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37 protocols using ta q2000

1

Differential Scanning Calorimetry Measurements

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Measurements of heat flow dQ/dT were performed at atmospheric pressure using a commercial TA Q2000 differential scanning calorimeter at 10 K min−1. Heat |Qf|=| (dQ/dT′)dT′| and entropy change |ΔSf|=| (dQ/dT′)/T′dT′| across the full transition were obtained after subtracting baseline backgrounds32 , with Ta chosen above (below) the transition on cooling (heating) and Tb chosen below (above) the transition on cooling (heating). The entropy change on partially driving the transition by heating to temperature T is ΔS(T)= (dQ/dT′)/T′dT′. The entropy change on partially driving the transition by cooling to temperature T is ΔS(T)=|ΔSf|− (dQ/dT′)/T′dT′.
Zero-field heat capacity data were obtained using the TA Q2000 on cooling in the modulated differential scanning calorimetry mode, with the constant temperature method33 . The temperature step was 1 K, the temperature modulation was 0.5 K and the period was 60 s.
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2

Thermal Analysis of Material Samples

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TMDSC measurements were performed on ∼10 mg of the sample, using a Q2000 TA Instruments set-up equipped with a liquid nitrogen cooling system. A helium flow rate of 25 mL/min was used throughout. Measurements were performed by placing the sample in sealed aluminum pans. Data were acquired on cooling at an average rate of 3 K/min, where the temperature oscillated around the average value with 0.5 K amplitude and a 60 s period.
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3

Thermal Behavior Analysis of Films

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To measure the thermal behavior of the films with and without post-treatments, DSC technique was used in a Q2000 TA Instruments unit. The samples were subjected to a temperature scan from 30 to 320°C and a heating rate of 10°C/min. In order to remove the water content in the samples and improve the baseline of thermogram, an isotherm at 120°C was performed prior to measurement in all cases.
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4

Characterization of Nonlinear Optical Materials

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All chemicals were commercially available and used without further purification. FT-IR spectra of KBr pellets were recorded on a Perkin-Elmer Spectrum One FT-IR spectrometer from 4000 to 400 cm−1. PXRD patterns (Cu-Kα) were collected on a Bruker Advance D8 θ–2θ diffractometer. Thermogravimetric analyses (TGA) were carried out on a TA Q50 system at a heating rate of 10 K min−1 in a N2 flow. Differential scanning calorimeter (DSC) measurements were performed on a TA Q2000 instrument, at a heating/cooling rate of 10 K min−1. Variable-temperature SHG experiments with a programmable temperature control system were executed by Kurtz-Perry powder SHG test using an Nd:YAG laser (1064 nm). The values of the NLO coefficients for SHG were determined by the comparison with commercialized KDP (KH2PO4).
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5

Isothermal Crystallization Analysis of Polymers

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The DSC studies were carried out using a TA Instruments temperature modulated DSC (TA Q2000, TA Instruments, New Castle, DE, USA). The instrument was previously calibrated with indium for the accurate determination of heat flow and temperature. The sample mass was kept constant at around 5 mg for all crystallization kinetics tests, while a nitrogen gas flow of 50 mL/min was purged into the DSC cell. The sample and reference pans were of identical mass, with an error ±0.01 mg.
Initially the samples were cooled to 0 °C and then heated at a rate of 20 °C/min to a temperature 40 °C higher than the melting temperature. The samples were held at this temperature for 5 min in order to erase any thermal history and were then cooled back to the isothermal crystallization temperature (Tc) with the highest achievable rate. At that temperature, the sample was held for a time tc, which was selected based on the recommendations from Muller and co-workers, that crystallization time should be 5 times the time to reach the minimum of the exothermic signal generated as a function of time at Tc [36 (link)]. After the samples were isothermally crystallized at different temperatures, they were re-heated at a rate of 20 °C/min up to 230 °C, in order to study their melting behaviour after isothermal crystallization.
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6

Thermal Stability of Proteins

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Changes in thermal stability of proteins were measured using a differential scanning calorimeter (TA Q2000, TA Instruments, New Castle, DE, USA) as previously described by Liu et al. [17 (link)] with slight modifications. Thawed samples (10 mg) were accurately weighed and placed in a tightly sealed aluminum pan, while a sealed empty aluminum pan was used as a control group. Samples were equilibrated at 20 °C for 2 min and then heated from 20 to 100 °C at a heating rate of 5 °C/min.
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7

Characterization of Shape-Memory Properties

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The shape-memory property was characterized by a dynamic mechanical analyzer (DMA, type: TA Q800). The maximal force was 18 N and the resolution was 0.1 mN. Using stretching mode, the strain and stress could be auto detected. In addition, the temperature could be controlled by a temperature sensor. In order to avoid sliding, the sample was clamped tightly. Differential scanning calorimetry (DSC) measurements were conducted using a TA Q2000 machine under N2 at a temperature ramping rate of 5 °C/min. Mechanical tests were performed using a Zwick/Roell tensile machine at a stretching speed of 10 mm/min and the sample geometry was 25 mm × 5 mm × 0.3 mm. The applied force sensor was 1.5 kN, and it utilized physical clamps.
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8

Structural and Thermal Analysis of Post-Impact Glasses

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For the post-impact glasses, structural analyses were performed by HRTEM and SAED. The thermal response of glasses was investigated with differential scanning calorimetry (DSC; TA Q2000): heating the glass up to 823 K in a pure argon atmosphere at a heating rate of 20 K/min and subsequent cooling to room temperature at the same rate. The specific heat capacity was measured under high vacuum conditions with a Quantum Design physical property measurement system (PPMS), which allows cooling down to 2 K with a liquid helium system. For comparison, both DSC and PPMS measurements were also performed on the original as-cast glasses.
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9

Thermal Properties of Polylactic Acid

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The glass transition temperatures, cold crystallization temperature, melting temperatures and degree of crystallinity of PLA were measured on a TA Q-2000 differential scanning calorimeter (DSC). All DSC samples were heated to 200 °C at 20 °C min−1 and held in the molten state for 5 min, then cooled to 0 °C as quickly as possible, at last ramped the temperature from 0 °C to 200 °C at 10 °C min−1. Degree of crystallinity (Xcc) after cold crystallization was calculated as follows: where ΔH100%m is the theoretical melting enthalpy for PLA with 100% of crystallinity (93.1 J g−1); ΔHcc is the crystallization enthalpy; w is the mass fraction of the additive.
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10

Thermal Analysis of PEG-SNA Nanoparticles

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Individual samples of the PEG shell, unmedicated SNA 15 base, AS, AMT, AS HTS and AMT HTS were thermally analysed using a differential scanning calorimeter (TA Q2000, TA instruments, New Castle, DE, USA) equipped with TA-Q Universal Analysis 2000 software. Approximately 5–7 mg sample was precisely weighed and heated from 0–250 °C at a rate of 5 °C/min, with nitrogen gas flowing at 20 mL/min. Interference in the melting behaviour of the HTS shell and the drug loaded core was evaluated for each sample.
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