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Dead zero signal

Figure 4.20.A shows a more recent cell reported by Cobben et al. It consists of three Perspex blocks, of which two (A) are identical and the third (B) different. Part A is a Perspex block (1) furnished with two pairs of resilient hooks (3) for electrical contact. With the aid of a spring, the hooks press at the surface of the sensor contact pads (4), the back side of which rests on the Perspex siuface, so the sensor gate is positioned in the centre of the block, which is marked by an engraved cross as in the above-described wall-jet cell. Part B is a prismatic Perspex block (2) (85 x 24 x 10 mm ) into which a Z-shaped flow channel of 0.5 mm diameter is drilled. Each of the wedges of the Z reaches the outside of the block. The Z-shaped flow-cell thus built has a zero dead volume. As a result, the solution volume held between the two CHEMFETs is very small (3 pL). The cell is sealed by gently pushing block A to B with a lever. The inherent plasticity of the PVC membrane ensures water-tight closure of the cell. The closeness between the two electrodes enables differential measurements with no interference from the liquid junction potential. The differential signal provided by a potassium-selective and a sodium-selective CHEMFET exhibits a Nemstian behaviour and is selective towards potassium in the presence of a (fixed) excess concentration of sodium. The combined use of a highly lead-selective CHEMFET and a potassium-selective CHEMFET in this type of cell also provides excellent results. Figure 4.20.A shows a more recent cell reported by Cobben et al. It consists of three Perspex blocks, of which two (A) are identical and the third (B) different. Part A is a Perspex block (1) furnished with two pairs of resilient hooks (3) for electrical contact. With the aid of a spring, the hooks press at the surface of the sensor contact pads (4), the back side of which rests on the Perspex siuface, so the sensor gate is positioned in the centre of the block, which is marked by an engraved cross as in the above-described wall-jet cell. Part B is a prismatic Perspex block (2) (85 x 24 x 10 mm ) into which a Z-shaped flow channel of 0.5 mm diameter is drilled. Each of the wedges of the Z reaches the outside of the block. The Z-shaped flow-cell thus built has a zero dead volume. As a result, the solution volume held between the two CHEMFETs is very small (3 pL). The cell is sealed by gently pushing block A to B with a lever. The inherent plasticity of the PVC membrane ensures water-tight closure of the cell. The closeness between the two electrodes enables differential measurements with no interference from the liquid junction potential. The differential signal provided by a potassium-selective and a sodium-selective CHEMFET exhibits a Nemstian behaviour and is selective towards potassium in the presence of a (fixed) excess concentration of sodium. The combined use of a highly lead-selective CHEMFET and a potassium-selective CHEMFET in this type of cell also provides excellent results.
Adjust the receiver s dead time (the time between the end of the pulse and the beginning of acquisition of the signal) to minimize pulse breakthrough, which is manifested by a baseline roll. Certain spectrometers carry out this operation in the following way. First, a spectrum is recorded and phased as usual. Then, a software command calculates the dead time such that the first-order (left) phase control equals zero in a repeated spectrum. [Pg.57]

To determine the model parameters, a minimum of three injection experiments with tracers plus one for each solute have to be carried out. The evaluation of these experiments is sketched in Fig. 6.11, together with the symbols of the measured first moments. The injected signal for all experiments is represented by a rectangular pulse. The first tracer experiment detects the dead time of the plant while the column is replaced by a zero volume connector. The other experiments are carried out with the column in place, using a tracer that cannot get into the pores (Tracerl) and... [Pg.257]

There are two important results from this analysis. First, the rate constants for binding and dissociation can be obtained from the slope and intercept, resp>ec-tively, of a plot of the observed rate versus concentration. In practice this is possible when the rate of dissociation is comparable to ki [S] under conditions that allow measurement of the reaction. At the lower end, resolution of i is limited by the concentration of substrate required to maintain pseudo-first-order kinetics with substrate in excess of enzyme and by the sensitivity of the method, which dictates the concentration of enzyme necessary to observe a signal. Under most circumstances, it may be difficult to resolve a dissociation rate less than 1 sec by extrapolation of the measured rate to zero concentration. Of course, the actual error must be determined by proper regression analysis in fitting the data, and these estimates serve only to illustrate the magnitude of the problem. In the upper extreme, dissociation rates in excess of 200 sec make it difficult to observe any reaction. At a substrate concentration required to observe half of the full amplitude, where [S] = it., the reaction would proceed toward equilibrium at a rate of 400 sec. Thus, depending upon the dead time of the apparatus, much of the reaction may be over before it can be observed at the concentrations required to saturate the enzyme with substrate. [Pg.18]

If Tg is very short, it is difficult to see the signal because the FID will decay before the instrumental dead time is over. This situation will usually occur only for solids, and one way to deal with it is to try to form an echo which occurs later than the end of the dead time. Such echoes are fairly easy to form in the presence of a large inhomogeneous broadening such as in metals and with many quadrupolar nuclei in NQR. You will need a high speed digitizer because the echoes will be very sharp. For some other solid state echoes, see IV.B.3. and IV.B.4. Another possible solution is to use the zero time resolution method described in VI.D.4. [Pg.139]

A different method of loss-free counting has been implemented in the zero dead time method (ZDT) of a commercial digital signal processor. The ZDT correction is dynamically calculated by the processor to produce both the corrected data spectrum and the channel-by-channel variance spectrum. Upp et al. (2001) have shown that this digital method allows correct estimates of the uncertainty. [Pg.1603]

It is apparent then that we need to measure SFC independently in order to find the proportionality constants. This is naturally done using NMR. Typical benchtop instruments operate at 20MHz, and the free induction decay (FID) times for solids are in the order of 10 ps for Hydrogen in the crystalline fraction, and over 200 ms for the liquid. The estimate of the signals at time zero is done by extrapolation of the signals at later times, due to the dead time of the probe. [Pg.91]

In both tests, the NO2 outlet trace exhibited first a dead time, then it slowly grew and eventually approached the feed concentration level. Also, immediate evolution of N2 and NO was recorded at both temperatures upon NO2 feed, then the signals of the same species slowly decreased with time, evenmally approaching zero. Figures 9.7a, b clearly point out however that the increase of catalyst temperature from 120 to 200 °C over the Cu-zeolite resulted in an incremented NO formation and a corresponding decreased N2 evolution a higher temperature thus favors the reduction of nitrites by ammonia, reaction (9.7), against the oxidation of nitrites to nitrates, reaction (9.2), in line with what reported for Fe-zeolites. [Pg.258]


See other pages where Dead zero signal is mentioned: [Pg.698]    [Pg.698]    [Pg.309]    [Pg.131]    [Pg.169]    [Pg.199]    [Pg.35]    [Pg.125]    [Pg.302]    [Pg.566]    [Pg.478]    [Pg.134]    [Pg.215]    [Pg.116]    [Pg.865]    [Pg.267]    [Pg.524]    [Pg.444]    [Pg.1574]    [Pg.277]    [Pg.563]    [Pg.406]    [Pg.65]    [Pg.709]    [Pg.202]    [Pg.328]    [Pg.469]    [Pg.368]    [Pg.268]   
See also in sourсe #XX -- [ Pg.587 ]




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