Determining the time-dependent effective relaxation time of biofunctionalized magnetic nanoparticles conjugated with biotargets by using a high-Tc SQUID-based ac susceptometer for a magnetic immunoassay

2017 ◽  
Vol 238 ◽  
pp. 66-70 ◽  
Author(s):  
Shu-Hsien Liao ◽  
Yu-Kai Su
RSC Advances ◽  
2018 ◽  
Vol 8 (8) ◽  
pp. 4057-4062 ◽  
Author(s):  
Shu-Hsien Liao ◽  
Han-Sheng Huang ◽  
Jean-Hong Chen ◽  
Yu-Kai Su ◽  
Yuan-Fu Tong

This study determined the characteristics of the time-dependent effective relaxation time τeff and magnetization M when biofunctionalized magnetic nanoparticles (BMNPs) associated with biomarkers in a liquid immunoassay.


Entropy ◽  
2021 ◽  
Vol 23 (2) ◽  
pp. 193 ◽  
Author(s):  
Giovanni Alberto Ummarino ◽  
Antonio Gallerati

We calculate the possible interaction between a superconductor and the static Earth’s gravitational fields, making use of the gravito-Maxwell formalism combined with the time-dependent Ginzburg–Landau theory. We try to estimate which are the most favorable conditions to enhance the effect, optimizing the superconductor parameters characterizing the chosen sample. We also give a qualitative comparison of the behavior of high–Tc and classical low–Tc superconductors with respect to the gravity/superfluid interplay.


Author(s):  
Yingxin Gao ◽  
Alan S. Wineman ◽  
Anthony M. Waas

There is experimental evidence to suggest that extensible connective tissues are mechanically time-dependent. In view of this, the mechanics of time-dependent lateral stress transfer in skeletal muscle is investigated by employing a viscoelastic shear lag model for the transfer of tensile stress between muscle fibres and the surrounding extracellular matrix (ECM) by means of shear stresses at the interface between the muscle fibre and the ECM. The model allows for both mechanical strains in the muscle as well as the strain owing to muscle contraction. Both the ECM and the muscle fibre are modelled as viscoelastic solids. As a result, time-dependent lateral stress transfer can be studied under a variety of loading and muscle stimulation conditions. The results show that the larger the muscle fibre creep time relative to the ECM relaxation time, the longer it takes for the muscle fibre stress to relax. It also shows that the response of the muscle–ECM composite system also depends on the characteristic time of a strain history relative to the characteristic relaxation time of the ECM. The results from the present model provide significant insight into the role of the parameters that characterize the response of the muscle composite system.


2012 ◽  
Vol 109 (4) ◽  
pp. 685-690 ◽  
Author(s):  
Hanna Maria Baranowska ◽  
Marek Sikora ◽  
Magdalena Krystyjan ◽  
Piotr Tomasik

2019 ◽  
Vol 46 (9) ◽  
pp. 4070-4076 ◽  
Author(s):  
Yipeng Shi ◽  
John B. Weaver

2021 ◽  
Vol 521 ◽  
pp. 167535
Author(s):  
Lennart J. Gresing ◽  
Patricia Radon ◽  
Ralf P. Friedrich ◽  
Diana Zahn ◽  
Martin Raasch ◽  
...  

2013 ◽  
Vol 20 (1) ◽  
pp. 012503 ◽  
Author(s):  
J. S. Wrobel ◽  
C. J. Hansen ◽  
T. R. Jarboe ◽  
R. J. Smith ◽  
A. C. Hossack ◽  
...  

2007 ◽  
Vol 574 ◽  
pp. 495-505 ◽  
Author(s):  
HUDONG CHEN ◽  
STEVEN A. ORSZAG ◽  
ILYA STAROSELSKY

We derive, without approximation, a closed-form macroscopic equation for finite Knudsen number flow using the Boltzmann–BGK kinetic theory with constant relaxation time. This general closed-form equation is specialized into a compact integro-differential equation for time-dependent isothermal unidirectional flows and results are presented for channel flow. This equation provides a clear demonstration of the effects of finite Knudsen number, and it also illustrates the limitations of the Boltzmann–BGK theory with constant relaxation time and bounce-back boundary conditions.


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