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The purpose of tracking is to let you specify a point based on the object snaps of existing objects. Temporary tracking lines are drawn from points you specify, and guide you so that you can easily specify the point that you want. Use the OTRACK button on the status bar to turn object snap tracking on and off. Object snap tracking can easily handle all of the following tasks and many more: You re drawing a line and have specified the start point. You want the endpoint to be exactly vertical to the endpoint of an existing line. You re drawing a circle inside a rectangle (which could be a hole inside a sheet-metal plate). You want the center of the circle to be exactly centered inside the rectangle, at the intersection of the midpoints of the rectangle s two sides. You want to start a line at the point where two existing lines would intersect if they were extended.

5 With phase-shifting techniques, a series of Fizeau or Twyman Green interferograms can be used without the introduction of tilt, even if closed loop fringes are formed A series of a minimum of three interferograms have to be taken with different values of the constant term for the phase, also called piston term Then, the interpretation of the wavefront evaluation becomes relatively simple from a mathematical point of view, but it is much more complicated from the experimental point of view The phase shifting techniques are described in detail in 14 When measuring an aspheric wavefront with phase shifting, the defocusing term has to be properly chosen so that the fringe spacing is minimum as described before As pointed out before, the limitation is that by using the optimum focus setting, the Nyquist condition is not violated 6.

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Start the SQLTool SQL commands processor: The SQLTool is a command-line interpreter that will interactively execute any SQL commands against the HSQLDB server that you started up in Step 1. The SQLTool uses the sqltool.rc file that you copied to your home directory in the previous step to obtain a connection to the database server. Open another console window and change the directory to wrox-pix-web. Start the SQLTool using the following command:

If the wavefront has a strong deviation from sphericity, even phase shifting techniques become impossible Another possibility under these conditions is to test the wavefront by dividing the complete aperture into small regions where the Nyquist condition is not violated In other words, in all small regions the fringe spacing should be larger than twice the pixel separation This technique, sometimes referred to as a wavefront stitching technique, will be described in this chapter 7 If a longer wavelength is used, the dynamic range is increased by reducing some of its sensitivity For example, by operating at 106 mm, the dynamic range is increased twenty times, approximately 8 Sources and detectors for longer wavelengths may be prohibitively expensive A solution to this problem may be found in two-wavelength methods, where fringes at longer (synthetic) wavelength are created by simultaneous exposure at two different wavelengths.

Return Loss (dB)

Figure 10.10 Simulation results for h = 0.1. Plot (b) shows the eigenvalues of I + hA. Both plots were obtained by applying the explicit form of the Euler method to the ODE system of Example 10.9. Clearly, the simulation is stable for h = 0.1.

These fringes, which are resolvable for high slopes at a longer wavelength, may be analyzed with a phase shifting method Different synthetic wavelengths can be obtained by combining different visible wavelengths, as described in 15 and Section 1213 in this chapter 9 Lateral or radial shear interferometry, as described in s 4 and 5, provides a larger dynamic range for testing strong aspherics, but a smaller sensitivity..

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