scanning calorimetry (DSC) instrument designed for thermal analysis. It measures the heat flow associated with transitions in materials as a function of temperature or time, providing information about physical and chemical changes that occur in the sample.

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2 protocols using q20 dsc system

1

Thermal and Spectroscopic Characterization of Samples

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1H NMR spectra of the samples were recorded on a Varian Unity 400 MHz spectrometer, using tetramethylsilane (TMS) as an internal standard and employing chloroform-d as the solvent in the room temperature test, and 1, 2-dichlorobenzene-d4 as the solvent in the variable temperature test.
FTIR was performed on a Bruker Vertex 70 FTIR spectrometer equipped with a heating cell. The samples for FTIR analysis were first dissolved in CH2Cl2 to form a homogeneous concentrated solution and then cast onto a KBr window, and after solvent evaporation, a transparent film was obtained and used in situ, and the result was recorded at different temperatures.
Differential scanning calorimetry (DSC) analysis was performed on a Q20 DSC system (TA Instruments) under a nitrogen atmosphere in the temperature range of −30 °C to 80 °C at a heating rate of 5 °C min−1. The samples were heated twice to eliminated thermal history, and the transition temperature was taken from the second heating curve.
Dynamic mechanical analysis (DMA) of the specimen was performed on a TA Instrument DMA Q800 system in a film tension clamp using “multi-frequency strain mode” with a frequency of 1 Hz. The temperature was increased from −30 °C to 75 °C at a heating rate of 5 °C min−1. Rectangular specimens (7.2 × 7 × 0.2 mm3) were prepared for analyses.
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2

Comprehensive Characterization of Novel Nitrogen-Enriched Carbon Aerogels

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Scanning electron microscopy (SEM) images were taken by JSM-6510LV, Japan. Thermogravimetric analysis was performed using a Q50 TGA system and Q20 DSC system (TA Instruments-Waters LLC, US). 4 mg sample was used for the analysis. Samples were heated in nitrogen from 50 °C to 850 °C at a heating rate of 5 °C/min. X-Ray diffraction (XRD) measurements were performed on a Shimadzu diffractometer (XRD-7000, Tokyo, Japan) operating in reflection mode with Cu Kα radiation at a step size of 0.06 per second. Fourier Transform infrared spectroscopy (FTIR) spectra were recorded using a Thermo Nicolet 6700 FTIR spectrometer from 400 to 4000 cm - 1 . The specific surface area of NECAGs was obtained using a Brunauer-Emmett-Teller apparatus (BET, Micromeritics, ASAP2020). The compressive tests were performed in an Instron (Micro Tester, 5848, Instron) using a 10 N load cell and strain control mode with a strain rate of 1 mm/min. The electrical conductivity of NECAGs was characterized using the set-up shown in Figure 4(a) where the resistivity (R) of NECAG monoliths was measured by a multimeter. As R=ρ×L/A = ρ×4L/πD 2 (ohm law), thus the conductivity (S) of CAG S= 1⁄ρ = 4L/πRD 2 , where L is the length and D is the diameter of the probe as shown in Fig. S2.
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