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t o show that F,V = x(qv + 2q,) and xF; = xq,. (b) Evaluate Fzn/Fzep using (10.19a,b), neglecting strange quarks. The upper limit follows from assuming d d >> u u; the lower limit from assuming d d << u G.

Figure 4-17: This example shows data points plotted on top of a map (from Wikimapia). The challenge in doing this is aligning the latitudes and longitudes so the points are properly placed.

cssStyles.setStyle( .emphasized , {fontWeight: bold , textDecoration: underline }); ;

function inspectBehavior(msgStr){ var argArray,layerMenu,layersArray,menuLength,found; argArray = extractArgs(msgStr); layerMenu = findObject( LAYER_LIST ); //Get all layers references including parent frames layersArray = getAllObjectRefs( NS 4.0 , LAYER ); menuLength = layerMenu.options.length; //Loop through all the <select> options for(var i=0;i<menuLength;i++){ //If the layer reference is same as the argument, got the layer if(getNameFromRef(layersArray[i]) == argArray[1]){ layerMenu.selectedIndex = i; //Set the flag and stop looping found = true; break; } } //If the layer is not found, alert! if(!found){ alert(argArray[1] + could not be found ) } //Populate the rest of the UI with remaining arguments if(argArray[2]){ findObject( Z-INDEX ).value = argArray[2]; } }

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The electron current collected by the anode is the flux that diffuses through the magnetic field times the Boltzman factor at the sheath: (44-3) where A,, is again the anode surface area exposed to the plasma discharge The actual current distributions and potential distribution in a Kaufman thruster are the same as for the DC discharge thruster shown in Fig 4-9 However, there are several terms that were analyzed for ring-cusp thrusters that can be neglected in Kaufman thrusters First, if the axial magnetic field in the discharge chamber is on the order of 100 G, then the Larmor radius for, say, 20-eV primaries is 15 mm Since the magnetic field lines do not intersect the anode and primaries are too energetic to participate in the collective instabilities that drive Bohm diffusion, the primary electrons must make collisions in order to cross the magnetic field to be lost.

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private function onLoad():void { if (str == value1 ) { Alert.show( value1 ); } else if (str == value2 ) { Alert.show( value2 ); } else if (str == yes ) { Alert.show( something else ); } }

FIGURE 27.25 Three closed paths (shapes) with the five Pathfinder options applied to them. From left to right: the two original paths and the same paths after applying after applying Add, Subtract, Intersect, Exclude Overlap, and Minus Back options.

For example, a text Find and Replace operation that searches for FW using the Whole Word option, and replaces it with Fireworks is defined with code like this:

The nature of the interrupt request is similar to that of a single-access port discussed in Section 16.3.2. After the request is accepted, it must be cleared so that the same request will not be processed multiple times. The flag FF discussed in Section 7.2.4 can be used for this purpose.

Same Blending Mode (Select Same Blending Mode) selects objects that have the same Blending mode attributes of the currently selected object. The objects are selected regardless of their other attributes as long as the Blending modes are the same.

5.10

MOD (a, k, n) d : 1; aa : a; while (k . 0) do begin if (1 (k mod 2)) then d : (d a) mod n; k : (k 2 (k mod 2)) div 2; aa : (aa aa) mod n; end;

10. Expand the package in the Package Explorer in Flash Builder to examine the project s files (see Figure 25.5).

onClipEvent(load){ _root.isLoading = true; trace( isLoading s type = + typeof(_root.isLoading)); } onClipEvent(enterFrame){ if(this._framesLoaded >= this._totalFrames){ _root.isLoading = false; } }

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