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In addition to Process Version, another important starting point for establishing the best possible default rendering for your photos is to apply a camera profile using the Camera Calibration panel (see Figure 4 8). Note: camera profiles can only be applied to camera raw and dng imag es. Other file types will show Embedded , though you can still tweak slider adjustments here (but I don t recommend it.) With the current camera profiles installed, Lightroom will show only the profiles Figure 4-8 applicable for the camera used to make the capture. If your camera is not listed, you can use the default Adobe profiles or create your own. In some cases, you may see several versions of Adobe Camera Raw (ACR) profiles. The numbers indicate during what version(s) of Adobe Camera Raw the original matrix-style profile was created for that camera model. If there is more than one listed, this indicates the profile for that camera was updated in the newer version of ACR. The newer Adobe Standard profile replaces the older ACR profiles. (For camera models released after ACR 5.2, the profile menu will not list the ACR profiles.) In addition to the Adobe profiles, depending on your camera make and model, you will also very likely see camera-specific profiles listed. These mimic the picture styles in the camera and the camera-maker s dedicated software. Some images benefit from differ ent profiles Try each of the various profiles until you get the best results. Choosing a different profile can dramatically improve the baseline rendering of your captures! Installing/uninstalling camera profiles At the time of this writing, Adobe s camera profiles are automatically installed when you install Lightroom (version 2.2 and higher), dng C onverter (v5.2 and higher) or Adobe Camera Raw (v5.2 and higher). If you installed earlier

Here s an example that uses nm to show some of the symbols in /usr/lib/libdl.a:

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Sets up user environment information for every user. It is executed when you first log in. This file provides values for your path, as well as setting environment variables for such things as the location of your mailbox and the size of your history files. Finally, /etc/profile gathers shell settings from configuration files in the /etc/profile.d directory. Executes for every user who runs the bash shell, each time a bash shell is opened. It sets the default prompt and may add one or more aliases. Values in this file can be overridden by information in each user s ~/.bashrc file. Used by each user to enter information that is specific to his or her own use of the shell. It is executed only once, when the user logs in. By default it sets a few environment variables and executes the user s .bashrc file. Contains the information that is specific to your bash shells. It is read when you log in and also each time you open a new bash shell. This is the best location to add environment variables and aliases so that your shell picks them up. Executes each time you log out (exit the last bash shell). By default, it simply clears your screen.

$ sed s/test/trial/g data4 This is a trial of the trial script. This is the second trial of the trial script. $

var1=10 var2=-57 var3=testing var4="still more testing"

Figure 4.33 illustrates the PSPS and bifurcation behavior of a simple batch reactive distillation process. Qualitatively, the surface of potential singular points is shaped in the form of a hyperbola due to the boiling sequence of the involved components. Along the left-hand part of the PSPS, the stable node branch and the saddle point branch 1 coming from the water vertex, meet each other at the kinetic tangent pinch point x = (0.0246, 0.7462) at the critical Damk hler number Da = 0.414. The righthand part of the PSPS is the saddle point branch 2, which runs from pure THF to the binary azeotrope between THF and water. Figure 4.34 shows the PSPS for the reactive membrane separation process with application of a Knudsen-membrane. In comparison with reactive distillation, the membrane turns the vertical hyperbola into a horizontal hyperbola. In particular, the membrane shifts the stable node branch towards the THF-vertex such that THF-rich products can be attained in the considered Knudsen-membrane reactor. Because the boiling temperature of 1,4-BD is much higher than of the two reaction products and the reaction is irreversible, the bifurcation behavior is only affected by the mass transfer coefficient ratio water/ THF, if BD is not extremely high or low. There exists a critical value of water/ THF = 2.1, above which the stable node branch approaches the THF-vertex.

Since the maximum instantaneous SINR at the combiner output is still given by 1 the relation in (11.2), where Rni is now the inverse of (11.51), then once again the eigenvalue decomposition of Rni yields the result in (11.5), where now there exist L NI nonrandom eigenvalues NI +1 , NI +2 , . . . , L , each with value 2 and NI random eigenvalues 1 , 2 , . . . , NI . Although we still obtain a product form for the MGF of the combiner output SINR, namely M (s) = M (s)

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