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in the limit of p r 1. The weight distribution (Eq. 2-131) is shown in Fig. 2-14 for several values of f . The extents of reaction have been adjusted to maintain a constant number-average degree of polymerization of 80 in all four cases. The size distribution becomes progressively narrower with increasing functionality of Af. This is also evident from Eq. 2-133, where X w =X n decreases from 2 for f 1 to 1.25 for f 4 (at p 1). Linear polymers are formed for f values of 1 or 2, while branched polymers are formed when f is greater than 2. The case of f 1 corresponds to the type 3 polymerization discussed in Sec. 2-6. The distribution is the exact same as the most probable distribution for linear polymerization (Sec. 2-7). Linear polymerization with f 2 is of interest in that the distribution is narrower than that for the usual linear polymerization. The linking of two statistically independent A type polymer chains into one B polymer molecule via an A molecule leads to a signi cantly narrower distribution that in A the usual polymerizations of the A or A plus B types. B A B

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FIGURE 7.14. Deviations of the ambient electrical (top graph) and magnetic (middle graph) elds. The ionospheric plasma content during magnetic storms is presented for short-term period of 3 minutes (denoted along the horizontal axis).

2-10

Polymerization of the A plus Af system (with f > 2) in the presence of B will lead not B B only to branching but also to a crosslinked polymer structure. Branches from one polymer molecule will be capable of reacting with those of another polymer molecule because of the presence of the B reactant. Crosslinking can be pictured as leading to structure XVII, in B

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Inserting a Single Barcode into Microsoft Excel . Switch to the Add-Ins tab. Open the TBarCode Panel . Position the mouse cursor in a cell. Select the barcode type (e.g. Code 128 ). Enter the barcode data or use the default data for the selected barcode . Adjust the size of the barcode (width, height, module width etc).

increases, an increase in the intensity uctuations is observed. Finally, for a given frequency, when phase uctuation becomes larger, the effect of the signal intensity uctuations becomes stronger. To verify the proposed approach of how to estimate effects of ionosphere on signal fading in land-satellite communication links regarding GPS applications, special numerical computations were performed to investigate the role of magnetic storms that usually occurred in the ionosphere due to solar activity, its in uence on the magnetosphere and changes to magnetosphere-ionosphere coupling, on ionospheric plasma perturbations [42,43] (see also literature referred therein). As was found experimentally, the plasma density due to a magnetic storm falls at 100% and higher. For example, in Figure 7.14 extracted from Reference [43], the changes of ambient electric eld (top graph), magnetic eld (middle graph), and ionospheric plasma content (bottom graph) are presented during magnetic storms registered by satellites in special measurements, described in Reference [42]. It is clearly seen that during the storm (the magnetic eld strength is maximum) the ionospheric plasma content was decreased signi cantly (more than twice). The decrease of plasma content leads to the creation of strong plasma irregulaties caused by the corresponding strong deviations of signal phase and amplitude, that is, the intensive signal scintillations at the receiver. As was mentioned above, this effect depends on radiated frequency.

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which two polymer chains have been joined together (crosslinked) by a branch. The branch joining the two chains is referred to as a crosslink. A crosslink can be formed whenever there

To show this effect we performed a numerical virtual experiment in the ionosphere above the USA territory The following results are measurements carried out in Reference [42] for low, mid, and high latitudes of the ionosphere, which we refer in our experiment as the south of the USA, mid latitude of the USA, and Alaska We compared for these three regions a random mean square (RMS) of signal intensity uctuations as a function of normalized mean density of ionospheric plasma (1012 m 3 , for the usually used frequencies of 10, 32, and 60 GHz, and for the spectral index of p corresponding to each case of the perturbed region Thus, for the perturbed south ionosphere of the USA it was taken from the ionospheric data equal p0 2, for the perturbed mid latitude ionosphere equal p0 3, and for the perturbed polar ionosphere above Alaska equal p0 4.

A BA BA A B A B Crosslink A B A B A B B A B A B A B A B A AB A A B A B B AB BA AB AB AB BA BA BA B A A B A B A AB AB AB AB AB AB BA BA A B B A B A B A

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are two branches (e.g., those indicated in XVII by the arrows) that have different functional groups at their ends, that is, one has an A group and the other a B group. Crosslinking will also occur in other polymerizations involving reactants with functionalities greater than two. These include the polymerizations

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