A novel method for direct measurement of the pKa's of weakly acidic hydrocarbons

1978 ◽  
Vol 43 (9) ◽  
pp. 1812-1813 ◽  
Author(s):  
J. O. Stoffer ◽  
D. R. Strait ◽  
D. L. Filger ◽  
E. T. Lloyd ◽  
C. Crain
2019 ◽  
Vol 123 (1) ◽  
Author(s):  
J. Fu ◽  
M. A. Giorgi ◽  
L. Henry ◽  
D. Marangotto ◽  
F. Martínez Vidal ◽  
...  

2010 ◽  
Vol 54 (5) ◽  
pp. 599-600 ◽  
Author(s):  
Gayatri Sharma ◽  
David Muller ◽  
Stephen O'Riordan ◽  
Sinead Bryan ◽  
Peter Hindmarsh ◽  
...  

2014 ◽  
Vol 178 (1) ◽  
pp. 142-153 ◽  
Author(s):  
A. M. Blom ◽  
E. B. Volokhina ◽  
V. Fransson ◽  
P. Strömberg ◽  
L. Berghard ◽  
...  

2011 ◽  
Vol 7 (S284) ◽  
pp. 442-445
Author(s):  
Alberto Domínguez

AbstractThe extragalactic background light (EBL) is of fundamental importance both for understanding the entire process of galaxy evolution and for γ-ray astronomy. However, the overall spectrum of the EBL between 0.1 and 1000 μm has never been determined directly, neither from observed luminosity functions (LFs), over a wide redshift range, nor from any multiwavelength observation of galaxy spectral energy distributions (SEDs). The evolving overall spectrum of the EBL is derived here utilizing a novel method based on observations only. It is emphasized that the local EBL seems already well constrained from the UV up to the mid-IR. Different independent methodologies such as direct measurement, galaxy counts, γ-ray attenuation and realistic EBL modelings point towards the same EBL intensity level. Therefore, a relevant contribution from Pop III stars to the local EBL seems unlikely.


2015 ◽  
Vol 5 (1) ◽  
pp. 10-14 ◽  
Author(s):  
Muhammad Saiedullah ◽  
Nasreen Chowdhury ◽  
Md Aminul Haque Khan

Background: Friedewald’s formula (FF) is used worldwide to calculate low-density lipoprotein cholesterol (LDL-chol). But it has several shortcomings: overestimation at lower triglyceride (TG) concentrations and underestimation at higher concentrations. In FF, TG to very low-density lipoprotein cholesterol (VLDL-chol) ratio (TG/VLDL-chol) is considered as constant, but practically it is not a fixed value. Recently, by analyzing lipid profiles in a large population, continuously adjustable values of TG/VLDL-chol were used to derive a novel method (NM) for the calculation of LDL-chol. Objective: The aim of this study was to evaluate the performance of the novel method compared with direct measurement and regression equation (RE) developed for Bangladeshi population. Materials and Methods: In this cross-sectional comparative study we used lipid profiles of 955 adult Bangladeshi subjects. Total cholesterol (TC), TG, HDL-chol and LDL-chol were measured by direct methods using automation. LDL-chol was also calculated by NM and RE. LDL-chol calculated by NM and RE were compared with measured LDL-chol by twotailed paired t test, Pearson’s correlation test, bias against measured LDL-chol by Bland-Altman test, accuracy within ±5% and ±12% of measured LDL-chol and by inter-rater agreements with measured LDL-chol at different cut-off values. Results: The mean values of LDL-chol were 110.7 ± 32.0 mg/dL for direct measurement, 111.9 ± 34.8 mg/dL for NM and 113.2 ± 31.7 mg/dL for RE. Mean values of calculated LDL-chol by both NM and RE differed from that of measured LDL-chol (p<0.01 for NM and p<0.0001 for RE). The correlation coefficients of calculated LDL-chol values with measured LDL-chol were 0.944 (p<0.0001) for NM and 0.945 (p<0.0001) for RE. Bland- Altman plots showed good agreement between calculated and measured LDL-chol. Accuracy within ±5% of measured LDL-chol was 49% for NM, 46% for RE and within ±12% of measured LDL-chol was 79% for both NM and RE. Inter-rater agreements (?) between calculated and measured LDL-chol at LDL-chol <100 mg/dL, 100–130 mg/dL and >130 mg/dL were 0.816 vs 0.815, 0.637 vs 0.649 and 0.791 vs 0.791 for NM and RE respectively. Conclusion: This study reveals that NM and RE developed for Bangladeshi population have similar performance and can be used for the calculation of LDL-chol. DOI: http://dx.doi.org/10.3329/jemc.v5i1.21491 J Enam Med Col 2015; 5(1): 10-14


Nanoscale ◽  
2015 ◽  
Vol 7 (42) ◽  
pp. 17637-17641 ◽  
Author(s):  
A. M. Katzenmeyer ◽  
G. Holland ◽  
J. Chae ◽  
A. Band ◽  
K. Kjoller ◽  
...  

Scanning thermal infrared microscopy (STIRM) is a novel method that provides the chemical composition and thermal conductivity information with nanoscale resolution.


2020 ◽  
Vol 67 (3) ◽  
pp. 2422-2429 ◽  
Author(s):  
Jernej Herman ◽  
Samo Begus ◽  
Polona Mihalic ◽  
Jovan Bojkovski

Author(s):  
Rajender Katkam ◽  
Tania To ◽  
Matthew Hibert ◽  
Patrick Shaughnessy ◽  
Irina Erengurg ◽  
...  

2020 ◽  
Vol 493 (2) ◽  
pp. 1782-1787 ◽  
Author(s):  
Shuang-Xi Yi ◽  
Yuan-Chuan Zou ◽  
Xuan Yang ◽  
Bin Liao ◽  
Shao-Wen Wei

ABSTRACT In this paper, we present a novel method to test the Einstein equivalence principle (EEP) using (simultaneous) multi-wavelength radio observations of polarized blazars. We analyse simultaneous multi-wavelength polarization observations of 3C 279 at 22, 43, and 86 GHz obtained by two antennas of the Korean VLBI Network. We obtained 15 groups of polarization data, and applied the Metropolis–Hastings Markov chain (MHMC) to simulate the parameters when considering the EEP effect and the simplest form of Faraday rotation (single external Faraday screen). The final results show the constraint of the parametrized post-Newtonian (PPN) parameter γ discrepancy as Δγp = (1.91 ± 0.34) × 10−20. However, the single external Faraday screen is an oversimplification for blazars because there are numerous observations showing complex Faraday rotation behaviour for blazars due to internal/external Faraday dispersion, beam depolarization, etc. The Δγp results of this paper can only be considered as upper limits. Only if all other effects are revealed and considered should the result be taken as a direct measurement of the violation of the EEP.


1978 ◽  
Vol 9 (37) ◽  
Author(s):  
J. O. STOFFER ◽  
D. R. STRAIT ◽  
D. L. FILGER ◽  
E. T. LLOYD ◽  
C. CRAIN

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