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Eight gain passes through the zigzag slab ampli er can be achieved using passive polarization switching in the regenerative ampli er ring The fact that the SBS cell provides interstage gain isolation makes this possible since, if it were replaced with a mirror, the small signal gain through eight consecutive gain passes would result in possible parasitic oscillation from the small re ective losses of AR-coated optical surfaces in the ring or in the output beam When the Pockels cell is located inside the regenerative ampli er ring, the length of the laser pulse to be ampli ed is limited to the transit time inside the ring minus the high-voltage switching time for the Pockels cell Now, with passive polarization switching, this time limit is increased to be the transit time for four ring revolutions.

In mammals, WAT occurs throughout the body in discrete depots, which are homologous among all species but show considerable variation in size and functional importance (Pond, 1992; Pond, 1999). This dispersed distribution has frustrated many attempts to classify fat depots according to anatomical location or physiological function (Shen et al., 2003), and improved understanding of the molecular biology of WAT has now rendered some previous classi cations obsolete. Total body fat, comprising the sum of all depots, is usually subdivided into subcutaneous and internal adipose tissue (Shen et al., 2003) (Table 4.1). Subcutaneous fat constitutes the layer between the dermis and the outer surface

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Longer pulses can be ampli ed, and the relative timing accuracy requirement between the injected pulse and the Pockels cell voltage pulse is greatly reduced In fact, the replacement of the Pockels cell with a full-aperture Faraday isolator has been shown to allow the ampli cation of laser pulses of over 500 ns in duration [32], as will be described in a following section of this chapter Another advantage is that the SBS phase conjugator very effectively conjugates the rst-order aberration of tilt The combination of this tilt correction and relay imaging greatly reduces the sensitivity of the system performance to small changes of optical alignment in the ring No change in output power or pointing direction during operation is observed for large mirror misalignments in the ring, limited only to those angular excursions that result in vignetting of the beams at the edges of the ampli er slab 5.

325 Single-frequency oscillator The 1053-nm transition in Nd:YLF closely matches the uorescence curve peak in the Nd-doped phosphate glass used in this ampli er system It is desirable to have a single-frequency oscillator input pulse both for generating reproducible smooth temporal input pro les without modulation from multilongitudinal modes and for achieving the best wavefront reversal delity in the SBS phase conjugator [33, 34] Although single longitudinal mode output from an Nd:YLF Q-switched oscillator has been demonstrated by injection locking to a low-power single-frequency master oscillator, this technique requires careful mode matching between the master and slave oscillators and active cavity length stabilization of the Q-switched slave oscillator [35] A simpler method of achieving single-frequency output was chosen for this application by using a variation of the electronic linewidth narrowing technique [36, 37] In this method,.

TABLE 8.1. Ionization Potentials (IP), Proton A nities (PA), pK b Values, and BF3 A nities Molecule Water, H2 O Methanol, CH3 OH Dimethyl ether, CH3 OCH3 Tetrahydrofuran, (CH2 )4 O Oxetane, (CH2 )3 O Formaldehyde, CH2 O Acetaldehyde, CH3 C(O)H Acetone, CH3 C(O)CH3 Acrolein, CH2 CHC(O)H Butenone, CH2 CHC(O)CH3 (E )-methylacrolein, CH3 CH CHC(O)H Dimethylacrolein, (CH3 )2 C CHC(O)H Methyl acetate, CH3 C(O)OCH3 Methyl acrylate, CH2 CHC(O)OCH3 IPa (eV) 12.6 11.0 9.9 9.4 9.7 10.9 10.2 9.7 10.1 10.5 PAb (kJ/mol) 707 766 798 825 832 704 770 769 814 835 835 859 822 835 pKb c 15.74 16 17.5 18 24 21 20.5 20 BF3 a nityb (kJ/mol) 46 65 71 85 82 26 50 44 58 58 60 66 58 53

The research undertaken at The University of Nottingham has demonstrated that currently available CFD software can be used to model ventilation flows within the end region of an electric motor. The modelling gave air flow predictions to within 20 per cent and heat transfer predictions to within 30 per cent of measurement. And valuable insights into the phenomena taking place were gained. The confidence gained from this research has prompted the use of CFD in the design office at ALSTOM Electrical Machines Limited the prospect is for CFD to become a tool that is integrated into the design process.

are scalars. Since soLis scalar and C-' is symmetric,