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Base width

STM and AFM profiles distort the shape of a particle because the side of the tip rides up on the particle. This effect can be corrected for. Consider, say, a spherical gold particle on a smooth surface. The sphere may be truncated, that is, the center may be a distance q above the surface, where q < r, the radius of the sphere. Assume the tip to be a cone of cone angle a. The observed profile in the vertical plane containing the center of the sphere will be a rounded hump of base width 2d and height h. Calculate q and r for the case where a - 32° and d and h are 275 nm and 300 nm, respectively. Note Chapter XVI, Ref. 133a. Can you show how to obtain the relevent equation ... [Pg.742]

Urp Pi 1 — / If) where Wis the base width, is the distance between emitter and collector junctions and is the minority carrier diffusion length ia the... [Pg.351]

Therefore, the peak with a base width (w(j- -i)) of peak (r -1),... [Pg.204]

The curve in Figure IB is probably more useful from a practical point of view. Although the standard deviations of any dispersion process are not additive, they do give a better impression of the actual dispersion that a connecting tube alone can cause. It is clear that a tube 10 cm long and 0.012 cm I.D. can cause dispersion resulting in a peak with a standard deviation of 4 pi. Now, a peak with a standard deviation of 4 pi would have a base width of 16 pi and, in practice, many short... [Pg.298]

For an LC column operating at a flow rate of 1 ml/min., a peak with a base width of 4 seconds would represent a peak volume of about 67 pi. Consequently, the peaks... [Pg.311]

Consider the separation depicted in Figure 1. It is assumed that the pair of solutes represent the elution of the solute of interest and its nearest neighbor. Now, when the sample volume becomes extreme, the dispersion that results from column overload, to the first approximation, becomes equivalent to the sample volume itself as the sample volume now contributes to the elution of the solutes. Thus, from Figure 1, the peak separation in milliliters of mobile phase will be equivalent to the volume of sample plus half the sum of the base widths of the respective peaks. [Pg.421]

In TLC, plate efficiency is measured in a similar manner to that in GC and LC employing a similar expression. However, the retention distance from the sampling point to the position of the spot center is substituted for the retention volume, time or distance and the spot width as an alternative to the peak base width, viz.. [Pg.450]

The basie measure of the effieaey of a single-eolumn ehromatographie system in separating two neighbouring peaks ean be effeeted by the resolution (RJ, whieh is equal to the ratio between the two peak maxima. At, (distanee between the peak een-tres) and the average base width of the two peaks, as follows (3) ... [Pg.111]

The first clip should be attached at a point about one base width from the last seizing on the dead end of the rope and tightened securely. The saddle of the clip should rest upon the long or main rope and the U-bolt upon the dead end. All clips should be attached in this manner (see Figure 4-74). The short end of the rope should rest squarely upon the main portion. [Pg.596]

To determine the band dispersion that results from a significant, but moderate, sample volume overload the summation of variances can be used. However, when the sample volume becomes excessive, the band dispersion that results becomes equivalent to the sample volume itself. In figure 10, two solutes are depicted that are eluted from a column under conditions of no overload. If the dispersion from the excessive sample volume just allows the peaks to touch at the base, the peak separation in milliliters of mobile phase passed through the column will be equivalent to the sample volume (Vi) plus half the base width of both peaks. It is assumed in figure 10 that the efficiency of each peak is the same and in most cases this will be true. If there is some significant difference, an average value of the efficiencies of the two peaks can be taken. [Pg.119]

Because it is often difficult to measure the base width (W) accurately, it is probably better to use the peak width at half peak height, which is known to equal 2.355Gaussian distribution. Hence ... [Pg.108]

AED combined with GC x GC was first reported by van Stee et al. [21 ] for element-selective detection in petrochemical samples. The AED used in this study had a maximum data acquisition rate of 10 Hz, which when applied to the detection of GCxGC peaks of base width of 100-300 ms, will not achieve the required minimum of 5-10 data points per peak. In order to meet this criterion, peak widths need to be broader, with necessary widths of400-1- ms required. Deliberate broadening of second... [Pg.458]

FIGURE I A chromatogram showing retention time (t ), void time (Tg), peak at base width (Wb), and peak height (h). [Pg.22]

