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where V, is the total voltage across the accelerator gap (the sum of the screen and accel voltages): (5.2-9) and R is the ratio of the net beam voltage to the total voltage. Using Eq. (5.2-2) for the space-charge-limited current density and the electric field from Eq. (5.2-8), the maximum achievable thrust density is

Property outerHTML Nodes ELEMENT_NODE Returns for <p>Hello <i>world!</i></p> p.outerHTML would return: <p>Hello <i>world!</i></p> data TEXT_NODE COMMENT_NODE J. Lowery where the tag reads <p>J. Lowery</p> Returns the text string contained within a contiguous block of text or a comment Description Returns the HTML source or a tag, including the tag fcode

n Base point/second point method. At the Specify base point or [Displacement/mOde] <Displacement>: prompt, pick a base point. This can be anywhere in your drawing. At the

Each auxiliary module has type Filter. It must define two methods, i n i t and rewrite, which will be called to initialize the module and supply it with Styx messages

Using (P/V)large = (P/V)small , where (P/V)large and (P/V)small represent P/V at the large and small scales, respectively, results in P D3 , and substituting for P gives N3 D2 = constant, resulting in N D 2/3 (18-3)

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PHP is so efficient at passing data around because the developers made a very handy but (in theory) slightly sketchy design decision. PHP automatically, but invisibly, assigns the variables for you on the new page when you submit a data set using GET or POST. Most of PHP s competitors make you explicitly do this assignment yourself on each page; if you forget to do so or make a mistake, the information will not be available to the processing agent. PHP is faster, simpler, and mostly more goof-proof. But because of this automatic variable assignment, you need to always use a good NAME attribute for each INPUT. NAME attributes are not strictly necessary in HTML proper your form will render fine without them but the data will be of little use because the HTML form-field NAME attribute will be the variable name in the form handler. In other words, in this form:

The Pohlig Hellman Algorithm Calculation for the Factor pni i For 1 i k and m 0 to ni 2 1 do S1. Calculation of xi,m; write

11

Flash only supports the following Photoshop blending modes in editable form: Normal, Darken, Multiply, Lighten, Screen, Hard Light, Difference, and Overlay. If your selected import option results in Flash trying to preserve an unsupported blending mode in editable form, the blending mode is reset to Normal in the movie clip. However, if Flash is rasterizing your imported layer into a bitmap, the effects of even unsupported blending modes are retained in the bitmap.

(6.8-3)

For example, the family (ve, eL) transforms under the gauge group SU(2), x U(l)g. The simplest assumption is that this constitutes a weak SU(2) doublet, so t = f and t3 = Using Qv= 0 and Qe = -1, eq. (9.2), and requiring that yv = ye gives the first two lines of Table 9.1. As another example, the right-handed fermions do not enter the charged-current weak interactions so eR must be an SU(2), singlet: t = t 3 = 0. Then from (9.2), y = -2 for Q = -1.

(i) HomogeneousSystems for UnderstandingLocal Fluid Theories A major simplification arises from the fact that we expect the building blocks for our complex fluid to be of a local nature The essence of a local theory can be explained best in terms of an example, such as the model of a complex fluid with a tensor and a scalar as configurational variables According to (434) and (435), the energy and entropy are space integrals of energy and entropy densities, where these densities at the position T depend only on the independent variables at the position T Being interested in these generators, we can thus limit ourselves to situations where only the variables at a given point are relevant or, in other words, we may consider a homogeneous system without any loss of generality.

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