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Follow these steps to make sure your hardware is working before you start using the BottleRocket software. 1. Connect the Firecracker hardware. The X10 Firecracker interface is a little dongle about the size of a Fig Newton. Plug it into a serial port on your computer (by default, BottleRocket will look for it in the COM1 port, represented by /dev/ttyS0 in Linux, but you can identify a different one later). Plug the transceiver into any electrical outlet. Figure 7-2 shows the Firecracker and transceiver ready to go.

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REFER sip:userb@there.com SIP/2.0 Via: SIP/2.0/TCP pc.there.com:5060;branch=z9hG4bK765d To: User B <sip:userb@there.com> From: User A <sip:usera@here.com> Call-ID: a5-32-43-12-77@4.3.2.1 CSeq: 2 REFER Refer-To: <sip:UserC@anywhere.com> Referred-By: <sip:usera@here.com> Content-Length: 0

One-Dimensional Horizontal Arrays . . . . . . . . . . . . . . . . . . . . . . 379 One-Dimensional Vertical Arrays . . . . . . . . . . . . . . . . . . . . . . . . 380 Two-Dimensional Arrays . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 380

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Another typical and rather simple system featuring the first and second type combiners is shown in Figure 7.40. Such an arrangement may be used, for example, to couple a TV carrier (Tx4) in addition to the message carriers (Tx1, 2, 3). If TV transmission is only occasional, the Tx4 chain can also be used as a common stand-by chain for the three other chains (by using a proper arrangement of supplementary switches). This provides an efficient and economical redundancy (3+1) scheme.

>>>(a,b,c)=func() >>>(a,b,c) ( fff , city ,8023)

(4.5)

N Choose the Insert Function command from the menu. N Click the Insert Function button, located next to the formula bar. In ver-

There s one more thing I d like to show you, Bob said, leading her to the IT team s cluster of cubicles between the data center and the business offices. It was cluttered with hundreds of blue cables stretched like arteries along the ceiling, and most of the cubicles contained half a dozen laptops or handhelds that were in varying degrees of disrepair. There, on the long wall above the cubicles, was a picture of a baseball in a wind tunnel (see Exhibit 12.3). In 1959, renowned scientist Lyman Briggs, who served as director of the National Institute of Standards and Technology, used a wind tunnel previously created to study aviation aerodynamics to prove that a thrown ball can actually curve. At the time, the revelation that the ball s spin and not

in the up and down states, respectively, where u(t, T; st) > d (t, T; st) for all t < T 1 and st. The same symbols u and d are used for both the states and returns on the bond to visually link the state with changes in the underlying bond price process.13 We can characterize the evolution of the one-factor zero-coupon bond price process as u (t , T ; st )P (t , T ; st ) P (t + 1, T ; st +1 ) = d (t , T ; st )P (t , T ; st ) if st +1 = st u with q(t ; st ) > 0 if st +1 = st d with q(t ; st ) > 0 (12.40)

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