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Pools in Tg S, Fluxes in Tg S y 1, Tg = 1012 g; (turnover times) Marine 3.2 (10d) COS (5 10 y) Seasalt particles 140 y 1 Biogenic 15 30 y 1 Deposition 231 y 1

More detailed information obtained by tracking the evolution of an arbitrary material line in a ow can be described by the stretching of a small vector attached to any particle in the ow: dl = ( v)T l dt lt=0 = l0 (3-7)

public c l a s s CentMutex extends P r o c e s s implements Lock { // a s s u m e s t h a t P-0 c o o r d z n a t e s a n d d o e s n o t r e q u e s t l o c k s . boolean haveToken ; f i n a l int l e a d e r = 0; I m t L i n k e d L i s t pending$ = new I n t L i n k e d L i s t ( ) ; public CentMutex( Linker initComm) { super (initComm ) ; haveToken = (myId == l e a d e r ) ; } public synchronized void r e q u e s t C S ( ) { sendMsg ( l e a d e r , r e q u e s t ) ; while ( ! have l oken) myWait ( ) ;

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When you test the movie, it ought to display two buttons with default labels of start and pause. Click on the start button, and it will start the playback of the sound, and the button will toggle to the stop state. While the sound is playing you can pause it. With the sound paused you can resume the sound.

Not only can layers be positioned, but, like any HTML element, they can be set to be either visible or invisible. Obviously, an invisible layer isn t much use because nobody can see it. The trick is to make it visible at some point to achieve a particular effect. You can make a layer invisible by including the attribute style= visibility: hidden . See more details in 18.

You can use several different photo file formats with iPhoto. These are the three file formats for which iPhoto provides full support: G J PEG . A file format developed by the Joint Photographic Experts Group, JPEG is the most widely used format for digital photos. JPEG typically uses lossy

convective ow have been altogether neglected The classic approach of drawing a black box around the reactor and examining only the intrinsic kinetics of the reactive process is only meaningful when macroscopic inhomogeneities can no longer be detected This method treats the intrinsic kinetics properly but can only give insight for processes with slow reactions It is bound to fail when reactions occur faster than the time scale for homogenization in the system In such cases we run the risk of overestimating the selectivity and conversion during the design process (a typical problem during reactor scale-up) but completely ignore that a well-mixed homogeneous state may never be reached during the entire life of the process (recall Figure 3-6) Chaotic ows are the only effective route to destroy segregation rapidly in viscous mixing applications, which are particularly prone to remaining inhomogeneous for long times (Lamberto et al.

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1. Draw a circle with the Ellipse tool. Remember to keep Shift pressed so you end up with a perfect circle. 2. Click the Convert Anchor Point tool. 3. Click each of the anchor points and then release. This converts the smooth anchor points to corner anchor points. The rhombus (diamond shape) should look like the illustration in Figure 6.26.

In this case, the number of digits is a small number between 0 and 4, because TOTALPRICE is never negative and always under $10,000. The following expression turns the number of digits into a lower and upper bounds, assuming that the underlying value is never negative:

2. Placement (rt, lt, middle)

Single Photon Emission Computed Tomography (SPECT)

function createLib(num){ for(i=1;i<=num;i++){

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