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1. Use ab18-09.dwg if you have it open from the previous exercise. Otherwise, open it from the Results folder of the DVD. 2. Save the drawing as ab18-10.dwg in your AutoCAD Bible folder. 3. Type attdia . If it s currently set to 0, type 1 . 4. Choose Home tab Block panel Insert. Choose ARMCHAIR from the Name drop-down list. Verify that the Specify On-screen option is checked only for Insertion Point, and click OK. 5. Pick a point in front of the desk (turn off Object Snap if necessary) to insert the armchair and open the Edit Attributes dialog box. The values that were entered when the attributes were defined are displayed, but you can change them. 6. The default values exist because most of the furniture was purchased at one time when the office was opened. However, let s assume that this chair was purchased later. Change the purchase date to 3/05. Click OK. Because the attributes are invisible, you see only the chair, but the values do exist in the drawing database. 7. Save the drawing.

advantage of the multiplex grating approach is that the input eld of view will be comparable to conventional instruments, allowing convenient use of coded apertures or slits Unfortunately, the multiplex grating hologram of Fig 939(a) does not achieve this objective because the recording eld is Bragg-matched to both gratings along the input wavevector The shorter wavelength eld is nearly Bragg-matched to both gratings, but at a shifted input angle If the input eld scattered by all of the grating orders, then one must increase the output eld of view to capture all of the grating orders, and the system resolving power is simply determined by the largest value of K In the alternative recording geometry of Fig 939(b), independent gratings are recorded at two different wavelengths In this case both recording wavelengths are Bragg-matched at the same input and output angles.

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We also illustrate the Bragg matching condition on the outer wave normal surface of the grating K1 recorded on the inner wave normal surface and the Bragg matching condition on the inner wave normal surface for the grating K2 recorded on the outer surface The shift in the Bragg condition can be used in combination with an angularly ltered input aperture to ensure that a spectral band centered on k1 scatters from K1 while a spectral band centered on k2 scatters from K2 from the same input aperture into the same output aperture To use multiplex volume gratings in a diffractive spectrometer, one decreases D1 and increases L to increase the angular selectivity of the hologram In a conventional design, one seeks low angular selectivity to achieve reasonable etendue In a multiplex design, one maintains etendue by adding grating components Figure 9.

40 shows the increased angular selectivity for a lower-index-modulation hologram Figure 940(a) is a density plot of the data shown in Fig 915, showing the angular selectivity of a high-modulation, thin hologram Figure 940(b) shows the decreased angular range of thicker and lower-modulation hologram Figure 941 shows the diffraction ef ciency as a function of angular and wavelength detuning.

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