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All the values included in Table 9.4 are the average, x, and the standard deviation, n , of ve independent runs. Although it is commonly accepted that 30 independent runs should be performed at least, we were only able to run ve because of the very high complexity of such a large problem instance (2 612 TRXs) and the many different con gurations used. Let us start showing the performance of the two initialization methods. We present in Table 9.4 the AFP costs of the frequency plannings that result from both Random Init and Advanced Init. As expected, the latter reaches more accurate frequency assignments since it prevents the network from initially incurring in many interferences. For each con guration of the EAs, the AFP costs of these nal solutions are included in Table 9.5. If we analyze these results as a whole, it can be noticed that the con guration Rand&Rand-1 gets the lowest AFP cost on average, thus indicating that the computed frequency plannings achieve the smaller interference and therefore the better QoS for subscribers. Similar high quality frequency assignments are computed by the Rand&Interf-1, Rand&Interf-1, and Interf&Interf-3, where the cost values are around 20,000 units. We also want to remark two additional facts here. The rst one was already mentioned before and it lies in the huge reduction of the AFP costs that



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Over time a multifaceted approach has evolved, which starts with weight gain in an emotionally supportive setting and is then followed by more speci c psychotherapy when the patient has reached a weight at which she is able to make use of it (Russell, 1981) Furthermore, the patient s family and environment have come to be seen as supportive tools to be used in therapy, rather than necessarily as maintainers of the illness..





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This sets up an expectation and assumption that it is quite normal and expected that their serious problems may be eased a bit since they made the appointment. Rather than rigidly adhering to the format of immediately asking a direct question about any presession changes in the beginning of the first session, this question, like any useful question, should be asked in a timely fashion. 2. The formula first session task. This is the standard assignment given clients at the end of the first session. The task goes like this:

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the conductivity is complex, and it varies with the penetration depth and SC layer thickness (Ma and Wolff, 1996) The penetration depth changes with temperature, going to zero at Tc The real part of conductivity relates to the loss, and the imaginary part relates to the kinetic inductance Strong currents or strong magnetic elds will affect all parameters Sheen et al (1991) have formulated surface resistance, normal inductance, kinetic inductance, and current distribution for stripline, all as a function of penetration depth and lm thickness See also Ma and Wolff (1996) for formulations of complex conductivity and effective dielectric constant There was much interest in delay lines in the early 1990s Liang et al (1991) used YBCO on a lanthanum aluminum oxide substrate A re ection con guration with PIN diode switches was used, with 4 bits of phase produced.

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The change-back reaction predicts that whenever one person in a system changes, other people in the system will pressure that person to change back to the way she was prior to upsetting the equilibrium This is true even when changes are perceived as positive The change-back reaction does not emanate only from others The person who is changing often becomes anxious about the change and may change back even without pressure from others If these systemic reactions are predicted and planned for, women are less likely to capitulate to efforts to get them to return to their former way of being Another advantage of Bowen theory is the idea that, when conflict in a marital couple is high, conjoint therapy is often not helpful Bowen family systems therapy is often practiced with only one member of the family in the room.

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Each bit utilizes a 3 dB hybrid and 2 diodes; see Figure 319 The difference in line length between the switched and unswitched lines gives the phase bit Loss at 10 GHz was 11 dB, a value considerably less than that for copper phasers Because a 4-bit phaser provides up to 09375 of delay, the loss per wavelength was 12 dB However, most of this loss was due to substrate loss, diode loss, and mismatch loss Shen et al (1991) built a spiral delay line in coplanar line, using ThBaCaCuO on a LaAlO substrate Delay time was 11 ns, and the loss was 025 dB/ns at 8 GHz Liang et al (1993) worked spiral delay lines in YBCO; delays were 27 and 44 ns, with losses of 6 and 16 dB at 6 GHz These losses are 022 and 036 dB/ns, and 0.

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