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The shutter priority setting on your digital camera was born for action photography To freeze action, you ll need to use a fairly fast shutter speed Luckily, this higher shutter speed works to your advantage by opening up the aperture and diminishing the depth of field; this focuses the viewer s attention specifically on your subject On the downside, of course, focusing is more critical since the depth of field is more shallow In general, I recommend that you use the fastest shutter speed available to capture action On the other hand, you can use a technique called panning to capture the subject in good, sharp focus and keep the background as a motion blur See Figure 3-16 for an example of panning that I used to freeze a child s wild ride at a Renaissance festival Panning is convenient both when you want to make a somewhat artistic statement about the subject s motion and when you know the camera can t muster up a fast enough shutter speed to freeze the motion the ordinary way Panning involves some effort on your part To create a good pan, you need to twist your body in sync with the motion of the subject as you press the shutter release Here s how: 1 Position yourself where you can twist your body to follow the motion of the moving subject without having the camera s line of sight blocked by something else 2 Set the camera s shutter speed for about 1/60 Feel free to experiment with this, but if you set the shutter speed too slow, you can t capture the subject effectively it blurs And if the shutter is too fast, you won t get the pretty blur in the background 3 Twist your body with the motion of the subject and track it through the camera s viewfinder or on the LCD display Press the shutter release and continue tracking.

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CHAPTER 11 Solution Thermodynamics: Theory (1188)

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These equations establish a thermodynamic foundation for the activity coefficient, which appeared in Sec 105 as a factor introduced into Raoult's law to account for liquid-phase nonidealities Comparison with Eq (1147) shows that Eq (1188) relates yi to GE exactly as Eq (1147) relates $i to For an ideal solution, GE = 0, m therefore yi = 1 d An alternative form of Eq (1186) follows by introduction of the activity coefficient through Eq (1188):

The generality of these equations precludes their direct practical application Rather, use is made of restricted forms, which are written by inspection:

Dim allFonts As New Drawing.Text.InstalledFontCollection( ) For Each oneFamily As Drawing.FontFamily In allFonts.Families ListBox1.Items.Add(oneFamily.Name) Next oneFamily

FIGURE 3-16

Equations (1189) through (1192) are analogs of Eqs (1152) through (1155) for residual properties Whereas the fundamental residual-property relation derives its usefulness from its direct relation to experimental P V T data and equations of state, the fundamental excessproperty relation is useful because V E , H ~and yi are all experimentally accessible Activity , coefficients are found from vaporniquid equilibrium data, and vE and H~ values come from mixing experiments, topics treated in the following chapter Equation (1192) demonstrates that In yi is a partial property with respect to GE/RT It is the analog of Eq (1 155), which shows the same relation of 1nJi to GR/RT The partialproperty analogs of Eqs (1190) and (1191) are:

These equations allow calculation of the effect of pressure and temperature on the activity coefficient

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The following forms of the summability and GibbsIDuhem equations result from the fact that In y is a partial property with respect to G ~ / R T : i

When I was in college, I took my geeky love of Star Trek, added a dose of photography, and came up with a hobby that could pretty much only be done around 3:00 AM Although it didn t help my grades very much, it was a lot of fun to create special effects like phaser blasts and disintegration halos The best part It was all done in the lens ; so you can try it yourself if your

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