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Channel flow 842 INDEX

Figure 12 under the counter-flow mode at 0.5 A/cm2. The index with the MPL is larger than that without the MPL for an index of 0-1 as depicted in Fig. 12. This result also shows that the MPL enhances water back-transport from the cathode side to the anode side. However, when the index is negative, meaning that the internal water circulation from the anode channel to the cathode channel, the index with the MPL is slightly higher than the index without the MPL. Therefore, the MPL at the cathode suppressed water vapor absorption at the anode, which is explainable by membrane hydration attributable to the MPL at the cathode. Consequently, the MPL promotes membrane hydration, leading less internal water circulation from the anode to the cathode side. Figure 12 under the counter-flow mode at 0.5 A/cm2. The index with the MPL is larger than that without the MPL for an index of 0-1 as depicted in Fig. 12. This result also shows that the MPL enhances water back-transport from the cathode side to the anode side. However, when the index is negative, meaning that the internal water circulation from the anode channel to the cathode channel, the index with the MPL is slightly higher than the index without the MPL. Therefore, the MPL at the cathode suppressed water vapor absorption at the anode, which is explainable by membrane hydration attributable to the MPL at the cathode. Consequently, the MPL promotes membrane hydration, leading less internal water circulation from the anode to the cathode side.
When plastics flow through straight tubes or channels they are sheared and the viscosity expresses their resistance. A method to measure melt flow is by the melt index (MI) [also called melt flow index (MFI)]. It is an inverse measure of viscosity. High MI implies low viscosity and low... [Pg.11]

Melt viscosity, or flow, is typically measured using extrusion plas-tometers (or melt indexers), capillary rheometers, and parallel plate rheometers. The extrusion plastometer measures the flow of a polymer melt under conditions specified by ASTM standard D 1238. This test yields a single, low-shear-rate value which is typically used to specify resins. Capillary rheometers determine viscosity over a range of shear rates in channel flow. While they are subject to error, these rheometers are still the only means of measuring viscosity at high shear rates (typically -y > 1000 s i). Parallel-plate rheometers also measure viscosity over a range of shear rates, but the maximum allowable shear rate is about 100 s i. [Pg.324]

These techniques are based on the discrimination between the dissolution and the surface film growth component of the working electrode current [56]. The following derivation makes used of the RRDE parameters indexed D (disk) and R (ring). The transposition to an upstream-downstream pair of electrodes in any kind of flow cell (e.g., channel flow double electrode, CEDE) is straightforward. [Pg.106]

The Haake ProFlow on-line rheometer, which was designed for measuring the melt viscosity and flow index, was side-mounted at the end of a single screw extruder with a diameter of 20 mm and the melt shear viscosity of each resin was measured online at 250°C. The values of the shear rates inside the channel of conventional screw element and in the barrier clearance of the fluted mixing element used in this work, whieh are approximated by the Couette shear rate, are calculated to be about 10 s and 100 s, respectively. The viscosity ratios of the dispersed phase to the continuous phase for used PP/PA6 blend at these two shear rates are about 2.6 and 4.2, respectively. [Pg.2912]

A polymer melt is injected into a circular section channel under constant pressure. What is the ratio of the maximum non-isothermal flow length to the isothermal flow length in the same time for (a) a Newtonian melt and (b) a power law melt with index, n = 0.3. [Pg.411]

Research has been done showing that rapid pressnre-driven LC analysis can be done with little solvent consumption, demonstrating this as a viable process analytical tool. Using electrokinetic nanoflow pumps LC can be miniaturized to the point of being a sensor system. Developments in terms of sampling to enable sampling directly from a process stream, to the separation channel on a chip are critical for the application of miniaturized process LC. The components (valves and pumps) required for hydrodynamic flow systems appear to be a current limitation to the fnll miniatnrization of LC separations. Detection systems have also evolved with electrochemical detection and refractive index detection systems providing increased sensitivity in miniaturized systems when compared to standard UV-vis detection or fluorescence, which may require precolumn derivatization. [Pg.535]

In-situ measurement technique of water vapor concentration in gas flow channels in PEMFCs using tunable diode laser absorption spectroscopy (TDLAS)31-36 is also shown with fundamental descriptions on its measuring principle and validity of a practical system. Localized current density and through-plane water-back transport index are obtained with variation of vapor concentration along the gas channel taken into account. Demonstrative results showing that effect of the micro porous layer (MPL) on variation of through-plane water-back transport index is shown in an operating PEMFC. [Pg.202]

M 21] [P 20] Mixing near a T-junction (channel 750 pm wide and 40 pm deep) is complete at a 0.17 pi min-1 flow rate when using a micro impeller at 120 rpm, as demonstrated by scanometric color index profiles providing line concentration profiles [32]. [Pg.65]

The components separated by FFF are washed out of the channel and into a detector and/or fraction collection device. The detectors are mainly those used in liquid chromatography where light absorption, refractive index changes, and so on, are measured as components flush through a small flow cell following their elution. [Pg.201]

The major modification required to adapt conventional detectors for use in LC is to design flow cells that have small volumes. We have already seen that volumes around 10 xL are required in most cases to prevent peak broadening. The geometry of the flow channel is also critical in achieving a maximum path length without undue sensitivity to flow oscillations, turbulent flow, or (in the case of UV) refractive index changes. [Pg.110]

As we have already mentioned in Section 2, in OCT the complementary quantities characterizing the average noise (conditional entropy of the channel output given input) and the information flow (mutual information in the channel output and input) in the diatomic communication system defined by the conditional AO probabilities of Eq. (48) provide the overall descriptors of the fragment bond covalency and ionicity, respectively. Both molecular and promolecular reference (input) probability distributions have been used in the past to determine the information index characterizing the displacement (ionicity) aspect of the system chemical bonds [9, 46-48]. [Pg.40]

Fig. 71 Calcite saturation index and amount of calcite precipitated per year for a discharge of 0.5 L/s in a 400m long karst channel with a flow velocity of 0.25 m/s assuming turbulent mixing (P(C02) = 0.03 Vol%). Fig. 71 Calcite saturation index and amount of calcite precipitated per year for a discharge of 0.5 L/s in a 400m long karst channel with a flow velocity of 0.25 m/s assuming turbulent mixing (P(C02) = 0.03 Vol%).
Inflow rate of flow into an equalization basin at time Mean rate of withdrawal from an equalization basin Time at index i of calculation Time at index f -1- 1 of calculation Top width of channel Top width at critical section Average velocity at cross section of conduit Average velocity at cross section at point 1 Average velocity at cross section at point 2, ) Accumulated volume inside equalization basin between time intervals t 1 and ti... [Pg.223]


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