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primary(config)# changeto context ct1 primary/ct1(config)# interface e0/0.1 primary/ct1(config-if)# nameif outside primary/ct1(config-if)# security-level 0 primary/ct1(config-if)# ip address 192.168.11.1 255.255.255.0 standby 192.168.11.2 primary/ct1(config-if)# no shutdown primary/ct1(config-if)# exit primary/ct1(config)# interface e0/1.1 primary/ct1(config-if)# nameif inside primary/ct1(config-if)# security-level 100 primary/ct1(config-if)# ip address 10.0.1.111 255.255.255.0 standby 10.0.1.112 primary/ct1(config-if)# no shutdown primary/ct1(config-if)# exit primary/ct1(config)# changeto context ct2 primary/ct2(config)# interface e0/0.2 primary/ct2(config-if)# nameif outside primary/ct2(config-if)# security-level 0 primary/ct2(config-if)# ip address 192.168.12.2 255.255.255.0 standby 192.168.12.1 primary/ct2(config-if)# no shutdown primary/ct2(config-if)# exit primary/ct2(config)# interface e0/1.2 primary/ct2(config-if)# nameif inside primary/ct2(config-if)# security-level 100 primary/ct2(config-if)# ip address 10.0.2.112 255.255.255.0 standby 10.0.2.111 primary/ct2(config-if)# no shutdown primary/ct2(config-if)# exit
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where ra = rs + rk = the ramp height, in. (This is the initial de ection of the follower linkage to eliminate [1] preload, and [2] clearance, so that motion of the follower end is impending.) rs = L + S1 = initial static deflection of linkage, in. kf k f + ks kf
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Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.
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Democritus (460 370 BC) proposes an atomic theory wherein all matter is made up of indivisible particles, or atoms. Charles de Coulomb (1736 1806) discovers that the force of attraction between electric charges is proportional to the product of the two charges and inversely proportional to the distance between them. Luigi Galvani (1737 1798) discovers that two unlike metals immersed in blood cause the muscles of a frog s legs to twitch. Alessandro Volta (1745 1827) discovers that a current ows between two connected unlike metals in a salt solution and, thus, invents the battery. John Dalton (1766 1844) proposes the rst table of atomic weights of elements. Andr Ampere (1775 1836) develops the theory of magnetic lines of force and quanti es electric current for the rst time. Hans Oersted (1777 1851) discovers a connection between electric current and magnetism and a way to measure electric current by the de ection of a magnet. Georg Ohm (1787 1854) discovers the relationship (Ohm s Law) between voltage, current, and resistance in a circuit. Michael Faraday (1791 1867) analyzes the chemical reactions in batteries and de nes the terms electrode, anode, cathode, and electrolyte. James Clerk Maxwell (1831 1879) develops the mathematical equations relating electricity and magnetism. Joseph Thomson (1856 1940) proves that electricity consists of electrons.
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Discussion:
YOU TRY IT Calculate the volume enclosed when the curve y = x1/3 , 32
Security in XI is much more granular than in earlier versions of BusinessObjects and leverages the Crystal Enterprise security model. This is discussed in 13. As part of the import process, importing users and groups is fairly straightforward. However, importing the associated permissions to documents and universes requires a greater understanding of the new options in XI Release 2. If you have poorly defined security in your version 5 or 6, you do not want to import it; instead, you will find it faster to redefine permissions at the group and folder levels.
Reliability
The velocity 0.493 0.262p 1 - cos 0.698 = 0.437 in 0.698 y = w y = 75.398( 0.437) = 32.93 in sec y = The acceleration y = 0.493p 0.262p = 2.938 in rad 2 sin 0.698 ( 0.698)2
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The freezing point depression constant, Kf , is given by Tf K f m where Tf change in freezing point in C, K f is the freezing point depression constant in C kg/mol, and m is the molal concentration in mol/kg.
such a function F an antiderivative of f . In fact we often want to nd the most general function F , or a family of functions, whose derivative equals f . We can sometimes achieve this goal by a process of organized guessing. Suppose that f (x) = cos x. If we want to guess an antiderivative, then we are certainly not going to try a polynomial. For if we differentiate a polynomial then we get another polynomial. So that will not do the job. For similar reasons we are not going to guess a logarithm or an exponential. In fact the way that we get a trigonometric function through differentiation is by differentiating another trigonometric function. What trigonometric function, when differentiated, gives cos x There are only six functions to try, and a moment s thought reveals that F (x) = sin x does the trick. In fact an even better answer is F (x) = sin x + C. The constant differentiates to 0, so F (x) = f (x) = cos x. We have seen in our study of falling bodies that the additive constant gives us a certain amount of exibility in solving problems. Now suppose that f (x) = x 2 . We have already noted that the way to get a polynomial through differentiation is to differentiate another polynomial. Since differentiation reduces the degree of the polynomial by 1, it is natural to guess that the F we seek is a polynomial of degree 3. What about F (x) = x 3 We calculate that F (x) = 3x 2 . That does not quite work. We seek x 2 for our derivative, but we got 3x 2 . This result suggests adjusting our guess. We instead try F (x) = x 3 /3. Then, indeed, F (x) = 3x 2 /3 = x 2 , as desired. We will write F (x) = x 3 /3 + C for our antiderivative. More generally, suppose that f (x) = ax 3 + bx 2 + cx + d. Using the reasoning in the last paragraph, we may nd fairly easily that F (x) = ax 4 /4 + bx 3 /3 + cx 2 /2 + dx + e. Notice that, once again, we have thrown in an additive constant. You Try It: Find a family of antiderivatives for the function f (x) = sin 2x x 4 + ex .
There is always an attractive force, in an atom, between the negatively charged electron cloud and the positively charged nucleus. In the case of a covalent bond, two atoms come close enough together (under the right conditions) for
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