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A difference between the Controller_impl class we show in Section 10112 and this example is that we use an STL set, and not a map, as the m_assets data member This is because the Active Object Map of our POA stores the Thermometer_impl * servant pointers, so we have no need to keep a separate map that duplicates that storage Instead, m_assets stores only asset numbers The list implementation iterates over the set of asset numbers For each asset number, we must create an object reference for the device it represents To do this, we first convert the asset number to a string using an ostrstream, and then we convert the resulting string to an ObjectId using the string_to_ObjectId helper function supplied in the PortableServer namespace (this is a stand-alone function that converts strings to ObjectIds) In addition to the ObjectId, we need the repository ID for the most derived interface our new object will support To determine the correct repository ID, we use the asset number to read the model type directly from the device using the ICP_get device access function If the model type indicates that the device is a thermometer, we make the repos_id variable point to he repository ID for the Thermometer interface; otherwise, we make it point to the ID for the Thermostat interface We pass the oid and the repos_id arguments to create_reference_with_id to create the object reference for the device Because the return value of create_reference_with_id is a reference of type CORBA::Object, though, we narrow it to the CCS::Thermometer type before we assign it to our return sequence After we finish iterating over the m_assets set, we return the sequence of Thermometer references This implementation of list certainly works as desired Moreover, the fact that we do not need to create any servants to return object references for all our devices clearly illustrates that the life cycle of a CORBA object is completely independent of the life cycle of any servant used to incarnate it However, our list implementation contains a few assumptions that have some interesting side effects These side effects are related to the interface types of the objects and to the eventual activation of the objects.

UPC-A is the most common form of UPC codes that consists of 12 digits to encode goods sold t point-of-sale in North America.mdb", which defines all above three columns in Customer table, also define one extra column named "Barcode", with data ype "xs:base64Binary".). NET project with "Crystal Reports Application" as template. ame the project as "CrystalReportsBarcode".Related: Barcode Generating Crystal ASP.NET , VB.NET Barcode Generating , Barcode Generating .NET how to

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component, and that the recorded values were wholly interstellar, McLean (1976) pursued such an analysis more thoroughly A distance was determined as 114 kpc, thus providing an absolute magnitude at maximum brightness of 10m 1, a value consistent with its temporal photometric behaviour Zellner & Morrison (1971) reported polarimetric colour measurements of the very slow outburst of Nova HR Delphini 1967, and also for Nova Vulpeculae No 1 1968 and Nova Serpentis 1970 For HR Del 1967, after making correction for its interstellar component, p was 06% in the red during the rst 120 days following the outburst In the later phases, the intrinsic component was generally small and irregularly variable The same authors also found variations in p of 1% for Nova Serpentis 1970, but no variations for Nova Vulpeculae No 1 1968 According to Zellner (1971), Mie theory suggests that the polarization of HR Del 1967 can be explained by scattering from grains of iron or graphite within an asymmetric circumstellar cloud, and de nitely not pure silicate Such non-volatile matter may be the condensation of material ejected at the outburst, or may be the debris remaining from a previous outburst event Zellner (1971) also commented on the infrared excesses seen in Novae Ser 1970 and Aquilae 1970, attributing them to thermal radiation from grains in the dust shell Noting that the strong infrared uxes did not appear during Epoch I for Nova Del, nor for Nova Ser, during the early stages when the variable polarization was seen, Zellner suggested two distinct generations of circumstellar grains It is perhaps possible that the high ejection velocities of the fast novae prevent the formation of small grains, at least in the initial stages, or the lack of intrinsic polarization may simply indicate no source dust in the system Zellner proposed that the small grains responsible for the production of the polarization are precursors of condensation nuclei for the accretion of much larger particles of radius 1 m For future fast novae, it is important to combine polarimetry with infrared photometry to follow the suggested grain developments Pirrola & Korhonen (1979) made observations of Nova Cygni 1978 and noted an increase in polarization from 16% to 19% over a period of a week The change correlated with infrared observations promotes a notion of there being a dust forming stage Combined with photometry which revealed short-term ickering in Nova Cygni 1978, Blitzstein, Bradstreet, Hrivnak, et al (1980) also reported on polarimetric measurements made in the early phase of the outburst, prior to the time of dust formation After consideration of the interstellar component, a residual intrinsic polarization of 023% was deduced, attributable to non-spherical scattering of H emission A rough estimate of the distance was obtained by considering the interstellar component Variable, and hence ntrinsic polarization, was observed by Eggen, Mathewson & Serkowski (1967) for Nova Pyxidis in the very early stages of its outburst in 1966 1967 Little comment was made except that the lack of signi cant changes in the H line suggest that the polarization was generated in the outer shell of the nova Kemp & Rudy (1976) observed Nova Cygni 1975 over a wide range of wavelengths, including narrow-band studies of the H emission No structure in p ( ),.

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