A rapid and specific liquid chromatographic–tandem mass spectrometric method is described for simultaneous analysis of valsartan (VAL) and hydrochlorothiazide (HCTZ) in human plasma. VAL and HCTZ were chromatographed on a C8 column with 75:15:10 (v/v) acetonitrile–methanol–0.001% aqueous ammonia as mobile phase. VAL and HCTZ were eluted at 0.69 min and 1.22 min, respectively, and, after electrospray ionization (ESI), detected in selected-reaction-monitoring mode. The precursor to product-ion transitions m/z 434.32 → 179.22 and m/z 295.85 → 204.86 were used to quantify VAL and HCTZ, respectively. Recovery by solid-phase extraction was >90% for both analytes and the internal standard. The method was suitable for application to a pharmacokinetic study after oral administration of tablet containing 160 mg VAL and 25 mg HCTZ to 18 healthy volunteers. 相似文献
A rapid liquid chromatographic method with electrospray ionization tandem mass spectrometric detection has been developed and validated for quantification of quetiapine in heparinized human plasma. Plasma samples, without a drying and reconstitution step, were extracted by solid-phase extraction and eluted with acetonitrile. The analyte and zolpidem tartrate (internal standard, IS) were chromatographed on a C18 column; the mobile phase was 85:15 (v/v) acetonitrile–5 mM ammonium formate, pH adjusted to 4.5 with formic acid, at a flow rate of 0.5 mL min−1. The retention times of quetiapine and the IS were 1.25 and 1.05 min, respectively, and the run time was 1.8 min per sample. Selected reaction monitoring of MH+ at m/z 384.12 and 308.11 resulted in stable fragment ions with m/z 253.02 and 235.09 for quetiapine and the IS, respectively. Response was a linear function of concentration in the range 1.0–240.0 ng mL−1, with r ≥ 0.9994. Recovery of quetiapine and the IS ranged from 74.82 to 85.57%. The assay has excellent characteristics and has been successfully used for analysis of quetiapine in healthy human subjects in a bioequivalence study.
Electrochemical DNA sensor has been fabricated by immobilizing thiolated single stranded oligonucleotide (ssDNA) probe onto gold (Au) coated glass electrode for meningitis detection using hybridization with complementary DNA (CtrA) in presence of methylene blue (MB). These electrodes (ssDNA/Au and dsDNA/Au) have been characterized using atomic force microscopy (AFM), Fourier transform infrared spectroscopy (FT-IR), electrochemical impedance spectroscopy (EIS) and cyclic voltammetric (CV) technique. The DNA/Au electrode can detect the complementary DNA in the range of 7–42 ng/μl in 5 min (hybridization) with response time 60 s and electrode is stable for about 4 months when stored at 4 °C. The sensitivity of dsDNA/Au electrode is 115.8 μA/ng with 0.917 regression coefficient (R). 相似文献
Magnetic hyperthermia experiments were carried out using a biphasic gel of La1−xSrxMnO3(LSMO) and γ-Al0.07 Fe1.93O3 with an AC magnetic field of amplitude 88 mT and a frequency of 108 kHz. Specific absorption rate (SAR) increases with the increased ratio of Al-substituted maghemite. The Tmax value for the gels prepared by the mixture of LSMO and Al-substituted maghemite can be adjusted to suit therapeutic temperature. The time required to reach optimum temperature decreased with the increased ratio of later. Such biphasic gel could be very useful for magnetic hyperthermia with in vivo control of temperature. 相似文献
Partial discharge (PD) causes premature insulation failure of transformers. It is essential to detect PD to avoid unwanted failure of transformers. Only detection of PD is not sufficient for a transformer of huge size, unless it is possible to locate. Acoustic partial discharge measurement is advantageous for PD source location. There are different algorithms for PD source location. These are iterative and require large number of acoustic emission (AE) sensors. This paper presents a non-iterative source location algorithm employing four AE sensors. This algorithm is applied to experimental data. Proposed algorithm is also applied to published data and compared with existing iterative methods. Main error for source location is due to arrival time calculation. In order to reduce the error in AE signal arrival time calculation, different arrival time calculation methods are discussed and a comprehensive method is proposed. By applying these methods, arrival time is calculated from measured signal. 相似文献