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The trace() function is global to Flash Player; that is, it s always available without your having to reference or import an ActionScript class. The purpose of the trace() function is to send a text message to a logging target. In its simplest form, trace is called with a String value:
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There s a Feed Validator for checking the validity and quality of your feeds, so why not a program to test out how your feeds are getting served up Check out Unpolluted, a tool written in Python to do just that, at this URL:
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Drag gwen s mouth open onto the Stage and use the Align Panel to center the symbol. It s time to place our eyes and mouth onto GWEN! s face. Return to the main stage by choosing Edit Edit Movie (Ctrl+E or Command+E). Create two new layers, and name them eyes and mouth. Drag the newly created Movie Clip symbols, eyes and mouth, out of the Library onto GWEN! s face, as shown in the following figure. Make sure you select their respective layer before dragging each onto the Stage. At this point, you have a functional animated girl. If you test your movie now, you ll see that GWEN! s eyes blink, and her mouth opens for her yawn, but we still have to add the interactivity that lets the mouth tell the eyes when to shut and reopen. To do that, we first have to name the instance of the eyes Movie Clip you created and dragged onto the Stage so that the mouth Movie Clip instance can identify it. Then we have to add the Tell Target actions that control the eyes instance. Hang on GWEN!, we re almost there! Select the eyes Movie Clip on Stage, and then open the Instance Panel by choosing Modify Instance (Ctrl+I or Command+I). In the Instance Panel, you see a text field next to Name (see the following figure). That text field is where we give our Movie Clip instance a unique identification. Instance names are something like serial numbers they enable actions in the movie to address a specific copy of a Movie Clip. Type her-eyes in the Name text field, and then press Enter or Return.
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In InDesign (as with most programs), you can select only contiguous text. So if you have, for example, several subheads to which you want to apply local character formatting, you can t select them all and apply the formatting in one fell swoop. You have to do each text segment separately. (That s one reason to use character styles instead of local formatting.) n
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Table 4-10: Some Demographic Information about Zip Codes with and without Purchases with More Than 1000 Households HAS ORDER MEASURE Number of Zip Codes Average Number of Households Average Median Income Households on Public Assistance Population with College Degree Owner Occupied Households NO 6,244 3,168.7 $35,815 4.9% 13.1% 72.5% YES 9,947 8,182.1 $48,660 3.4% 27.8% 63.8%
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The result MUST be a valid query component with the original query part and the post elds combined. An HTTP GET operation is performed on the resulting URI. application/x-wwwform-urlencoded The eld names and values are escaped using URI-escaping and assembled into an application/x-www-form-urlencoded media type. When a wml:post eld element is used to name a eld, and the value of the wml:post eld s value attribute references the control variable for a multiple-selection control, the eld value MUST be submitted as speci ed in [HTML4], where one name/value pair is included for each item in the list. For example, for a eld named x with value $(x) , where x is the control variable with value choice1; choice3 , the submitted data will be x=choice1& x=choice3 . The submission data is appended to the query component of the URI. The result MUST be a valid query component with the original query part and the post elds combined. An HTTP GET operation is performed on the resulting URI. multipart/form-data Error. The user agent MUST ignore the wml:go element. post application/vnd.wap.wml.form.urlencoded The eld names and values are escaped using URI-escaping and assembled into an application/x-www-form -urlencoded media type. When a wml:post eld element is used to name a eld, and the value of the wml:post eld s value attribute references the control variable for a multiple-selection control, the eld value MUST be submitted as a semicolon-separated list of values. For example, for a eld named x with value $(x) , where x is the control variable with value choice1; choice3 , the submitted data will be x=choice1; choice3 . The submission data is sent as the body of the HTTP POST request. The Content-Type header MUST include the charset parameter to indicate the character encoding. application/x-wwwform-urlencoded The eld names and values are escaped using URI-escaping and assembled into an application/x-www-form-urlencoded media type. When a wml:post eld element is used to name a eld, and the value of the wml:post eld s value attribute references the control variable for a multiple-selection control, the eld value MUST be submitted as speci ed in [HTML4], where one name/value pair is included for each item in the list. For example, for a eld named x with value $(x) , where x is the control variable with value choice1;choice3 , the submitted data will be x=choice1&x=choice3 . The submission data is sent as the body of the HTTP POST request. The Content-Type header MUST include the charset parameter to indicate the character encoding when the part contains characters not in the US-ASCII character set. multipart/form-data The eld names and values are encoded as a multipart/formdata media type as de ned in [RFC2388].
for (var j=0; j<curImagemap.numCoords; j++) { if (j>0) WRITE_HTML( , ); WRITE_HTML(curImagemap.xCoord(j), , , curImagemap.yCoord(j)); }
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The deconfining phase transition of pure gauge fields may be ascribed to a color screening that converts the gluonic matter into a chromoplasma (814.3). At a qualitative level this picture should survive the introduction of dynamical fermions ( 13.1.10), but questions arise as t o the sharpness of the transition and to the choice of an appropriate order parameter to distinguish phases in the presence of dynamical quarks. This is not surprising, given the previous analogies with condensed matter systems: dynamical fermions contribute terms to the functional integral that are mathematically similar t o external fields for spin systems, and it is known that external fields smooth phase transitions in the latter case (Svetitsky, 1986). As we have just noted, in pure glue S U ( N ) theories the deconfining transition is characterized by a spontaneously broken global center Z N of the group S U ( N ) . When ZN is unbroken the expectation value ( L ) of the WilsonPolyakov loop (14.41) is zero, and the spontaneous breaking of this symmetry yields a finite value of ( L ) in the deconfined region (see Fig. 14.8). However, the global Z N symmetry is broken ezplzcitly by fermion mass terms. As a result, in the presence of dynamical fermions the expectation value of the Wilson-Polyakov loop fails to vanish for the confinement region, so it no longer constitutes an order parameter for the deconfinement transition. The physical reason for this was discussed in 514.3: dynamical quarks allow the creation of colorless hadrons through qij excitations,
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