Antennas with Non-Foster Matching Networks phần 2
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Tham khảo tài liệu antennas with non-foster matching networks phần 2, kỹ thuật - công nghệ, kĩ thuật viễn thông phục vụ nhu cầu học tập, nghiên cứu và làm việc hiệu quả
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Antennas with Non-Foster Matching Networks phần 2P1: RVMMOBK060-01 MOBK060-Aberle.cls January 19, 2007 17:23 6 ANTENNAS WITH NON-FOSTER MATCHING NETWORKS FIGURE 2: Geometry of monopole antenna as modeled in Antenna Model software. The monopole is a copper cylinder 0.6 m in length and 0.010 meters in diameter, mounted on an infinite perfect ground plane total quality factor of the antenna/matching network combination is given by 1 Q tot = , (8) + 1 1 Qr Qm where Q m is the quality factor of the matching network. However, the loss in the matching network reduces the total efficiency of the system resulting in less total energy being coupled into free space.P1: RVMMOBK060-01 MOBK060-Aberle.cls January 19, 2007 17:23 ANTENNAS WITH NON-FOSTER MATCHING NETWORKS 7 FIGURE 3: Real part of input impedance of the ESA monopole obtained from simulation FIGURE 4: Imaginary part of input impedance of the ESA monopole obtained from simulationP1: RVMMOBK060-01 MOBK060-Aberle.cls January 19, 2007 17:23 8 ANTENNAS WITH NON-FOSTER MATCHING NETWORKS FIGURE 5: Radiation quality factor of the ESA monopole obtained from simulation FOSTER’S REACTANCE THEOREM AND NON-FOSTER CIRCUIT ELEMENTS Foster’s reactance theorem is a consequence of conservation of energy and states that for a lossless passive two-terminal device, the slope of its reactance (and susceptance) plotted versus frequency must be strictly positive, i.e., ∂X (ω) ∂B (ω) > 0 and > 0. (9) ∂ω ∂ω A device is called passive if it is not connected to a power supply other than the signal source. Such a two-terminal device (or one-port network) can be realized by ideal inductors, ideal capacitors, or a combination thereof. It turns out that a corollary that follows from Foster’s reactance theorem is even more important than the theorem itself. The corollary states that the poles and zeros of the reac- tance (and susceptance) function must alternate. By analytic continuity, we can generalize this corollary of Foster’s reactance theorem to state the following about immittance (impedance andP1: RVMMOBK060-01 MOBK060-Aberle.cls January 19, 2007 17:23 ANTENNAS WITH NON-FOSTER MATCHING NETWORKS 9 admittance) functions for a passive one-port network comprising lumped circuit elements: 1. The immittance function can be written as the ratio of two polynomial functions of the Laplace variable s = σ + j ω: N (s ) Z (s ) = . (10) D (s ) 2. The coefficients of the polynomials N (s ) and D(s ) are positive and real. 3. The difference in the orders of N (s ) and D(s ) is either zero or 1. As two examples of the above, consider the following: A) Capacitor. The impedance function is given by 1 Z (s ) = . (11) sC B) Series RLC. The impedance function is given by s 2 LC + sCR + 1 1 Z (s ) = R + sL + = . (12) sC sC If a two-terminal device has an immittance function that does not obey any of the three conse- ...
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Antennas with Non-Foster Matching Networks phần 2P1: RVMMOBK060-01 MOBK060-Aberle.cls January 19, 2007 17:23 6 ANTENNAS WITH NON-FOSTER MATCHING NETWORKS FIGURE 2: Geometry of monopole antenna as modeled in Antenna Model software. The monopole is a copper cylinder 0.6 m in length and 0.010 meters in diameter, mounted on an infinite perfect ground plane total quality factor of the antenna/matching network combination is given by 1 Q tot = , (8) + 1 1 Qr Qm where Q m is the quality factor of the matching network. However, the loss in the matching network reduces the total efficiency of the system resulting in less total energy being coupled into free space.P1: RVMMOBK060-01 MOBK060-Aberle.cls January 19, 2007 17:23 ANTENNAS WITH NON-FOSTER MATCHING NETWORKS 7 FIGURE 3: Real part of input impedance of the ESA monopole obtained from simulation FIGURE 4: Imaginary part of input impedance of the ESA monopole obtained from simulationP1: RVMMOBK060-01 MOBK060-Aberle.cls January 19, 2007 17:23 8 ANTENNAS WITH NON-FOSTER MATCHING NETWORKS FIGURE 5: Radiation quality factor of the ESA monopole obtained from simulation FOSTER’S REACTANCE THEOREM AND NON-FOSTER CIRCUIT ELEMENTS Foster’s reactance theorem is a consequence of conservation of energy and states that for a lossless passive two-terminal device, the slope of its reactance (and susceptance) plotted versus frequency must be strictly positive, i.e., ∂X (ω) ∂B (ω) > 0 and > 0. (9) ∂ω ∂ω A device is called passive if it is not connected to a power supply other than the signal source. Such a two-terminal device (or one-port network) can be realized by ideal inductors, ideal capacitors, or a combination thereof. It turns out that a corollary that follows from Foster’s reactance theorem is even more important than the theorem itself. The corollary states that the poles and zeros of the reac- tance (and susceptance) function must alternate. By analytic continuity, we can generalize this corollary of Foster’s reactance theorem to state the following about immittance (impedance andP1: RVMMOBK060-01 MOBK060-Aberle.cls January 19, 2007 17:23 ANTENNAS WITH NON-FOSTER MATCHING NETWORKS 9 admittance) functions for a passive one-port network comprising lumped circuit elements: 1. The immittance function can be written as the ratio of two polynomial functions of the Laplace variable s = σ + j ω: N (s ) Z (s ) = . (10) D (s ) 2. The coefficients of the polynomials N (s ) and D(s ) are positive and real. 3. The difference in the orders of N (s ) and D(s ) is either zero or 1. As two examples of the above, consider the following: A) Capacitor. The impedance function is given by 1 Z (s ) = . (11) sC B) Series RLC. The impedance function is given by s 2 LC + sCR + 1 1 Z (s ) = R + sL + = . (12) sC sC If a two-terminal device has an immittance function that does not obey any of the three conse- ...
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