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Before glucose I-phosphate can enter glycolysis, it must first be converted into glucose 6-phosphate in the reversible reaction catalyzed by phosphoglucomutase: glucosel-phosphate & glucose 6-phosphate UDP- 1-glucose is also an intermediate in the pathways that synthesize glycogen and many different glycoconjugates. Indeed, it is for these reasons that lactose is an ideal dietary sugar for infants, who relative to adults, are more dependent on hepatic glycogen stores. Since UDP-1-glucose is in the direct pathway for the synthesis of glycogen, dietary galactose is converted directly into hepatic glycogen. In contrast, fructose derived from dietary sucrose must first be metabolized to triose phosphates, which are glycolytic intermediates. In the fed state, when dietary glucose stimulates insulin secretion, hepatic gluconeogenesis is suppressed and glycolytic intermediates are oxidized to pyruvate as opposed to being used to synthesize glycogen. Humans can also synthesize UDP-1-galactose from glucose when the diet does not contain lactose or any other source of galactose. Since both the uridyltransferase and epimerase reactions are reversible, the pathway shown in Figure 4-7 can run in either direction. Synthesis of UDP- 1-galactose is particularly important in the lactating mammary gland, which uses galactosyl transferase to synthesize lactose: UDP-1-galactose

--------------------Frame5-------------------SIP: - Session Initiation Protocol SIP: SIP: R SIP/2.0 Response Status Code=l80(Informational) ResponsePhrase=Ringing SIP: Via = SIP/2.0/UDP 192.168.1.1lO;branch=c45115398e3b9314d91685a56ec22dce53 1ecb88f58~3ad59dbb84~3~3 le9, SIP/%.O/UDP 192.168.1.74:58440 SIP: From = 14083465118 <sip: 14083465118@ 192.168.1.74>

Returns: String. Description: Method obtains the name of the Active Directory site that contains the local computer.

In this example, the current/working directory is /usr/bin. To find out the name of your home directory, type the echo command, followed by the $HOME variable:

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This is a demonstration database of 25 of the coolest combo and list box techniques. Full documentation is included in the CD directory. The database comes from a highly acclaimed paper given by Cary Prague at the Microsoft Access conferences.

Outlook s To-Do Bar can be useful for working with Calendar items. To display the To-Do Bar, select To-Do Bar from the View menu and then select Normal. The To-Do Bar is shown in Figure 11.6.

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Occasionally, you want to know where your mouse is on the screen. You can use two methods to find your mouse location. Your choice of methods depends on the version of OS X you are coding against. Prior to the Java 1.5 release for OS X, finding the mouse location on the screen was handled with the com.apple.eawt.Application class. The method getMouseLocationOnScreen() was called. The getMouseLocationOnScreen() returns an AWT Point object containing the mouse pointer s hot spot on the monitor. Since the release of Java 1.5, Apple deprecated the getMouseLocationOnScreen() method. On newer version of OS X, use a combination of the MouseInfo getPointerInfo() method and the PointerInfo s getLocation() method. The result is the same. The getLocation() method returns an AWT Point object.

sample arrangement. it is of utmost importance to take into account and make proper use of the optical properties of the sample: the absorption, the elastic and inelastic scattering. These are represented by: 0 the linear Napierian absorption coefficient (L, 0 the linear Napierian scattering coefficient r, 0 the linear Napierian Raman scattering coefficient s. These coefficients have the dimension of reciprocal length (Mills, 19XK), in this context, cm '. Kubelka and Munk (1931) described the optical properties of pigments by employing the parameters (r and r. The Kubelka-Munk theory is the basis of diffuse reflection spectroscopy (Sec. 6.4). We have extended the Kubelka-Munk approach in order to describe the Raman scattering of crystal powders (Schrader and Bergmann, 1967). The results can also be applied to liquids and transparent solids. The procedure is as follows: The radiation balance of a layer with the thickness d having an 'infinitely large' surface, irradiated homogeneously from one side with exciting radiation, is given by the solution of four coupled linear first-order differential equations (Eqs. 3.5-1 ...4). This is a boundary value problem, with the definitions given in Fig. 3 . 5 2 . We are discussing

The details of the scintillation process are complicated and depend very much on the molecular structure of the scintillator In organic crystals, the molecules of the organic solid are excited from their ground states to their electronic excited states (see Fig 1818) The decay of these states by the emission of photons occurs in about 1028 s ( uorescence) Some of the initial energy absorbed by the molecule is dissipated as lattice vibrations before or after the decay by photon emission As a result, the crystal will generally transmit its own uorescent radiation without absorption There are three common types of organic scintillator The rst type is a pure crystalline material, such as anthracene The second type, the liquid scintillator, is the solution of an organic scintillator in an organic liquid, such as a solution of p-terphenyl in toluene (%3 g solute/L solution).

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