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Distributed components such as inductors, transformers, and capacitors can be formed from microstrip transmission line sections on PCBs at microwave frequencies. A series or shunt inductor can be formed from a thin trace (Fig. 1.35), a shunt capacitor can be formed by a wide trace (Fig. 1.36), and a transformer can be formed by varying the width of the microstrip (Fig. 1.37).
Since for small angles, the relationship between x and xf is x xf = . l1 l2 Using this expression for x above gives l Keq = K 1 . l2 When l1 > l2, the spring appears stiffer than its physical stiffness, while for l1 < l2, the equivalent stiffness is less than the physical stiffness of the spring because of the mechanical advantage. 11.4.5 Massive Springs Up to this point, the springs considered have been ideal springs and have had no mass associated with them. In practice, it is often acceptable to model real springs as ideal springs if the mass of other elements in the system dominates the mass of the springs. This is not always the case, however, and real springs may need to be modeled as a combination of an ideal spring and a lumped mass. The equivalent mass of a massive spring (Fig. 11.17) can be derived by applying the concepts used in the previous section. Since the spring is a continuum, the kinetic energy is given by KE = 1 v 2 ( x )dm. 2 spring (11.55)
// Print a string backwards using recursion. #include <iostream> using namespace std; void reverse(char *s); int main() { char str[] = "this is a test"; reverse(str); return 0; }
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Copyright Glencoe/McGraw-Hill, a division of the McGraw-Hill Companies, Inc.
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Part III:
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To refer to integer 3,7 in nums of var of structure stype, you would write