Figure 10. Calculated variation with cladding thickness of the birefringence in a SOI ridge waveguide, for different Si02 cladding film stress values. The model waveguide is formed in a 2.2 [j,m thick Si layer and has a typical trapezoidal wet etched ridge profile, with a base width of 3.8 pm, a top width of 1.1 pm, and an etch depth or 1.47 pm. Figure 10. Calculated variation with cladding thickness of the birefringence in a SOI ridge waveguide, for different Si02 cladding film stress values. The model waveguide is formed in a 2.2 [j,m thick Si layer and has a typical trapezoidal wet etched ridge profile, with a base width of 3.8 pm, a top width of 1.1 pm, and an etch depth or 1.47 pm.
Figure 11. Comparison of calculated and measured birefringence for different Si02 cladding thicknesses for a trapezoidal waveguide formed in a 2 im thick Si layer as shown in the inset. The ridge base width is 3.8 p,m, the top width is 1.1 pm, and the etch depth is 1.47 pm. Figure 11. Comparison of calculated and measured birefringence for different Si02 cladding thicknesses for a trapezoidal waveguide formed in a 2 im thick Si layer as shown in the inset. The ridge base width is 3.8 p,m, the top width is 1.1 pm, and the etch depth is 1.47 pm.
Efforts to model the deformation of EPP foam by FEA have been hampered by the lack of a sufficient range of data. Mills and Masso-Moreu (a.20) showed that simple pyramid methods, initially proposed by Stupak, are successful for the ribs on EPP mouldings. The ribs (Figure 13(a)) in the calculation taper from a base width of 100 mm to a top width in the range 15 to 70 mm, over a height H = 75 mm, with a length 75 mm. In the model the steps are to ... [Pg.21]

On a column 125 cm long, operated at 160° C, these retention times (in minutes) were obtained air peak, 0 90, heptane, 1 22 and octane, 1-43. The base widths of the bands were 0-16 for heptane and 0-22 for octane. The relative retention and the resolution for these bands are ... [Pg.164]

A high gain transistor requires a nearly equal to 1. In the absence of collector junction breakdown, a is the product of the base transport factor and emitter efficiency. The base transport factor, aT, is the fraction of the minority current (electrons for an n-p—n transistor) that reaches the collector. ocT 1 — W2 /2L, where W is the base width, is the distance between emitter and collector junctions and Lg is the minority carrier diffusion length in the base. High gain transistors require a thin base as well as a long minority carrier lifetime for a large Lg. Because aT is >0.995 in modem transistors, there is little room for improvement. The emitter efficiency, the fraction of emitter current due to minority carriers injected into the base instead of the emitter,... [Pg.351]

Equation 2.18 is an equation of a Gaussian curve. This curve is described by its maximum and width. We can represent the Gaussian curve in terms of Equation 2.18 as shown in Figure 2.5. The base width of the curve is 2(2Dt)"5. [Pg.50]

One may study zone broadening in gas chromatography by observing the shape of the elution peak which is Gaussian in ideal systems. The base width of the Gaussian curve is measured in standard deviation units, therefore... [Pg.51]

Under normal operation, the emitter-base junction is forward biased, whereas the collector-base junction is reverse biased (Figure 11). The voltage across the emitter-base junction is varied by an input signal. Because the donor concentration in the emitter is higher than the acceptor concentration in the emitter, the current through the junction is primarily due to electrons injected into the base. The base width is smaller than the mean... [Pg.32]


See other pages where Base width is mentioned: [Pg.1433]    [Pg.352]    [Pg.203]    [Pg.204]    [Pg.151]    [Pg.419]    [Pg.538]    [Pg.196]    [Pg.651]    [Pg.107]    [Pg.97]    [Pg.457]    [Pg.95]    [Pg.104]    [Pg.70]    [Pg.176]    [Pg.179]    [Pg.68]    [Pg.157]    [Pg.260]    [Pg.352]    [Pg.63]    [Pg.34]    [Pg.648]    [Pg.7]    [Pg.316]    [Pg.92]   
See also in sourсe #XX -- [ Pg.11 ]




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