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1 s of the same samples obtained with a U-tube viscometer.
2 d fluid shear stress applied in a cone-plate viscometer.
3 to pathological shear stress in a cone-plate viscometer.
4 ell-defined shear conditions in a cone-plate viscometer.
5 he effects of nonlinear flow in a cone-plate viscometer.
6 ticle forces and attachment times within the viscometer.
7 plied to cells via a modified cone and plate viscometer.
8 ls of fluid shear stress in a cone-and-plate viscometer.
9 ter, and shear stress using a cone-and-plate viscometer.
11 man neutrophils were sheared in a cone-plate viscometer and the kinetics of aggregate formation was m
13 d transfectants were sheared in a cone-plate viscometer, and formation of heterotypic aggregates was
14 ed to increasing shear rates in a cone-plate viscometer, and levels of intact and cleaved GPVI were e
15 nal variations in adhesion efficiency in the viscometer, and that the overall efficiency is dependent
16 , purified VWF was subjected to shear in the viscometer, and VWF morphology was assessed using light
17 osity data collected previously using a CTOF viscometer, as well as with literature values obtained w
19 was compared with a vacuum-driven capillary viscometer at high shear rates (>500 s(-1)), at which th
20 ells (E3-ICAM) in suspension in a cone-plate viscometer at shear rates typical of venular blood flow
21 w-chamber-based platelet adhesion assays and viscometer-based shear-induced platelet aggregation and
24 imple droplet-based, water-in-oil continuous viscometer capable of measuring viscosity changes in 10
25 ameters; these components make the nanoliter viscometer completely self-calibrating, robust, and easy
26 we report measurements with a time-of-flight viscometer down to [Formula: see text] and up to [Formul
27 To address this challenge, a microfluidic viscometer driven by surface tension was developed to re
29 ress (0.1-4.0 dyn/cm(2)) in a cone-and-plate viscometer for 1-120 min showed a significant reduction
30 ess (0.1-2.75 dyn/cm(2)) in a cone-and-plate viscometer for 1-120 min was shown to increase, rather t
32 bility to readily integrate the microfluidic viscometer in other instrument platforms or modular micr
36 shear stress using a modified cone and plate viscometer, or cyclic elongational stretch using a compl
37 mechanotransduction measurements made in the viscometer over the range of conditions applied in typic
42 eloped a microfabricated nanoliter capillary viscometer that quickly, easily, and inexpensively measu
44 a self-calibrating microfabricated capillary viscometer to analyze non-Newtonian power law fluids.
45 nd then we apply this microfluidic diffusion viscometer to measure the viscosity of protein solutions
46 or, refractometer, and differential pressure viscometer) to characterize and compare the molecular pr
51 1) have been obtained on the microfabricated viscometer with the current geometry and channel dimensi
52 ne vesicles were sheared in a cone-and-plate viscometer, with the 42-kD protein band labeled by AAGTP
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