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So a spring with mass can be represented by a combination of an ideal spring with the same spring constant and an equivalent mass of one-third of the spring mass attached to the moving end of the spring. Similar techniques can be used to obtain equivalent masses for other distributed masses for which the rigid body assumption is not a good approximation. Such systems are better analyzed using other techniques, however (Ungar, 1985), so this is not detailed here.
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The first thing you must do is to give your router a unique hostname. Second, you must list the remote hostnames and passwords these remote hosts will use when authenticating to your router. This is accomplished with the username command. Please note that the password you configure on this side must match the password on the remote side (it s case-sensitive). On your router s WAN interface, you need to enable PPP with the encapsulation ppp command. Then you can specify PAP authentication with the ppp authentication pap command. The preceding client and server code listings perform a one-way authentication the client authenticates to the server and not vice versa. If you want to perform two-way authentication, where each side must authenticate to the other side, configure both devices as PAP servers and clients. 25.04.The CD contains a multimedia demonstration of configuring PPP authentication using PAP on a router.
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You pride yourself on being a very honest and forthright person, and you act as if you like this person immensely, but this is the opposite of what you actually feel. What is your behavior covering up that you need to examine
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Set to 01 for a challenge, 02 for the reply to a challenge, 03 for allowing the PPP connection, and 04 for denying the connection A local sequence number assigned by the challenger to distinguish among multiple authentication processes The random value used in the MD5 hash function The name of the challenging router (the server), which is used by the source to find the appropriate password to use for authentication
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Instead, the more uni ed UDF structure was applied to all types of DVD discs and this le system is suitable for all forms of content and any type of le format designed for storage on optical disc. It is also designed to be adaptable to all the major computer operating systems. To maintain backwards compatibility with earlier computers and operating systems that are not designed to read UDF, the UDF Bridge le system was designed. UDF Bridge is a hybrid system that includes support for discs recorded using the original ISO-9660 le system that originated with CD-ROMs. UDF Bridge also provides full support for discs containing les structured under UDF, as well. UDF Bridge maintains an important optical disc convention that has been followed ever since the Yellow Book CD-ROM format was introduced as a means of extending the compact disc to include computer data, as well as audio data. Computer-based playback devices and decoders, as much as possible, have been designed to read all earlier formats. CD-ROM drives were designed to read audio CDs. DVD-ROM drives, from the beginning, were equipped to be able to manage CD-ROM playback. The UDF Bridge format makes it possible to produce DVDs for older PCs running operating systems that do not yet have UDF support. In comparison, playback devices targeted for the entertainment industry and consumer use, such as audio CD players and DVD playback equipment, usually only accommodate a single format. The Enhanced CD format was designed as a hybrid format containing both audio and computer data. This allows CD players to play the audio present on the compact disc, while the computer data les could only be read if the disc were inserted in a PC CD-ROM drive. Similarly, DVD-Video discs often contain content designed for the PC, which is essentially ignored by the DVD playback equipment. The additional data only becomes available if you insert the disc in a DVD-ROM drive.
In primary active transport, the transport protein couples a reaction hydrolyzing ATP with moving the ion or molecule across the membrane. Recall from Chap. 7 that hydrolysis of ATP (adenosine triphosphate) involves cleaving one of the phosphate groups from ATP to form ADP (adenosine diphosphate). When the pyrophosphate bond is cleaved, a large amount of energy is released. This energy can be used by any process that is coupled to the reaction cleaving the phosphate bond. The coupling of a process to a reaction that involves hydrolysis of ATP is typically done by an enzyme classified as an ATPase, and the coupling is usually carried out by some conformational change in the enzyme. In the case of primary active transport, it is the transport protein itself that couples the hydrolysis with transporting a molecule or ion across the membrane. The mechanism of active transport involves a conformational change in the transport protein. The conformational change is needed to push the molecule (or ion) through the hydrophobic bilayer or to move the molecule (or ion) against a concentration gradient. In primary active transport, without the hydrolysis of ATP the conformational change is otherwise not favorable. The enthalpy from the hydrolysis of ATP tips the Gibbs energy change in favor the conformational change that pushes the molecule across the membrane.
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By de ning the Hamiltonian, H, of Eq. (13.42) and using the state Eq. (13.46), a two-point boundary-value problem can be obtained as follows: State equation: x2 - r0 x1 - r1 x2 + r0 x3 H x4 ( x, p,t ) = x= x5 p 2 r0 r1 x + ( r1 - r0 ) x - r0 r1 x + r0 x - p5 2 K 1 Kk Kk 3 Kk 4 2W2 Kk2 k Costate equation: NF rr 2 2 -2W1 Ffe r0 + 2W3 Ffe N F - 2W3 Ffe N F + p2 r0 - p5 0 1 x1 Kk 2 -2W r F - p + p r - p r1 - r0 1 1 fe 1 2 1 5 Kk H NF rr 2 2 ( x, p,t ) = 2W1r0 Ffe - 2W3 Kk Ffe N F - 2W3 Ffe N F p= - p3r0 + p5 0 1 x Kk x3 NF r0 2 -2W3 Ffe N F x - p3 - p5 K k 4 - 2W F 2 N N F - p -2W1 Kk Ffe 3 fe F 4 x5 Boundary Conditions: use Eq. (13.47). 13.5.8.2 Solution of the Two-Point Boundary-Value Problem. The two-point boundary-value problem given by Eqs. (13.48) and (13.49) cannot be integrated directly. A trial initial value for the costate vector, p(0)(0), is chosen and the system of Eq. (13.48) and (13.49) are integrated forward in time. In general, however, the nal state, x(0)(1) will not coincide with the boundary condition x(1) speci ed by Eq. (13.47). It is necessary, therefore, to develop a new and hopefully improved estimate of p(0)(0) based on the
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// Demonstrate the :: qualifier. using System; using Counter; using AnotherCounter; // Give Counter an alias called Ctr. using Ctr = Counter; // Declare a namespace for counters. namespace Counter { // A simple countdown counter. class CountDown { int val; public CountDown(int n) { val = n; } // ... } } // Another counter namespace. namespace AnotherCounter { // Declare another class called CountDown, which // is in the AnotherCounter namespace. class CountDown { int val;
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9. Measuring and Using Numbers Write a balanced chemical equation for the reaction
Time (min) 32 36 40 44 48 52 56 60
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