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Moreover, Q = A H for mechanically reversible, constant-pressure, closed-system processes [Eq (223)] and for the transfer of heat in steady-flow exchangers where A E p and A EK are negligible and W, = 0 In either case,

FIGURE 12-3

Public Sub ReprocessSecuritySet( ) ' ----- Reload in the security set for the current ' user. If no user is logged in, clear all settings. Dim counter As Integer Dim sqlText As String Dim dbInfo As SqlClient.SqlDataReader = Nothing

Evaluation of the integral in Eq (43) requires knowledge of the temperature dependence of the heat capacity This is usually given by an empirical equation; the two simplest expressions of practical value are:

where a , B, and y and a , b, and c are constants characteristic of the particular substance With the exception of the last term, these equations are of the same form We therefore combine them to provide a single expression:

Using those programs, all you need to do is drag and drop the individual images in the proper order (see Figure 12-3) The software matches the edges all by itself, and does a good job even with low-quality digital cameras, wide-angle lenses, and other technical difficulties

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where either C or D is zero, depending on the substance considered Since the ratio CpIR is dimensionless, the units of C p are governed by the choice of R As shown in Chap 6, for gases it is the ideal-gas heat capacity, rather than the actual heat capacity, that is used in the evaluation of such thermodynamic properties as the enthalpy The reason is that thermodynamic-property evaluation is most conveniently accomplished in two steps: first, calculation of values for a hypothetical ideal-gas state wherein ideal-gas heat capacities are used; second, correction of the ideal-gas-state values to the real-gas values A real gas becomes ideal in the limit as P + 0; if it were to remain ideal when compressed to finite pressures, its state would remain that of an ideal gas Gases in their ideal-gas states have properties that reflect their individuality just as do real gases Ideal-gas heat capacities (designated by C: and are therefore different for different gases; although functions of temperature, they are independent of pressure Ideal-gas heat capacities increase smoothly with increasing temperature toward an upper limit, which is reached when all translational, rotational, and vibrational modes of molecular motion are fully excited [see Eq (1618)] The influence of temperatureon C for argon, nitrogen, water, and carbon dioxide is illustrated in Fig 41 Temperature dependence is expressed

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' ----- Clear out the existing items. For counter = 1 To MaxLibrarySecurity SecurityProfile(counter) = False Next counter ' ----- Exit if there is no user logged in. If (LoggedInUserID = -1) Or _ (LoggedInGroupID = -1) Then Return Try ' ----- Load in the security elements for this user. sqlText = "SELECT ActivityID FROM GroupActivity " & _ "WHERE GroupID = " & LoggedInGroupID dbInfo = CreateReader(sqlText) Do While (dbInfo.Read) SecurityProfile(CInt(dbInfo!ActivityID)) = True Loop dbInfo.Close( ) Catch ex As Exception ' ----- Some database-related error. GeneralError("ReprocessSecuritySet", ex) If (dbInfo IsNot Nothing) Then dbInfo.Close( ) ' ----- Un-log in the administrator through recursion. LoggedInUserID = -1 LoggedInGroupID = -1 ReprocessSecuritySet( ) Finally dbInfo = Nothing End Try End Sub

Not all panoramas are photographed just to take wide, scenic landscapes Sometimes, you might want to photograph a subject in sections so you can get more pixels for a high-res print What am I talking about Consider a situation in which you want to make a 20 30-inch poster-sized print, but your 2-megapixel camera doesn t have remotely enough resolution to make a large picture You can still get the shot, as long as you re trying to photograph a stationary object Shoot it in sections then stitch the individual segments together on the PC

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analytically by equations such as Eq (44), here written:

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