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, Academic Press, New York, 1980 Hardy J W, J E Lefebvre, and C L Koliopoulos, Real-Time Atmospheric Compensation, JOSA, 67, 360 (1977) Hardy J W and A J McGovern, Shearing Interferometry: A Flexible Technique for Wavefront Measurement, Proc SPIE, 816, 180 (1987) Hariharan P, Optical Holography, Cambridge, London, 1984, p 232 Hariharan P, Quasi-Heterodyne Hologram Interferometry, Opt Eng 24, 632 (1985) Hariharan P, Phase-Stepping Interferometry: Effects of Multiple Re ected Beams, Appl Opt, 26, 2506 (1987) Hariharan P, Phase-Stepping Interferometry With Laser Diodes: Effects of Changes in Laser Power with Output Wavelength, Appl Opt, 28, 27 (1989a) Hariharan P, Phase-Stepping Interferometry With Laser Diodes 2: Effects of Laser Wavelength Modulation, Appl, 28, 1749 (1989b) Hariharan P, B F Oreb, and C H Freund, Stroboscopic Holographic Interferometry: Measurements of Vector Components of a Vibration, Appl Opt, 26, 3899 (1987a).

not your imagination. This only happens when you haven t chosen an Action. The head Action item stays in place once you choose an Action, even if you haven t added any settings. After you set up a head Action, you can copy it by copying its icon in the head, and then pasting it into the same head (to customize for a similar Action) or using it in another page. (See the Sharing Actions Between Pages or Sites sidebar earlier in the chapter.) Just remember that if you copy an OnCall head Action you need to give it a new name because the name is not carried to the new location. GoLive automatically gives it a code name because all OnCall Actions need names. But this code name won t be much help when you go to choose the Action from a setup menu; it really is a code.

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Hariharan P, B F Oreb, and T Eiju, Digital Phase-Shifting Interfeometry: A Simple ErrorCompensating Phase Calculation Algorithm, Appl Opt 26, 2504 (1987b)..

You can use array_unshift() to insert an element or elements at the start of an array. Just pass the array, followed by one or more elements to add. The function returns the new number of elements in the array. For example:

where the current in the nonlinear element is computed through the time domain ig (t) = imax tgh g V cos( 0 t + v ) imax Ig cos( 0 t + g ) = (1.121)

where T is the fractional transmission of light through the film T is equal to the intensity of the light transmitted through the film I divided by the intensity of the light before attenuation by the film I0 The OD of film base material is about 007 OD, and residual emulsion adds another 005 OD per emulsion layer The combination of base plus emulsion density is called the gross fog, and results in a baseline density of 012 to 020 OD Useful image densities in diagnostic radiology range from about 030 OD, which corresponds to transmission of 50% of the incident light, to about 20 OD, or 1% transmission of the incident light The relationship between OD and exposure is plotted as a curve, as shown in Figure 15-26, which is known as the characteristic curve for the film.

For most indoor applications, you will choose one of three different types of antennas: An omnidirectional antenna A directional antenna A highly directional antenna An omnidirectional antenna radiates transmissions out and receives transmissions in from all directions, although not equally in all directions. Most of the antennas in this category are thin rods or long flat sticks. The Hawking H-AI6SI shown in Figure 12-1 is a good example of an indoor omnidirectional antenna that offers from 2 to 6dBi of gain (4x). Meant for a 2.4 GHz b/g network, this vertically polarized antenna costs about $32. Hawking has a line of wireless antennas that can be added onto your devices, and this particular one comes with both an RP-SMA and an RPTPC connector.