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xmlnamespaces ( 'http://www.w3.org/2001/XMLSchema-instance' as xsi ,'http://schemas.milambda.net/Music' as m ,'http://schemas.milambda.net/Music-Album' as ma ) distinct Discography.Person.query (' data(@m:firstName) ').value ( '.' ,'nvarchar(150)' ) as FirstName

As the frequency is raised without limit, the set of plates starts to act more and more like a short circuit When the frequency is low, there is a small charging current, but this quickly drops to zero as the plates become fully charged As the frequency becomes high, the current flows for more and more of every cycle before dropping off; the charging time remains constant while the period of the charging/discharging wave is getting shorter Eventually, if you keep on increasing the frequency, the period of the wave will be much shorter than the charging/discharging time, and current will flow in and out of the plates in just about the same way as it would flow if the plates were shorted out The opposition that the set of plates offers to ac is the capacitive reactance It is measured in ohms, just like inductive reactance, and just like resistance But it is, by convention, assigned negative values rather than positive ones Capacitive reactance, denoted X C , can vary, just as resistance and inductive reactance do, from near zero (when the plates are huge and close together, and/or the frequency is very high) to a few negative ohms, to many negative kilohms or megohms Capacitive reactance, like inductive reactance, varies with frequency But X C gets larger (negatively) as the frequency goes down This is the opposite of what happens with inductive reactance, which gets larger (positively) as the frequency goes up Often, capacitive reactance is talked about in terms of its absolute value, with the minus sign removed Then we say that the absolute value of X C increases as the frequency goes down, or that the absolute value of X C is decreases as the frequency goes up

Use the File | Open Dictionary command from AppleScript Editor This is the normal and more formal way You ll probably want to use this way most of the time Drag the application s icon and drop it on the AppleScript Editor icon This way works well when the AppleScript Editor icon appears on the Dock (as it does when AppleScript Editor is open) and you ve got a Finder window open to the Applications folder

,Discography.Person.query (' data(@m:middleName) ').value ( '.' ,'nvarchar(150)' ) as MiddleName ,Discography.Person.query (' data(@m:lastName) ').value ( '.' ,'nvarchar(150)' ) as LastName from @xml.nodes (' /ma:discography/ma:album/ma:track/ma:author ') Discography (Person)

To open the dictionary file for TextEdit, follow these steps:

xmlnamespaces ( 'http://www.w3.org/2001/XMLSchema-instance' as xsi ,'http://schemas.milambda.net/Music' as m ,'http://schemas.milambda.net/Music-Album' as ma ) distinct Discography.Band.query (' data(@ma:bandName) ').value ( '.' ,'nvarchar(450)' ) as [Name] from @xml.nodes (' /ma:discography/ma:album/ma:track/ma:band ') Discography (Band)

In one sense, capacitive reactance behaves like a reflection of inductive reactance But looked at another way, X C is an extension of XL into negative values If the frequency of an ac source (in hertz) is given as f, and the capacitance (in farads) is given as C, then the capacitive reactance in ohms, X C, is calculated as follows: X C = 1/(2 f C ) Again, we meet our friend ! And again, for most practical purposes, we can take 2 to be equal to 628 Thus, the preceding formula can be expressed like this: XC = 1/(628f C ) This same formula applies if the frequency, f, is in megahertz and the capacitance, C, is in microfarads Capacitive reactance varies inversely with the frequency This means that the function X C versus f appears as a curve when graphed, and this curve blows up as the frequency gets close to zero Capacitive reactance also varies inversely with the actual value of capacitance, given a fixed frequency Therefore, the function of X C versus C also appears as a curve that blows up as the capacitance approaches zero The negative of X C is inversely proportional to frequency, and also to capacitance Relative graphs of these functions are shown in Fig 14-4