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The rack rows were laid out, along with hot and cold aisles. Only cold aisles had perforated tiles. The equipment had front-to-back cooling, and each rack front faced a cold aisle.

Undo: To restore an image to the way it looked before the last operation, choose Edit Undo (Ctrl+Z). You can undo the effect of a paint or edit tool, a change made to a selection outline, or a special-effect or color-correction command. You can t undo disk operations, such as opening or saving. Photoshop does enable you to undo an edit after printing an image, though. You can test an effect, print the image, and then undo the effect if you think it looks awful. Revert: Choose File Revert (or press the F12 key) to reload an image from disk. This is generally the last-resort function, the command you choose after everything else has failed.

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Spatial Frequency ( c/mm)

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superimposing at the output port the converted contributions from the various ports, their original correlation must be accounted for, and they do not simply add in power. In case other noise-generating mechanisms are present in the device, they can simply be superimposed, provided the generating mechanisms are uncorrelated; otherwise, they must be included in the formulation [31]. This fundamentally nonlinear internal noise correlation is such that the noise properties of a mixer cannot be represented by a simple resistive model; in particular, noise level is increased with respect to a statically biased semiconductor device. Given the formulation above, prediction of correct noise levels are easily obtained once the large-signal local oscillator is known, and the conversion matrix is computed. Obviously, the physical mechanisms at the origin of the noise, which determine the correlation properties of the internal noise at the mixer ports, must be known. This is by no means a trivial problem; however, many noise sources are known well enough for effective noise prediction within nonlinear analysis methods such as, for example, harmonic balance.

At the very bottom of the screen is the status bar (refer to Figure 1-2). At the left are the X,Y coordinates. As you move your mouse, these coordinates change. (If they don t change, click them and move your mouse again.) The status bar also contains several buttons that I explain later in this book.

>>> Code=StringIO.StringIO( str = hi there ) >>> tokenize.tokenize(Code.readline) 1,0-1,3: NAME str 1,3-1,4: OP = 1,4-1,14: STRING hi there 2,0-2,0: ENDMARKER

hemispherical lens as illustrated in Figure 5.11. Using this principle and the basic cyclic con guration, Murty designed the interferometers shown in Figures 5.12 and 5.13. The hemispherical cavity in the second interferometer may be emptied or lled with oil, in order to obtain the desired radial shear. Some very unconventional radial shear interferometers with discontinuous stepping wave-fronts have been described by Bryngdahl (1970, 1971).

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plotted as seen down the C3 axis Molecular orbital 5 has the C3 axis in the plane of the paper Notice that MOs 1 and 2 resemble atomic 1s and 2s orbitals, respectively, and that the other occupied MOs [3, 4, and 5 (HOMO)] resemble 2 p orbitals The degenerate pair together describes the threefold symmetry of the molecule The nodal surfaces are at right angles in the two MOs (3 and 4) The orientation of the node itself is arbitrary As it happens, the nodal plane of MO 4 as displayed in Figure 26 (fortuitously) coincides with the plane containing one of the NH bonds The HOMO would be described as the lone pair on N, but it is a true MO.

12 A

The function exp(x) returns e to the power of x, while log(x) returns the natural logarithm of x. The function log10(x) returns the base-10 logarithm of x. The function pow(x,y) returns x raised to the power of y. Note that 5**-1 (an integer to a negative power) is illegal, but math.pow(5,-1) is legal (and equals 0.2, as you would expect). math.pow(-5,0.5) is still illegal for that, you need to use the cmath module. (See Computing with Complex Numbers later in this chapter.) The function ldexp(x,y) (short for load exponent ) returns x * (2**y). The function frexp(x) returns the mantissa and exponent of x a tuple (a,b) such that x == a * (2**b). The exponent, b, is an integer. The mantissa, a, is such that 0.5<=a<1, unless x is 0, in which case, frexp(x)==(0.0,0).

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