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n Select the points of the dimensions you want to remove. If you see two possible edit points in line with each other that could be creating the dimension you want to remove, select both of them. n Right-click and choose Add. Use object snaps to add one or more points. n Right-click and choose Exit to continue with the command. 5. At the Specify dimension line position, or [Continuous/Staggered/ Baseline/ Ordinate/Radius/Diameter/datumPoint/Edit/seTtings] <Continuous>: prompt, right-click and choose an option if you want to change the type of dimension. 6. The prompt repeats. Pick a location for the new set of dimensions. 7. Press Enter to end the command and update the dimensions.

we denote the transformation of a function w E P 5 ( K )to K+. In Paragraph 4.1.4 we learned how to express the first partial derivatives 8w/dx,, j = 1,2, by means of the partial derivatives 8W/8[, the Jacobi matrix J K = DxK/DE. The rule (4.20) for the and transformation of gradients yields

8. To sort the data, select a column from the first drop-down list under Sort, and then select either Ascending or Descending from the second list. 9. You can see what results are returned for the recordset at any time by clicking Test.

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The ribbon has several states that you can choose from to balance between convenience and space. Click the button to the right of the Output tab to toggle between three states: n Full ribbon. Displays the current tab and all its buttons n Tabs. Displays one row of the tab names only n Panel titles. Displays the tab names and the panel names for the current tab To move the ribbon to the left or right of your screen in a vertical configuration, right-click any blank space on the tab bar at the top of the ribbon, and choose Undock. The ribbon undocks and then functions like a palette, which I cover later in this chapter. You can dock it on the left or right and auto-hide it. Right-click the gray, vertical title bar for more options.

The Wiener lter is an example of regularization. Regularization constrains inverse problems to keep noise from weakly sensed signal components from swamping data from more strongly sensed components. The Wiener lter speci cally damps noise from null regions of the system transfer function. In discrete form, Eqn. (8.17) is implemented by Toeplitz matricies. Hansen presents a recent review of deconvolution and regularization with Toeplitz matrices [112]. We consider regularization in more detail in the next section. 8.4 IMPLICIT CODING

If you have a compatible scanner attached to your PC, you can scan a picture directly into the Clip Organizer (which you learned about in 12), and from there import it into PowerPoint. You can also use the scanner s interface from outside of PowerPoint (and outside of the Clip Organizer).

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3. The conservation laws for momentum and energy can be used for the elastic collisions between particles and for the reflections of particles at the walls of the container. More precisely, it is possibleto fade out one aspect of the interaction between particles, namely, nonideal behavior of the gas; the effect of collisions on the temporal evolution of the gas, however, remains finite and is described by Boltzmann's kinetic e q ~ a t i o n . ~ Such a situation can be realized in the following limit. We assume d -+ 0 and N + 00 such that the effect of collisions between the particles of decreasing size remains important, which translates into Nd2 = constant (see Section 7.1.2). In this limit, we have N d 3 -+ 0, so that the volume fraction of the spherical particles in a container of fixed volume vanishes, and ideal gas behavior is thus approached. If one wants to keep the total mass constant, Nm = constant, then the mass density of the particles must diverge as l/d. This formal limit, which is useful for justifying the validity of Boltzmann's kinetic equation in a rigorous manner, is known as the Grad l m t In the ii. alternative limit Nd2 + 0, at least formally, collisions become unimportant. This limit is known as the Knudsen gas, that is, a gas of particles moving independently without any collisions, except at the walls of the container."

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