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1 e flow properties of the exposed oil using a viscometer.
2 s of the same samples obtained with a U-tube viscometer.
3 d fluid shear stress applied in a cone-plate viscometer.
4 to pathological shear stress in a cone-plate viscometer.
5 ell-defined shear conditions in a cone-plate viscometer.
6 he effects of nonlinear flow in a cone-plate viscometer.
7 ticle forces and attachment times within the viscometer.
8 plied to cells via a modified cone and plate viscometer.
9 ls of fluid shear stress in a cone-and-plate viscometer.
10 luid samples was measured using an Ubbelohde viscometer.
11 ter, and shear stress using a cone-and-plate viscometer.
12 for the shear PV measured using conventional viscometers.
13 Through the combined use of a microfluidic viscometer, a smartphone camera for image capture, and a
17 man neutrophils were sheared in a cone-plate viscometer and the kinetics of aggregate formation was m
19 d transfectants were sheared in a cone-plate viscometer, and formation of heterotypic aggregates was
20 ed to increasing shear rates in a cone-plate viscometer, and levels of intact and cleaved GPVI were e
21 nal variations in adhesion efficiency in the viscometer, and that the overall efficiency is dependent
22 , purified VWF was subjected to shear in the viscometer, and VWF morphology was assessed using light
24 osity data collected previously using a CTOF viscometer, as well as with literature values obtained w
27 was compared with a vacuum-driven capillary viscometer at high shear rates (>500 s(-1)), at which th
28 ells (E3-ICAM) in suspension in a cone-plate viscometer at shear rates typical of venular blood flow
29 w-chamber-based platelet adhesion assays and viscometer-based shear-induced platelet aggregation and
32 imple droplet-based, water-in-oil continuous viscometer capable of measuring viscosity changes in 10
33 ameters; these components make the nanoliter viscometer completely self-calibrating, robust, and easy
34 we report measurements with a time-of-flight viscometer down to [Formula: see text] and up to [Formul
35 To address this challenge, a microfluidic viscometer driven by surface tension was developed to re
36 ial refractive index (dRI), and differential viscometer (dVis)) that is coupled to an ultraviolet (UV
38 ress (0.1-4.0 dyn/cm(2)) in a cone-and-plate viscometer for 1-120 min showed a significant reduction
39 ess (0.1-2.75 dyn/cm(2)) in a cone-and-plate viscometer for 1-120 min was shown to increase, rather t
40 a portable single-use analytical chip-based viscometer for determining the viscosity of protein solu
42 bility to readily integrate the microfluidic viscometer in other instrument platforms or modular micr
46 teers were exposed to high shear stress in a viscometer or microfluidics channel to mimic mechanical
47 shear stress using a modified cone and plate viscometer, or cyclic elongational stretch using a compl
48 mechanotransduction measurements made in the viscometer over the range of conditions applied in typic
53 eloped a microfabricated nanoliter capillary viscometer that quickly, easily, and inexpensively measu
54 rement and single-use characteristics of the viscometer, thus showing great promise in developability
56 a self-calibrating microfabricated capillary viscometer to analyze non-Newtonian power law fluids.
57 nd then we apply this microfluidic diffusion viscometer to measure the viscosity of protein solutions
58 or, refractometer, and differential pressure viscometer) to characterize and compare the molecular pr
64 1) have been obtained on the microfabricated viscometer with the current geometry and channel dimensi
65 ne vesicles were sheared in a cone-and-plate viscometer, with the 42-kD protein band labeled by AAGTP